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tomorrow-night.css diff --git a/404.html b/404.html new file mode 100644 index 0000000..04eb3a6 --- /dev/null +++ b/404.html @@ -0,0 +1,169 @@ + + + + + + Page not found - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
+ +
+ + + + + + + +
+
+

Document not found (404)

+

This URL is invalid, sorry. Please use the navigation bar or search to continue.

+ +
+ + +
+
+ + + +
+ + + + + + + + + + + + diff --git a/Acknowledgements.html b/Acknowledgements.html new file mode 100644 index 0000000..da35491 --- /dev/null +++ b/Acknowledgements.html @@ -0,0 +1,180 @@ + + + + + + Acknowledgements - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
+ +
+ + + + + + + +
+
+

Acknowledgements

+
    +
  • Qijing Zheng: The WAVECAR related function are written with the help of this code.
  • +
  • pymatgen and ASE: Some test files are copied from these two repositories.
  • +
  • RustFFT and ndrustfft: +These two crates make wav3d and wav1d become possible.
  • +
  • plotly.rs: This crate makes the visualization possible.
  • +
+ +
+ + +
+
+ + + +
+ + + + + + + + + + + + diff --git a/Band-example-SiDFT.html b/Band-example-SiDFT.html new file mode 100644 index 0000000..c38984c --- /dev/null +++ b/Band-example-SiDFT.html @@ -0,0 +1,106 @@ +
+ diff --git a/Band-example-SiDFT0.html b/Band-example-SiDFT0.html new file mode 100644 index 0000000..4211d68 --- /dev/null +++ b/Band-example-SiDFT0.html @@ -0,0 +1,61 @@ +
+ diff --git a/Band-example-SiDFT1.html b/Band-example-SiDFT1.html new file mode 100644 index 0000000..c382cef --- /dev/null +++ b/Band-example-SiDFT1.html @@ -0,0 +1,106 @@ +
+ diff --git a/Band-example-ncl.html b/Band-example-ncl.html new file mode 100644 index 0000000..487799a --- /dev/null +++ b/Band-example-ncl.html @@ -0,0 +1,334 @@ +
+ diff --git a/Band-example-ncl.toml b/Band-example-ncl.toml new file mode 100644 index 0000000..c158cb4 --- /dev/null +++ b/Band-example-ncl.toml @@ -0,0 +1,8 @@ +kpoint-labels = ["M", "Γ", "K", "M"] +procar = "PROCAR" +outcar = "OUTCAR" +txtout-prefix = "band_ncl_raw" +htmlout = "band_ncl.html" +segment-ranges = [[81, 120], [1, 40], [41, 80]] +ncl-spinor = "Z" +colormap = "jet" diff --git a/Band-example-pband.toml b/Band-example-pband.toml new file mode 100644 index 0000000..2f0d073 --- /dev/null +++ b/Band-example-pband.toml @@ -0,0 +1,10 @@ +kpoint-labels = ["L", "Γ", "X", "U|K", "Γ"] +procar = "PROCAR" +outcar = "OUTCAR" +txtout-prefix = "pband_raw" +htmlout = "pband.html" +segment-ranges = [[1, 10], [11, 20], [21, 30], [31, 40]] + +[pband.Si-p-orbit] +orbits = "px py pz" +color = "red" diff --git a/Band.html b/Band.html new file mode 100644 index 0000000..7c49166 --- /dev/null +++ b/Band.html @@ -0,0 +1,947 @@ + + + + + + Band Structure - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
+ +
+ + + + + + + +
+
+

Band Structure

+

rsgrad band can plot the band structure from PROCAR and OUTCAR.

+
+ +

Help Message

+
$ rsgrad band -h
+rsgrad-band
+Plot bandstructure and projected bandstructure
+
+USAGE:
+    rsgrad band [OPTIONS]
+
+OPTIONS:
+    -c, --config <CONFIG>
+            Band structure plot configuration file path
+
+        --colormap <COLORMAP>
+            [default: jet]
+
+        --efermi <EFERMI>
+            Set the E-fermi given from SCF's OUTCAR and it will be the reference energy level
+
+        --gen-template
+            Generate band structure plot configuration template
+
+    -h, --help
+            Print help information
+
+        --htmlout <HTMLOUT>
+            Save the band structure plot as HTML [default: band.html]
+
+    -k, --kpoint-labels <KPOINT_LABELS>
+            Symbols for high symmetry points on the kpoint path
+
+        --ncl-spinor <NCL_SPINOR>
+            [possible values: X, Y, Z]
+
+        --outcar <OUTCAR>
+            OUTCAR path [default: ./OUTCAR]
+
+        --procar <PROCAR>
+            PROCAR path [default: ./PROCAR]
+
+        --show
+            Open the browser and show the plot immediately
+
+        --to-inline-html
+            Render the plot and print the rendered code to stdout
+
+        --txtout-prefix <TXTOUT_PREFIX>
+            Save the raw data of band structure [default: band_raw]
+
+        --ylim <YLIM> <YLIM>
+            Set the y-range of the plot [default: "-1 6"]
+
+

Configuration Template

+
# rsgrad Band plot configuration in toml format.
+# multiple tokens inside string are seperated by whitespace, if you 
+
+# kpoint-labels   = ["G", "K", "M", "G"]   # should be consistant with the boundaries in KPOINTS
+procar          = "PROCAR"
+outcar          = "OUTCAR"
+txtout-prefix   = "band_raw"
+htmlout         = "band.html"
+# segment-ranges  = [[1, 40], [41, 80], [81, 120]]  # if commented, rsgrad will find the boundaries by judging if k[i] == k[i+1]
+# ncl-spinor      = "Z"     # for vasp_ncl calculation
+# colormap        = "jet"     # the colormap specified to plot ncl-band
+# efermi          = 0.0       # if commented, rsgrad will read the efermi from OUTCAR, but if may be slightly different from scf's
+# ylim            = [-1, 6]
+
+# [pband.plot1]
+# spins   = "up down"     # "u d" are also ok, for ncl system, "tot x y z" are available
+# atoms   = "1 3..7 -1"   # which atoms to project on, if commented, all atoms are selected
+# orbits  = "s px dxy"    # which orbits to project on, if commented, all orbits are selected
+# color   = "red"         # the color of marker
+
+

Example (without configuration file)

+

Simply run rsgrad band can plot the band structure.

+
$ rsgrad band
+[2022-07-14T18:40:18Z INFO  rsgrad::commands::band] Reading fermi level and lattice data from "./OUTCAR"
+[2022-07-14T18:40:18Z INFO  rsgrad::commands::band] Reading band data from "./PROCAR"
+[2022-07-14T18:40:18Z INFO  rsgrad::commands::band] Found Fermi level: 12.7626, shifting eigenvalues ...
+[2022-07-14T18:40:18Z WARN  rsgrad::commands::band] No k-point labels found, use empty labels instead
+[2022-07-14T18:40:18Z INFO  rsgrad::commands::band] Plotting raw bands ...
+[2022-07-14T18:40:18Z INFO  rsgrad::commands::band] Writing Bandstructure to "band.html"
+[2022-07-14T18:40:18Z INFO  rsgrad::commands::band] Writing raw band data to "band_raw.txt"
+[2022-07-14T18:40:18Z INFO  rsgrad] Time used: 79.644034ms
+
+

There may be a warning reminds you provide the labels of each high-symmetry point.
+rsgrad identifies high-symmetry points by calculate the difference of consecutive k-points. +If the difference equals zero, these two points are labelled as one high-symmetry point.

+

For example:

+
...
+k-point    38 :       0.0000    0.0256    0.0000
+k-point    39 :       0.0000    0.0128    0.0000
+k-point    40 :       0.0000    0.0000    0.0000
+k-point    41 :       0.0000    0.0000    0.0000
+k-point    42 :      -0.0085    0.0171    0.0000
+k-point    43 :      -0.0171    0.0342    0.0000
+...
+
+

k-point 40 and k-point 41 are same, thus be identified as one high-symmetry point. Each of the high-symmetry +points need a label. You may either left the --kpoint-labels empty or provide the correct labels seperated +by white spaces. Sometimes it may produce wrong band structure due to the special k-point path like

+
kpoints for bandstructure L-G-X-U K-G
+ 10
+line
+reciprocal
+  0.50000  0.50000  0.50000    1
+  0.00000  0.00000  0.00000    1
+
+  0.00000  0.00000  0.00000    1
+  0.00000  0.50000  0.50000    1
+
+  0.00000  0.50000  0.50000    1
+  0.25000  0.62500  0.62500    1
+
+  0.37500  0.7500   0.37500    1
+  0.00000  0.00000  0.00000    1
+
+

The end of third segment (0.25000, 0.62500, 0.62500) and the beginning of fourth segment (0.37500, 0.7500, 0.37500) +are not consistent, which produces wrong k-path, leading to wrong band structure:

+
+ +

To solve this issue, you need to try the configuration file.

+

Example (with configuration file)

+

With the configuration in the following

+
kpoint-labels   = ["L", "Γ", "X", "U|K", "Γ"]
+procar          = "PROCAR"
+outcar          = "OUTCAR"
+txtout-prefix   = "pband_raw"
+htmlout         = "pband.html"
+segment-ranges  = [[1, 10], [11, 20], [21, 30], [31, 40]]
+
+[pband.Si-p-orbit]
+orbits  = "px py pz"
+color   = "red"
+
+

and run rsgrad -c pband.toml

+
$ rsgrad band -c pband.toml
+[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Reading porjected band configuration fomr Some("pband.toml")
+[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Reading fermi level and lattice data from "OUTCAR"
+[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Reading band data from "PROCAR"
+[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Found Fermi level: 12.7626, shifting eigenvalues ...
+[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Plotting raw bands ...
+[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Plotting projected bands ...
+[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Writting projected band Si-p-orbit to "pband_raw_Si-p-orbit.txt" ...
+[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Projected band plot time usage: 1.220401ms
+[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Writing Bandstructure to "band.html"
+[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Writing raw band data to "pband_raw.txt"
+[2022-07-14T18:41:02Z INFO  rsgrad] Time used: 77.804627ms
+
+

then it produces

+
+ +

Example (for non-collinear system)

+

For the results produced by vasp_ncl, rsgrad supports plotting the \(z\) (\(x\) and \(y\) are also OK) projection to +analyze the spin angular moments.

+
kpoint-labels   = ["M", "Γ", "K", "M"]
+procar          = "PROCAR"
+outcar          = "OUTCAR"
+txtout-prefix   = "band_ncl_raw"
+htmlout         = "band_ncl.html"
+segment-ranges  = [[81, 120], [1, 40], [41, 80]]
+ncl-spinor      = "Z"
+colormap        = "jet"
+
+

then it produces

+
+ + +
+ + +
+
+ + + +
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+ +
+ +
+ + + + + + + +
+
+

Charge Density Difference

+

rsgrad chgdiff can calculate the charge density difference from CHGCAR files:

+

$$ +\Delta \rho = \rho_{A+B} - (\rho_A + \rho_B) +$$

+

Where \(\rho_{A+B}\), \(\rho_A\) and \(\rho_B\) are the charge densities of total structure, +A structure and B structure, respectively.

+

You may also need rsgrad poscar --split ... to generate +the structure of A and B from A+B.

+

Help message

+
$ rsgrad chgdiff --help
+rsgrad-chgdiff
+Calculate charge density difference.
+
+The operation is performed by `chgdiff = chgcar_ab - (chgcar_a + chgcar_b)`.
+
+USAGE:
+    rsgrad chgdiff [OPTIONS] <CHGCAR_AB> <CHGCAR_A> <CHGCAR_B>
+
+ARGS:
+    <CHGCAR_AB>
+            The CHGCAR of A+B system
+
+    <CHGCAR_A>
+            The CHGCAR of A system
+
+    <CHGCAR_B>
+            The CHGCAR of B system
+
+OPTIONS:
+    -h, --help
+            Print help information
+
+    -o, --output <OUTPUT>
+            The output charge density difference file path
+
+            [default: CHGDIFF.vasp]
+
+

Example

+

You need to calculate the electronic structure of the three structures (A+B, A and B) first, +then rsgrad chgdiff CHGCAR_A+B CHGCAR_A CHGCAR_B like

+
$ rsgrad chgdiff ../scf/CHGCAR Ag/CHGCAR noAg/CHGCAR
+[2022-07-14T18:34:59Z INFO  rsgrad::commands::chgdiff] Reading charge density from "Ag/CHGCAR"
+[2022-07-14T18:34:59Z INFO  rsgrad::commands::chgdiff] Reading charge density from "noAg/CHGCAR"
+[2022-07-14T18:34:59Z INFO  rsgrad::commands::chgdiff] Reading charge density from "../scf/CHGCAR"
+[2022-07-14T18:35:06Z INFO  rsgrad::commands::chgdiff] Calculating charge density difference by `CHGDIFF = "../scf/CHGCAR" - ("Ag/CHGCAR" + "noAg/CHGCAR")`
+[2022-07-14T18:35:06Z INFO  rsgrad::commands::chgdiff] Writing charge difference to "CHGDIFF.vasp"
+[2022-07-14T18:35:10Z INFO  rsgrad] Time used: 11.189259653s
+
+

finally use VESTA to visualize the data

+

+ +
+ + +
+
+ + + +
+ + + + + + + + + + + + diff --git a/DOS.html b/DOS.html new file mode 100644 index 0000000..87b8d95 --- /dev/null +++ b/DOS.html @@ -0,0 +1,399 @@ + + + + + + Density of States - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
+ +
+ + + + + + + +
+
+

Density of States

+

The rsgrad dos command calculates the Density of States (DOS) of current system.

+
+ +

rsgrad DOES NOT read the DOSCAR, but calculates the DOS from PROCAR instead by

+

$$ +D(E) = \frac{1}{V} \sum_{i=1}^{N} \delta(E-E(\mathbf{k}_i)) +$$

+

Because rsgrad uses arbitrary unit, the factor \(\frac{1}{V}\) is omitted. The \(\delta(x)\) +is replaced by Gaussian function or Lorentzian function:

+

$$ +g(x) = \frac{1}{\sigma\sqrt{2\pi}} \exp \left( -\frac{1}{2} \frac{(x-\mu)^2}{\sigma^2} \right) \\ +l(x) = \frac{1}{\pi} \frac{\sigma}{(x-\mu)^2 + \sigma^2} +$$

+

where \(\mu\) is \(E(\mathbf{k}_i)\) and \(\sigma\) is sigma of configuration in the implementation.

+

This method makes it easier to calculate projected DOS with projection of specific atoms, angular moments and k-points. +However, this method sometimes differs from DOSCAR with ISMEAR = -5. For detailed explaination, see the +document here.

+

The OUTCAR is also needed to get the Fermi level.

+

Help Message

+
$ rsgrad dos -h
+rsgrad-dos
+Calculate density of states from PROCAR and OUTCAR
+
+USAGE:
+    rsgrad dos [OPTIONS]
+
+OPTIONS:
+    -c, --config <CONFIG>       Projected DOS configuration file path
+        --gen-template          Generate projected DOS configuration template
+    -h, --help                  Print help information
+        --htmlout <HTMLOUT>     Save the projected DOS plot as HTML. Then you can view it in the
+                                browser [default: dos.html]
+        --outcar <OUTCAR>       OUTCAR path [default: ./OUTCAR]
+        --procar <PROCAR>       PROCAR path [default: ./PROCAR]
+        --show                  Open the browser and show the plot immediately
+        --show-brief            Print brief info of PROCAR, this may be helpful when you write the
+                                configuration
+        --to-inline-html        Render the plot and print the rendered code to stdout
+        --txtout <TXTOUT>       Save the raw data of projected DOS. Then you can replot it with more
+                                advanced tools [default: dos_raw.txt]
+        --xlim <XLIM> <XLIM>    Set the x-range of the plot [default: -1 6]
+
+

Configuration Template

+

The configuration template can be generated by running rsgrad dos --gen-template. The following configuration +is written to pband.toml by default:

+
# rsgrad DOS configuration in toml format.
+# multiple tokens inside string are seperated by whitespace
+method      = "Gaussian"        # smearing method
+sigma       = 0.05              # smearing width, (eV)
+procar      = "PROCAR"          # PROCAR path
+outcar      = "OUTCAR"          # OUTCAR path
+txtout      = "dos_raw.txt"     # save the raw data as "dos_raw.txt"
+htmlout     = "dos.html"        # save the pdos plot as "dos.html"
+totdos      = true              # plot the total dos
+fill        = true              # fill the plot to x axis or not
+xlim        = [-1, 6]           # x-range of plot
+
+[pdos.plot1]                  # One label produces one plot, the labels CANNOT be repetitive.
+                              # This label is 'plot1', to add more pdos, write '[pdos.plot2]' and so on.
+kpoints = "1 3..7 -1"         # selects 1 3 4 5 6 7 and the last kpoint for pdos plot.
+atoms   = "1 3..7 -1"         # selects 1 3 4 5 6 7 and the last atoms' projection for pdos plot.
+orbits  = "s px dxy"          # selects the s px and dx orbits' projection for pdos plot.
+factor  = 1.01                # the factor multiplied to this pdos
+
+[pdos.plot2]                  # One label produces one plot, the labels CANNOT be repetitive.
+                              # This label is 'plot2', to add more pdos, write '[pdos.plot2]' and so on.
+kpoints = "1 3..7 -1"         # selects 1 3 4 5 6 7 and the last kpoint for pdos plot.
+atoms   = "1 3..7 -1"         # selects 1 3 4 5 6 7 and the last atoms' projection for pdos plot.
+orbits  = "s px dxy"          # selects the s px and dx orbits' projection for pdos plot.
+factor  = 1.01                # the factor multiplied to this pdos
+
+# The fields can be left blank, if you want select all the components for some fields,
+# just comment them. You can comment fields with '#'
+
+ +

Example (without configuration file)

+

This command can calculate total DOS only. To calculate projected DOS, +use configuration instead (see next section).

+
$ rsgrad dos
+[2022-07-14T18:42:55Z INFO  rsgrad::commands::dos] Parsing PROCAR file "./PROCAR"
+[2022-07-14T18:42:55Z INFO  rsgrad::commands::dos] Parsing OUTCAR file "./OUTCAR" for Fermi level
+[2022-07-14T18:42:55Z INFO  rsgrad::commands::dos] Found Fermi level = -1.9018, eigenvalues will be shifted.
+[2022-07-14T18:42:55Z INFO  rsgrad::commands::dos] Plotting Total DOS ...
+[2022-07-14T18:42:55Z INFO  rsgrad::commands::dos] Total DOS plot time usage: 29.055µs
+[2022-07-14T18:42:55Z INFO  rsgrad::commands::dos] Writing DOS plot to "dos.html"
+[2022-07-14T18:42:55Z INFO  rsgrad::commands::dos] Writing raw DOS data to "dos_raw.txt"
+[2022-07-14T18:42:55Z INFO  rsgrad] Time used: 124.426652ms
+
+

The output html should be like something in the following

+
+ +

Example (with configuration file)

+

To plot multiple PDOS, using configuration file is suggested.

+

With the configuration (pdos.toml) in the following

+
method      = "Gaussian"
+sigma       = 0.05
+procar      = "PROCAR"
+outcar      = "OUTCAR"
+txtout      = "dos_raw.txt"
+htmlout     = "dos.html"
+totdos      = true
+fill        = true
+xlim        = [-1, 6]
+
+[pdos.Benzene]
+atoms   = "37..48"
+
+[pdos.AgSurf]
+atoms   = "3 6 10 14 21 23 25 33 36"
+
+

then rsgrad dos -c pdos.toml

+
$ rsgrad dos -c pdos.toml
+[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Reading PDOS configuration from Some("pdos.toml")
+[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Parsing PROCAR file "PROCAR"
+[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Parsing OUTCAR file "OUTCAR" for Fermi level
+[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Found Fermi level = -1.9018, eigenvalues will be shifted.
+[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Plotting Total DOS ...
+[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Total DOS plot time usage: 42.878µs
+[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Plotting PDOS ...
+[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] PDOS plot time usage: 6.223076ms
+[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Writing DOS plot to "dos.html"
+[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Writing raw DOS data to "dos_raw.txt"
+[2022-07-14T18:43:34Z INFO  rsgrad] Time used: 61.982958ms
+
+

you will get something in the following

+
+ +

Usage of txtout

+

rsgrad can write the raw data of plot by setting txtout (dos_raw.txt by default). The organization of it +shows the energy, total DOS and projected dos respectively:

+
# E-Ef TotDOS Benzene AgSurf
+...
+        -7.921938         0.002969         0.002158         0.000004
+        -7.899296         0.016032         0.011655         0.000019
+        -7.876654         0.070713         0.051408         0.000085
+        -7.854012         0.254749         0.185212         0.000307
+        -7.831371         0.749573         0.544998         0.000910
+        -7.808729         1.801235         1.309709         0.002202
+        -7.786087         3.534640         2.570233         0.004349
+        -7.763446         5.663677         4.118580         0.007011
+        -7.740804         7.409459         5.388357         0.009226
+        -7.718162         7.913407         5.755104         0.009908
+        -7.695520         6.898991         5.017578         0.008683
+        -7.672879         4.909619         3.570876         0.006208
+        -7.650237         2.854880         2.076535         0.003622
+        -7.627595         1.373037         0.998928         0.001724
+        -7.604953         0.617183         0.449840         0.000672
+        -7.582312         0.494734         0.362904         0.000231
+        -7.559670         0.977346         0.718873         0.000173
+        -7.537028         2.169137         1.593003         0.000599
+        -7.514387         4.077126         2.981347         0.002383
+        -7.491745         6.295459         4.560748         0.007858
+        -7.469103         8.005154         5.685401         0.021128
+...
+
+

The first line shows the labels of each series and have a hastag # in the beginning in order to let numpy.loadtxt +can read it directly.

+

Then you can throw it into other plotters like Excel, Matplotlib, OriginPro GnuPlot etc. and do whatever fancy things you prefer.

+ +
+ + +
+
+ + + +
+ + + + + + + + + + + + diff --git a/Feedback.html b/Feedback.html new file mode 100644 index 0000000..7a2d132 --- /dev/null +++ b/Feedback.html @@ -0,0 +1,198 @@ + + + + + + Feedback - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
+ +
+ + + + + + + +
+
+

Feedback

+

We are happy that you reach here. As an open-source project, rsgrad welcomes feedback.

+
    +
  • +

    If you have want to add features to rsgrad, just open an issue at +GitHub Issues. We also created a feature-requests list, +you can follow it at this page.

    +
  • +
  • +

    If rsgrad complains something or produces wrong result, just open an issue at +GitHub Issues. We are grateful if you can provide +the input files in order that we can reproduce the issue conveniently, +thus solve the issue as soon as possible.

    +
  • +
  • +

    If you are interested in rsgrad and want to contribute to the source code, just fork rsgrad and create pull requests at +Pull Requests. We are super grateful if you can contribute +to rsgrad.

    +
  • +
+ +
+ + +
+
+ + + +
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z-?ra7<4n?x&FYaE?cEGI)-)$tD$5+muBu}U?sPHFKe+hV5?aCTUXV`J=9AHC=o-*Q zXUuT@-0>M!)m+!o+T(oHaeB!5lJUF^EcXIqSUNsvI7$4;|X#{w!e5pUJ_ zak1J+C*mxrK*L>l)}}XDmB5!T;U_ev;jCB9B2`6t)Wa`7=7pam>YPepUHy>E1}-i| zx=cTq2|P}#Ey5pcy4D8*2oic4dykynV%zxoUkQ#ZS%}$Wd?mL`_nI;G*TmEF^KJp z_vh{DE5H7`9RZOzAku0+?DJ`Ocwh zS7jB5f%YHF1(sTSKSuTtezZh?ey859@nDV}*wx8We3^(^>c;D^k{15Qf0gLJdBw#% zK4AOfnWngIHTLC=dT)#w{3rZBSpE+*HU0+;Htp>`-fzW8*#W`aU5e&a;9&m+kS-Mo literal 0 HcmV?d00001 diff --git a/Gap.html b/Gap.html new file mode 100644 index 0000000..52f5a68 --- /dev/null +++ b/Gap.html @@ -0,0 +1,257 @@ + + + + + + Gap - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +

+ +
+ +
+ + + + + + + +
+
+

Gap

+

This command (rsgrad gap) calculates the band gap and prints positions of VBM and CBM.

+

There are two ways to run this command:

+
    +
  1. Use WAVECAR only. All required information can be extracted from WAVECAR.
  2. +
  3. Or use PROCAR and OUTCAR instead. PROCAR is read for the band energies, band occupations and k-point coordinates; +OUTCAR is read for the Fermi level only.
  4. +
+

Note: Usually it's faster to parse results from WAVECAR.

+

If your system is a non-SCF calculation for band structure, you may need to specify the correct Fermi level by +rsgrad gap -e <put the correct E-fermi here>, the correct Fermi level can be obtained from the OUTCAR of SCF calculation.

+

Help Message

+
$ rsgrad gap --help
+rsgrad-gap
+Find band gap and print positions of VBM and CBM
+
+USAGE:
+    rsgrad gap [OPTIONS]
+
+OPTIONS:
+    -e, --efermi <EFERMI>      Specify Fermi level, if left empty, this value would be read from
+                               WAVECAR or OUTCAR
+    -h, --help                 Print help information
+    -o, --outcar <OUTCAR>      OUTCAR file name, this file is parsed to get Fermi level only
+                               [default: OUTCAR]
+    -p, --procar <PROCAR>      PROCAR file name, OUTCAR is also needed to get Fermi level [default:
+                               PROCAR]
+    -w, --wavecar <WAVECAR>    WAVECAR file name, no more files needed [default: WAVECAR]
+
+

Example

+
    +
  1. For metal system:
  2. +
+
[2022-12-01T11:30:49Z INFO  rsgrad::commands::gap] Trying to parse "WAVECAR" ...
+----------------------------------------
+ Current system is         Metal
+----------------------------------------
+[2022-12-01T11:30:49Z INFO  rsgrad] Time used: 166.251241ms
+
+
    +
  1. For non-spin-polarized direct gap system:
  2. +
+
[2022-12-01T11:37:15Z INFO  rsgrad::commands::gap] Trying to parse "WAVECAR" ...
+--------------------------------------------------------------------------------
+ Current system has    Direct Gap    of   0.328    eV
+  CBM @ k-point     1 of ( 0.000, 0.000, 0.000) , band   819 of    0.322 eV
+  VBM @ k-point     1 of ( 0.000, 0.000, 0.000) , band   818 of   -0.006 eV
+--------------------------------------------------------------------------------
+[2022-12-01T11:37:15Z INFO  rsgrad] Time used: 253.556682ms
+
+
    +
  1. For spin-polarized direct gap system:
  2. +
+
$ rsgrad gap
+[2022-12-01T11:38:16Z INFO  rsgrad::commands::gap] Trying to parse "WAVECAR" ...
+--------------------------------------------------------------------------------
+    ====================  Gap Info For     SPIN UP      ====================
+ Current system has    Direct Gap    of   0.976    eV
+  CBM @ k-point     1 of ( 0.000, 0.000, 0.000) , band   129 of    0.498 eV
+  VBM @ k-point     1 of ( 0.000, 0.000, 0.000) , band   128 of   -0.478 eV
+    ====================  Gap Info For    SPIN DOWN     ====================
+ Current system has    Direct Gap    of   0.980    eV
+  CBM @ k-point     1 of ( 0.000, 0.000, 0.000) , band   129 of    0.499 eV
+  VBM @ k-point     1 of ( 0.000, 0.000, 0.000) , band   128 of   -0.481 eV
+--------------------------------------------------------------------------------
+[2022-12-01T11:38:16Z INFO  rsgrad] Time used: 31.744371ms
+
+
    +
  1. For non-spin-polarized indirect gap system:
  2. +
+
$ rsgrad gap
+[2022-12-01T11:40:52Z INFO  rsgrad::commands::gap] Trying to parse "WAVECAR" ...
+--------------------------------------------------------------------------------
+ Current system has   Indirect Gap   of   1.160    eV
+  CBM @ k-point    25 of ( 0.000, 0.444, 0.444) , band     5 of    1.097 eV
+  VBM @ k-point    17 of ( 0.000, 0.000, 0.000) , band     4 of   -0.062 eV
+--------------------------------------------------------------------------------
+[2022-12-01T11:40:52Z INFO  rsgrad] Time used: 22.565948ms
+
+ +
+ + +
+
+ + + +
+ + + + + + + + + + + + diff --git a/Installation.html b/Installation.html new file mode 100644 index 0000000..1096060 --- /dev/null +++ b/Installation.html @@ -0,0 +1,221 @@ + + + + + + Installation - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
+ +
+ + + + + + + +
+
+

Installation

+

There are two ways to install rsgrad, downloading the pre-built binaries and building from scratch.

+

Download the Binary from GitHub Release

+

We provide the pre-built binaries at GitHub Release.

+

There are four platforms we support with pre-built binaries

+
    +
  • +

    rsgrad-<VERSION>-linux-x86_64-musl.tar.gz: Statically linked binary. Can run on almost all Linux distros. +However, the musl libc may have performance issues in some scenes like wave1d, wav3d etc.

    +
  • +
  • +

    rsgrad-<VERSION>-linux-x86_64.tar.gz: Dynamically linked against glibc and other fundamental +system libraries.
    +For the binaries with 0.3.6_ci-test or upper version, they can run on most Linux distros +(e.g. CentOS 7, Ubuntu 18.04).
    +If it still complains with message like /lib64/libc.so.6: version 'GLIBC_2.18' not found, just switch to -musl +binary or build from scratch.

    +
  • +
  • +

    rsgrad-<VERSION>-macos-x86_64.tar.gz: Binary for macOS (Intel). rsgrad is developed on macOS 13, which +means you are don't need to worry about the availability if you are using macOS.

    +
  • +
  • +

    rsgrad-<VERSION>-macos-aarch64.tar.gz: Binary for macOS (Apple Silicon).

    +
  • +
  • +

    rsgrad-<VERSION>-windows-x86_64.zip: Binary for Windows system. We have no plan to support 32-bit systems.

    +
  • +
+

Download the corresponding binary and put it in $PATH (or %PATH% on Windows), and have fun!

+

Build from Scratch

+

The build requires Internet accessibility.

+
    +
  • +

    If you haven't installed Rust toolchain, run curl --proto '=https' --tlsv1.2 -sSf https://sh.rustup.rs | sh +and follow the instructions to configure it. When you finished the toolchain installation, you should be able to +run cargo in command-line. Detailed instructions can be found here.

    +
  • +
  • +

    If you have installed Rust toolchain already, just run cargo install --git https://github.com/Ionizing/rsgrad. +Several minutes later, the rsgrad should be installed to ~/.cargo/bin, no need to modify the $PATH (or %PATH% on Windows).

    +
  • +
+ +
+ + +
+
+ + + +
+ + + + + + + + + + + + diff --git a/Introduction.html b/Introduction.html new file mode 100644 index 0000000..ddf7be4 --- /dev/null +++ b/Introduction.html @@ -0,0 +1,195 @@ + + + + + + Introduction - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
+ +
+ + + + + + + +
+
+

Introduction

+

rsgrad is an open-source command-line tool to help VASP players play better with VASP.
+rsgrad is written proudly in pure Rust.

+

Now rsgrad provides several features:

+
    +
  1. Track the relaxation and MD (molecular dynamics) progress;
  2. +
  3. Calculate and visualize the DOS (density of states) and pDOS (projected DOS);
  4. +
  5. Plot and visualize the band structure and fat band structure;
  6. +
  7. Save the frames with given MD or relaxation trajectory;
  8. +
  9. Calculate charge density difference;
  10. +
  11. Analyze the vibration eigen values and eigen vectors;
  12. +
  13. Plot the wave function at given bands in real-space;
  14. +
  15. Plot the wave function at given bands in real-space then integrate it over specified plane;
  16. +
  17. Plot and visualize the work function;
  18. +
  19. Split POSCAR;
    +Convert between fractional coordinates and Cartesian coordinates;
    +Format POSCAR;
  20. +
  21. Generate POTCAR according to POSCAR;
  22. +
  23. Calculate Transition Dipole Moment from WAVECAR;
  24. +
  25. Calculate band gap and print locations of CBM and VBM.
  26. +
  27. Convert one quantity to other units that representing same energy.
  28. +
+

Wish you have a good time with rsgrad ^_^

+ +
+ + +
+
+ + + +
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z0o*tjD1drx$@1p-L+DQ*_p~+G#FTl1&K_f6xr}U@%%#@JWRA-7{y5;Z^I^dJ=VvJ1 z5y=obhGkz2AV7gh7g;nEGLd1r8seHb66gbbySr8WStY}OsJwD zqks3}qazoU!cp4ei#;h@@ej=Om#JYx&u_=gW8X|*0am{GGJ4)WVIG^g$sGMttu z7amr;bh4d&@w2WMq*)g5QRcYic7Og#{t1S( zD4y?W@`_jQn*5LbQ59296eclU`E&;D2IckM7PqSmzWAtqLR0h2zs>g#WxPb)wn@M6 z?<@Z2i%2qx8q#gOnp$}M-=qG=LUe%D=yW9i?Ync7YH4;Fp=yZ;~Bf7 + + + + + POSCAR - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
+ +
+ + + + + + + +
+
+

POSCAR

+

There are several operations that rsgrad pos can do

+
    +
  • Convert the fractional coordinates to Cartesian coordinates or convert reversely;
  • +
  • Split the POSCAR and save the two parts;
    +This command is useful when you want to calculate charge density difference and adsorption energy.
  • +
  • Format the POSCAR and add element symbol tags to each atom.
  • +
+

Help Message

+
$ rsgrad pos --help
+rsgrad-pos 
+Operation(s) about POSCAR, including split it into two POSCARs
+
+USAGE:
+    rsgrad pos [OPTIONS] [--] [POSCAR]
+
+ARGS:
+    <POSCAR>
+            Specify the input POSCAR file
+            
+            [default: ./POSCAR]
+
+OPTIONS:
+    -a, --a-name <A_NAME>
+            Splitted POSCAR path with selected atoms
+            
+            [default: POSCAR_A]
+
+    -b, --b-name <B_NAME>
+            Splitted POSCAR path with complement of `a_name`
+            
+            [default: POSCAR_B]
+
+    -c, --cartesian
+            Cartesian coordinates is used in writting POSCAR
+
+        --convert
+            Convert POSCAR to cartesian coordinates or fractional coordinates
+
+        --converted <CONVERTED>
+            The target path of converted POSCAR
+            
+            [default: POSCAR_new]
+
+    -h, --help
+            Print help information
+
+    -i, --select-indices <SELECT_INDICES>...
+            Selects the indices to operate.
+            
+            Step indices start from '1', if '0' is given, all the structures will be selected. Step
+            indices can be negative, where negative index means counting reversely. E.g. "-i -2 -1 1
+            2 3" means selecting the last two and the first three atom.
+
+        --no-add-symbols-tags
+            The symbols of each atom will not be written as comment in POSCAR
+
+        --no-preserve-constraints
+            Atom constraints will be dropped when writting POSCAR
+
+    -s, --split
+            Split POSCAR according to selected_indices
+
+

Examples

+
    +
  • Format the POSCAR to add element symbol tags
  • +
+

The original POSCAR of CO2:

+
 C  O 
+ 1.0000000000000000
+    20.0000000000000000    0.0000000000000000    0.0000000000000000
+     0.0000000000000000   20.0000000000000000    0.0000000000000000
+     0.0000000000000000    0.0000000000000000   20.0000000000000000
+ C   O  
+   1   2
+Direct
+  0.5000000000000000  0.5000000000000000 -0.5000000000000000
+  0.5754584707965210  0.4974961803083730  0.5000000000000000
+  0.4249089651951450  0.5078477015701101  0.5000000000000000
+
+

Then run rsgrad pos POSCAR --convert

+
$ rsgrad pos POSCAR --convert
+[2022-07-14T15:38:47Z INFO  rsgrad::commands::pos] Reading POSCAR file "POSCAR" ...
+[2022-07-14T15:38:47Z INFO  rsgrad::commands::pos] Converting it to "POSCAR_new"
+[2022-07-14T15:38:47Z INFO  rsgrad::commands::pos] Done
+[2022-07-14T15:38:47Z INFO  rsgrad] Time used: 1.96796ms
+
+

The formatted file should be POSCAR_new

+
C  O
+ 1.0000000
+      20.000000000       0.000000000       0.000000000
+       0.000000000      20.000000000       0.000000000
+       0.000000000       0.000000000      20.000000000
+      C      O
+      1      2
+Direct
+      0.5000000000      0.5000000000     -0.5000000000 !      C-001    1
+      0.5754584708      0.4974961803      0.5000000000 !      O-001    2
+      0.4249089652      0.5078477016      0.5000000000 !      O-002    3
+
+
    +
  • Convert POSCAR to Cartesian coordinates
  • +
+

Just run rsgrad pos POSCAR --convert --cartesian

+
$ rsgrad pos POSCAR --convert --cartesian
+[2022-07-14T15:40:33Z INFO  rsgrad::commands::pos] Reading POSCAR file "POSCAR" ...
+[2022-07-14T15:40:33Z INFO  rsgrad::commands::pos] Converting it to "POSCAR_new"
+[2022-07-14T15:40:33Z INFO  rsgrad::commands::pos] Done
+[2022-07-14T15:40:33Z INFO  rsgrad] Time used: 1.57861ms
+
+

The converted file POSCAR_new should be like

+
C  O
+ 1.0000000
+      20.000000000       0.000000000       0.000000000
+       0.000000000      20.000000000       0.000000000
+       0.000000000       0.000000000      20.000000000
+      C      O
+      1      2
+Cartesian
+     10.0000000000     10.0000000000    -10.0000000000 !      C-001    1
+     11.5091694159      9.9499236062     10.0000000000 !      O-001    2
+      8.4981793039     10.1569540314     10.0000000000 !      O-002    3
+
+
    +
  • Split the POSCAR
  • +
+

Let take the CO2 structure as the example again. Here we will take the +C atom out to see what the operation does.

+

The C atom index is 1, so we should run rsgrad pos POSCAR -s -i 1

+
$ rsgrad pos POSCAR -s -i 1
+[2022-07-14T15:49:32Z INFO  rsgrad::commands::pos] Reading POSCAR file "POSCAR" ...
+[2022-07-14T15:49:32Z INFO  rsgrad::commands::pos] Splitting it to "POSCAR_A" and "POSCAR_B" ...
+[2022-07-14T15:49:32Z INFO  rsgrad::commands::pos] "POSCAR_A" contains
+[2022-07-14T15:49:32Z INFO  rsgrad::commands::pos]       C     1
+[2022-07-14T15:49:32Z INFO  rsgrad::commands::pos] "POSCAR_B" contains
+[2022-07-14T15:49:32Z INFO  rsgrad::commands::pos]       O     2
+[2022-07-14T15:49:32Z INFO  rsgrad::commands::pos] "POSCAR_A" written
+[2022-07-14T15:49:32Z INFO  rsgrad::commands::pos] "POSCAR_B" written
+[2022-07-14T15:49:32Z INFO  rsgrad] Time used: 2.11275ms
+
+

The separated files should be like

+
$ bat POSCAR_A POSCAR_B
+───────┬──────────────────────────────────────────────────────────────────────────
+       │ File: POSCAR_A
+───────┼──────────────────────────────────────────────────────────────────────────
+   1   │ Generated by rsgrad, POSCAR with selected atoms
+   2   │  1.0000000
+   3   │       20.000000000       0.000000000       0.000000000
+   4   │        0.000000000      20.000000000       0.000000000
+   5   │        0.000000000       0.000000000      20.000000000
+   6   │       C
+   7   │       1
+   8   │ Direct
+   9   │       0.5000000000      0.5000000000     -0.5000000000 !      C-001    1
+───────┴──────────────────────────────────────────────────────────────────────────
+───────┬──────────────────────────────────────────────────────────────────────────
+       │ File: POSCAR_B
+───────┼──────────────────────────────────────────────────────────────────────────
+   1   │ Generated by rsgrad, POSCAR complement
+   2   │  1.0000000
+   3   │       20.000000000       0.000000000       0.000000000
+   4   │        0.000000000      20.000000000       0.000000000
+   5   │        0.000000000       0.000000000      20.000000000
+   6   │       O
+   7   │       2
+   8   │ Direct
+   9   │       0.5754584708      0.4974961803      0.5000000000 !      O-001    1
+  10   │       0.4249089652      0.5078477016      0.5000000000 !      O-002    2
+───────┴──────────────────────────────────────────────────────────────────────────
+
+

The process schema:

+

+ +
+ + +
+
+ + + +
+ + + + + + + + + + + + diff --git a/PseudoPotential.html b/PseudoPotential.html new file mode 100644 index 0000000..e754b64 --- /dev/null +++ b/PseudoPotential.html @@ -0,0 +1,278 @@ + + + + + + POTCAR - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
+ +
+ + + + + + + +
+
+

Pseudo Potential

+

This command generates POTCAR according to POSCAR. The usage is simple: rsgrad pot in the directory with POSCAR presents.

+

To use this command, a configuration file is required like:

+
[functional-path]
+PAW_PBE = "<path of PAW_PBE>"
+PAW_LDA = "<path of PAW_LDA>"
+
+

and you need to put it at ~/.rsgrad for Linux/macOS, +and C:\Users\<YourUserName>\.rsgrad.toml for Windows.

+

Note: rsgrad pot will give some hint if you have no idea on how to write the file.

+

Then you can specify the element type in POSCAR, for example:

+
Cd2 S2 HSE optimized
+   1.00000000000000
+     4.1704589747753724    0.0000000049514629    0.0000000000000000
+    -2.0852299788115007    3.6117232476351271   -0.0000000000000000
+     0.0000000000000000   -0.0000000000000000    6.7822968954189937
+   Cd   S
+     2     2
+Direct
+  0.6666669999999968  0.3333330000000032  0.5001535716160643
+  0.3333330000000032  0.6666669999999968  0.0001535716160644
+  0.6666669999999968  0.3333330000000032  0.8768464283839381
+  0.3333330000000032  0.6666669999999968  0.3768464283839381
+
+

Finally rsgrad-pot will read the line " Cd S ", and find the corresponding POTCAR and merge them.

+

In some cases, several elements does not have "standard" POTCAR that without suffix. E.g. the K/POTCAR +is not available for PBE functional. We provide two solutions for it:

+
    +
  • Write K_sv or other available K-related functionals in POSCAR +
    Cd2 S2 HSE optimized
    +   1.00000000000000
    +     4.1704589747753724    0.0000000049514629    0.0000000000000000
    +    -2.0852299788115007    3.6117232476351271   -0.0000000000000000
    +     0.0000000000000000   -0.0000000000000000    6.7822968954189937
    +   Cd   K_sv
    +     2     2
    +Direct
    +  0.6666669999999968  0.3333330000000032  0.5001535716160643
    +  ...
    +
    +
  • +
  • Use aliases field in .rsgrad.toml +
    [functional-path]
    +...
    +aliases = { K = "K_sv" }
    +
    +or +
    [functional-path]
    +...
    +[functional-path.aliases]
    +K = "K_sv"
    +
    +
  • +
+

Help Message

+
rsgrad-pot
+Generate the POTCAR according to POSCAR
+
+USAGE:
+    rsgrad pot [OPTIONS] [FUNCTIONAL]
+
+ARGS:
+    <FUNCTIONAL>
+            Specify the functional type, now only "PAW_PBE"(or "paw_pbe") and "PAW_LDA"(or
+            "paw_lda") are available
+
+            [default: PAW_PBE]
+
+OPTIONS:
+    -c, --config <CONFIG>
+            Specify the configuration file, if left blank, rsgrad will read `.rsgrad.toml` at your
+            home dir
+
+    -h, --help
+            Print help information
+
+    -p, --poscar <POSCAR>
+            Specify the POSCAR file
+
+            Note: the elements symbols' line should involve the specified valence configuration if
+            you need. For example, if you need a `K_sv` POTCAR for `K`, just write `K_sv` in the
+            POSCAR
+
+            [default: ./POSCAR]
+
+    -s, --save-in <SAVE_IN>
+            Specify where the `POTCAR` would be written
+
+            [default: ./]
+
+

Example

+
$ rsgrad pot
+[2023-10-20T16:19:48Z INFO  rsgrad::settings] Reading rsgrad settings from "/Users/ionizing/.rsgrad.toml" ...
+[2023-10-20T16:19:48Z INFO  rsgrad::settings] Checking rsgrad setting availability ...
+[2023-10-20T16:19:48Z INFO  rsgrad::commands::pot] Reading POSCAR file "../tests/POSCAR.CdS_HSE" ...
+[2023-10-20T16:19:48Z INFO  rsgrad::vasp_parsers::potcar] Reading POTCAR from "/Users/ionizing/apps/vasp/pp/potpaw_PBE.54/Cd/POTCAR"
+[2023-10-20T16:19:48Z INFO  rsgrad::vasp_parsers::potcar] Reading POTCAR from "/Users/ionizing/apps/vasp/pp/potpaw_PBE.54/S/POTCAR"
+[2023-10-20T16:19:48Z INFO  rsgrad::commands::pot] Writing POTCAR to "./POTCAR" ...
+[2023-10-20T16:19:48Z INFO  rsgrad] Time used: 5.524643ms
+
+ +
+ + +
+
+ + + +
+ + + + + + + + + + + + diff --git a/Relaxation.html b/Relaxation.html new file mode 100644 index 0000000..f5e19ef --- /dev/null +++ b/Relaxation.html @@ -0,0 +1,222 @@ + + + + + + Relaxation - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
+ +
+ + + + + + + +
+
+

Relaxation

+

To track the relaxation or MD process, use rsgrad rlx. This command is useful if you want to know the progress +of geometry optimization (aka relaxation) or molecular dynamics.

+

This commands extract the following tags from OUTCAR:

+
    +
  • TOTEN
  • +
  • TOTEN without entropy
  • +
  • TOTEN difference between two ionic steps
  • +
  • Maximum of atom forces (The negative EDIFFG is the threshold of this tag)
  • +
  • The index of the atom with the maximum of force
  • +
  • Number of SCF steps of each ionic step
  • +
  • Time usage of each ionic step
  • +
  • Volume of the cell
  • +
  • Total magnetic moment
  • +
+

Help Message

+
$ rsgrad rlx -h
+rsgrad-rlx
+Tracking relaxation or MD progress
+
+USAGE:
+    rsgrad rlx [OPTIONS] [OUTCAR]
+
+ARGS:
+    <OUTCAR>    Specify the input OUTCAR file [default: ./OUTCAR]
+
+OPTIONS:
+    -a, --favg               Prints averaged total force in eV/A
+    -e, --toten              Prints TOTEN in eV
+    -h, --help               Print help information
+    -i, --fmidx              Prints the index of ion with maximum total force load. Starts from 1
+        --no-fmax            Don't print maximum total force in A^3
+        --no-lgde            Don't print Log10(delta(TOTEN without entropy))
+        --no-magmom          Don't print total magnetic moment in muB
+        --no-nscf            Don't print number of SCF iteration for each ionic step
+        --no-time            Don't print time elapsed for each ionic step in minutes
+        --no-totenz          Don't print TOTEN without entropy in eV
+    -p, --poscar <POSCAR>    Specify the input POSCAR file [default: ./POSCAR]
+    -v, --volume             Prints lattice volume in A^3
+    -x, --fmaxis             Prints the axis where the strongest total force component lies on.
+                             [XYZ]
+
+

Example

+

+ +
+ + +
+
+ + + +
+ + + + + + + + + + + + diff --git a/Trajectory-example-xsf1.png b/Trajectory-example-xsf1.png new file mode 100644 index 0000000000000000000000000000000000000000..bdc062d16c510b2dcbfbdfc7f58a838491c321fe GIT binary patch literal 123587 zcmeGEbz2+X7d{GyU?Dig-3jg#cL}aVi#x@wSaB~}XrWkx6)W!UT3m~JDO%j+q@VBe zJJ)kw!1?cRUBk@IOm;GR@3roG-D^!^G}II@!K7dS0D!3omDK_Okm>*cAO;8sf5p<( zVjchhuiMMWXei3aP;0om*w{N-0|3yN&uOSSDZ_-pdoM4Zct9kaBs@O_VT6Kk$`((Y z&q+vlO3`QtQjSAg;0iD;t-h}78`2cR%0@%G%js9!M&3%%g47{EjF|UAwrY0~jJK&dKRjlzU2I@~9$oN0v@S z*YMsuU3{A=qR}ukI-0R#o~o+hj|;%B6An&(WcpSTboPzyV#20q#7DT2ndTNmpNHYS z_F|Cn!v2+H`m0#nq}1<^h_sCFV(0%l`{^ddMGWVf^RjKIEqwTNHy!+k4fA(d+e;Q=)D4N^3aMTf4v%<>|G@{o9@AS6<@{qgj#K6QW9@`H} zTUOO>zTzFV0#iKxnhj}=oSO1Yqd94toHNSqwASxxr+S521>WlR@_C!xVuYD(VE>^8 z+y;X@8&K`87u&2CQ(}BRKx)Ip6C9sR~2tuh8szpOX9|4Bd zYcT6zy^-;U`Teo|Bj`!m0=kmEfg#u-`5}IY#7)Ow?KP~z6~(scQV|3tgc5a^oN5VD zafH6^dE?3+0CEmd?@ilWc9nPpQpx~mql#%;q8WN5+mgBH5fr8RhLj4BN@N|9Kf 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zeSsHN$(^ufTJMqQc=hJN1IAOO_PfRNoTtBDx6O98X1UP}DVoo&9qU&3hx(+X#nYhmGMU2@*;d|p@jX+eYDuAk5B^KO3n zx6Jqb+SuQ}fOns?iT!#Nu5a^liSTmY*_Mpc)>wR6c0_#1x_{q)H09j;Qs@2JP3L=4 z#^X%U;|G@7JTy(L_sW_!7dZX1d+Af=8h79xyqQzAug~y#R{ehO_1C%SzBlHJ?g#aX zoj}V|6lYJ>J_>Ak9$>kmBV`u-FL(Rh<`bSO3+&%+`OI!tx=7yDB_@si=)u{Om+{8A zyoro_3fxO=E>ijJX1wjg7U4@FWo@F(`W?SyPa5oYKM<2*crD{w2% zk1YOe;IbA)r-2%10)ew^pC+=7pr-V`Tg_`BXVrkMftuOF3CxwrO>-eNIFd7f z4aInt3eE11SLJeeK}IgHZ=5WqFLvYiwws$bxBRHN-#_`~S=ZHJZ^Q3e7Jq87sNC;7 z`Dy#-ur)W + + + + + Trajectory - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
+ +
+ + + + + + + +
+
+

Trajectory

+

rsgrad reads OUTCAR then provide some operations in the following.

+
    +
  • Save selected steps as XDATCAR.
  • +
  • Save selected steps as POSCAR files.
  • +
  • Save selected steps as XSF files. With XSF, VESTA can show the force vectors on every atom.
  • +
+

Help Message

+
$ rsgrad traj --help
+rsgrad-traj
+Operations about relaxation/MD trajectory.
+
+POSCAR is needed if you want to preserve the constraints when saving frames to POSCAR.
+
+USAGE:
+    rsgrad traj [OPTIONS] [--] [OUTCAR]
+
+ARGS:
+    <OUTCAR>
+            Specify the input OUTCAR file
+
+            [default: ./OUTCAR]
+
+OPTIONS:
+        --cartesian
+            Save to POSCAR in cartesian coordinates, the coordinates written is direct/fractional by
+            default
+
+    -d, --save-as-xdatcar
+            Save whole trajectory in XDATCAR format
+
+    -h, --help
+            Print help information
+
+    -i, --select-indices <SELECT_INDICES>...
+            Selects the indices to operate.
+
+            Step indices start from '1', if '0' is given, all the structures will be selected. Step
+            indices can be negative, where negative index means counting reversely. E.g.
+            "-i -2 -1 1 2 3" means selecting the last two and first three steps.
+
+        --no-add-symbol-tags
+            Don't add chemical symbol to each line of coordinates
+
+        --no-preserve-constraints
+            Don't preverse constraints when saving trajectory to POSCAR
+
+    -p, --poscar <POSCAR>
+            Specify the input POSCAR file
+
+            [default: ./POSCAR]
+
+    -s, --save-as-poscar
+            Save selected steps as POSCARs
+
+        --save-in <SAVE_IN>
+            Define where the files would be saved
+
+            [default: .]
+
+    -x, --save-as-xsfs
+            Saves each selected modes to XSF file, this file includes each atom's force information
+
+

Examples

+
    +
  • Take the last step and save as XSF file
    +rsgrad traj -i -1 -x
  • +
+
$ rsgrad traj -i -1 -x
+[2022-07-14T18:37:35Z INFO  rsgrad::commands::traj] Parsing file "./OUTCAR" and "./POSCAR"
+[2022-07-14T18:37:35Z INFO  rsgrad::vasp_parsers::outcar] Saving ionic step to "./step_0003.xsf" ...
+[2022-07-14T18:37:35Z INFO  rsgrad] Time used: 11.223561ms
+
+

+
    +
  • Take the first step and save as POSCAR file
    +rsgrad traj -i 1 -s
  • +
+
$ rsgrad traj -i 1 -s
+[2022-07-14T18:38:51Z INFO  rsgrad::commands::traj] Parsing file "./OUTCAR" and "./POSCAR"
+[2022-07-14T18:38:51Z INFO  rsgrad::vasp_parsers::outcar] Saving trajectory step #    1 to "./POSCAR_00001.vasp" ...
+[2022-07-14T18:38:51Z INFO  rsgrad] Time used: 8.64197ms
+
+ +
+ + +
+
+ + + +
+ + + + + + + + + + + + diff --git a/TransitionDipoleMoment.html b/TransitionDipoleMoment.html new file mode 100644 index 0000000..7cc5b34 --- /dev/null +++ b/TransitionDipoleMoment.html @@ -0,0 +1,404 @@ + + + + + + Transition Dipole Moment - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
+ +
+ + + + + + + +
+
+

Transition Dipole Moment

+

This command (rsgrad tdm) calculates the transition dipole moment(tdm) +between given bands, and then plot the peaks with plotly.

+
+ +

Note: This command can only calculate the TDM between bands in same k-point. The inter-kpoint +transition is not supported yet. Also, this commands calculates the TDM in reciprocal space by

+

\[ +TDM_{i\to j} = \langle \phi_j | e\cdot\vec{r} | \phi_i \rangle = e\cdot\frac{i\hbar}{m_e\Delta E_{ij}} \langle \phi_j | \vec{p} | \phi_i \rangle +\]

+

Also, this command only calculates the TDM if \(j > i\), otherwise it will ignore the invalid \(i\to j\) pairs.

+

Help Message

+
$ rsgrad tdm --help
+rsgrad-tdm
+Calculate Transition Dipole Moment (TDM) between given bands.
+
+Note: This command can only calculate the TDM between bands in same k-point. The inter-kpoint
+transition is not supported yet. Also, this commands calculates the TDM in reciprocal space by
+
+tdm_{i->j} = <phi_j|e*r|phi_i> = i*ħ/(ΔE*m)*<phi_j|p|phi_i>
+
+USAGE:
+    rsgrad tdm [OPTIONS] --ibands <IBANDS>... --jbands <JBANDS>...
+
+OPTIONS:
+        --barwidth <BARWIDTH>
+            Specify the width of bars in the center of peaks. (eV)
+
+            [default: 0.1]
+
+        --gamma-half <GAMMA_HALF>
+            Gamma Half direction of WAVECAR. You need to set this to 'x' or 'z' when processing
+            WAVECAR produced by `vasp_gam`
+
+            [possible values: x, z]
+
+    -h, --help
+            Print help information
+
+        --htmlout <HTMLOUT>
+            Write the plot of TDM to html file
+
+            [default: tdm_smeared.html]
+
+    -i, --ibands <IBANDS>...
+            Initial band indices, start from 1
+
+    -j, --jbands <JBANDS>...
+            Final band indices, starts from 1
+
+    -k, --ikpoint <IKPOINT>
+            K-point index, starts from 1
+
+            [default: 1]
+
+        --npoints <NPOINTS>
+            How many points in the x axis PER eV
+
+            [default: 500]
+
+        --peakout <PEAKOUT>
+            Write the TDM peaks to raw txt file
+
+            [default: tdm_peaks.txt]
+
+    -s, --ispin <ISPIN>
+            Spin index, 1 for up, 2 for down
+
+            [default: 1]
+            [possible values: 1, 2]
+
+        --show
+            Open the default browser to show the plot
+
+        --sigma <SIGMA>
+            Smearing width, in eV
+
+            [default: 0.05]
+
+        --to-inline-html
+            Print the inline HTML to stdout
+
+        --txtout <TXTOUT>
+            Write the summed and smeared TDM to raw txt file
+
+            [default: tdm_smeared.txt]
+
+    -v, --verbose
+            Print the calculated TDM to screen
+
+    -w, --wavecar <WAVECAR>
+            WAVECAR file path
+
+            [default: ./WAVECAR]
+
+        --xmax <XMAX>
+            Highest energy scale for tdm_smeared.txt, default for max(dE) + 2.0
+
+        --xmin <XMIN>
+            Lowest energy scale for tdm_smeared.txt, default for min(dE) - 2.0
+
+

Example

+

The -i and -j arguments are required, or it will complain with error.

+
$ rsgrad tdm -i 2 -j {3..5}
+[2022-08-10T07:26:46Z INFO  rsgrad::commands::tdm] Reading "./WAVECAR"
+[2022-08-10T07:26:46Z INFO  rsgrad::commands::tdm] Writing peaks info to "tdm_peaks.txt" ...
+[2022-08-10T07:26:46Z INFO  rsgrad::commands::tdm] Writing smeared TDM data to "tdm_smeared.txt"
+[2022-08-10T07:26:46Z INFO  rsgrad::commands::tdm] Writing plot to "tdm_smeared.html"
+[2022-08-10T07:26:46Z INFO  rsgrad] Time used: 56.655387ms
+
+

It produces the HTML like:

+
+ +

You can view the \(x\), \(y\) and \(z\) components of each peak by hovering on the thin bars +at the center of peaks.

+

Note: If two peaks are in the same x position, one of them will be covered.

+

Then the tdm_peaks.txt should be like:

+
# iband jband     E_i     E_j      ΔE        Tx       Ty       Tz
+      2     3  -5.974  -3.675   2.298     1.311    2.556    0.000
+      2     4  -5.974  -3.675   2.298     2.556    1.311    0.000
+      2     5  -5.974  -0.975   4.999     0.000    0.000    5.309
+
+

And the tdm_smeared.txt should be like:

+
# E(eV)    Tx(Debye)   Ty(Debye)   Tz(Debye)
+         0.298325         0.007692         0.007692         0.001912         0.017295
+         0.300240         0.007706         0.007706         0.001914         0.017326
+         0.302155         0.007721         0.007721         0.001915         0.017357
+         0.304070         0.007736         0.007736         0.001917         0.017389
+         0.305985         0.007751         0.007751         0.001918         0.017420
+         0.307900         0.007766         0.007766         0.001920         0.017451
+...
+...
+
+

Then you can plot the TDM peaks with other tools like OriginPro.

+

If your WAVECAR is produced by vasp_gam, you'd better specify the gamma half direction by --gamma-half x or --gamma-half z, +or rsgrad tdm will produce wrong results.

+ +
+ + +
+
+ + + +
+ + + + + + + + + + + + diff --git a/UnitConversion.html b/UnitConversion.html new file mode 100644 index 0000000..df7c391 --- /dev/null +++ b/UnitConversion.html @@ -0,0 +1,281 @@ + + + + + + UnitConversion - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
+ +
+ + + + + + + +
+
+

UnitConversion

+

This command (rsgrad uc) converts input quantity to units representing same energy.

+

Metric prefixes are supported, from Atto(a, 10-18) to Exa(E, 1018).

+

Here are supported prefixes and corresponding acronyms:

+ + + + + + + + + + + + + + +
Metric prefixAcronymBase 10
attoa10-18
femtof10-15
picop10-12
nanon10-9
microμ10-6
millim10-3
----100
KiloK103
MegaM106
GigaG109
TeraT1012
PetaP1015
exaE1018
+

If you use acronyms, note that prefixes smaller than 1 (from a, atto to m, micro) must be +lowercased whereas the prefixes lager than 1 (from K, Kilo to E, Exa) must be uppercased.

+

Supported units:

+ + + + + + + + + + +
UnitSymbol
HartreeHa
Wavenumbercm-1
Temperature(Kelvin)K
Calorie per moleCal/mol
Joule per moleJ/mol
Wavelengthm
Periods
Electron volteV
FrequencyHz
+

Help Message

+
$ rsgrad uc
+Conversion between various energy units
+
+Usage: rsgrad uc [INPUT]...
+
+Arguments:
+  [INPUT]...  Input energy quantity to be converted. Multiple input are supported
+
+Options:
+  -h, --help  Print help
+
+Try `rsgrad uc 298K` to see what happens.
+
+

Examples

+
$ rsgrad uc 298K
+==================== Processing input "298K" ====================
+  298.000000 K ==   943.709369 μHa
+  298.000000 K ==   207.125149 cm-1
+  298.000000 K ==   298.000000 K
+  298.000000 K ==   592.202785 Cal/mol
+  298.000000 K ==     2.477776 KJ/mol
+  298.000000 K ==    48.281101 μm
+  298.000000 K ==   161.048425 fs
+  298.000000 K ==    25.679653 meV
+  298.000000 K ==     6.209312 THz
+================================================================================
+
+[2024-09-11T07:21:07Z INFO  rsgrad] Time used: 470.398µs
+
+

You can also input multiple quantities at a time

+
$ rsgrad uc 298K 25meV 300THz
+==================== Processing input "298K" ====================
+  298.000000 K ==   161.048425 fs
+  298.000000 K ==   207.125149 cm-1
+  298.000000 K ==     2.477776 KJ/mol
+  298.000000 K ==    25.679653 meV
+  298.000000 K ==    48.281101 μm
+  298.000000 K ==   943.709369 μHa
+  298.000000 K ==   592.202785 Cal/mol
+  298.000000 K ==     6.209312 THz
+  298.000000 K ==   298.000000 K
+================================================================================
+
+==================== Processing input "25meV" ====================
+   25.000000 meV ==   165.426708 fs
+   25.000000 meV ==   201.643250 cm-1
+   25.000000 meV ==     2.412198 KJ/mol
+   25.000000 meV ==    25.000000 meV
+   25.000000 meV ==    49.593677 μm
+   25.000000 meV ==   918.732590 μHa
+   25.000000 meV ==   576.529191 Cal/mol
+   25.000000 meV ==     6.044973 THz
+   25.000000 meV ==   290.112953 K
+================================================================================
+
+==================== Processing input "300THz" ====================
+  300.000000 THz ==     3.333333 fs
+  300.000000 THz ==    10.007154 Kcm-1
+  300.000000 THz ==   119.712599 KJ/mol
+  300.000000 THz ==     1.240700 eV
+  300.000000 THz ==   999.308150 nm
+  300.000000 THz ==    45.594872 mHa
+  300.000000 THz ==    28.611998 KCal/mol
+  300.000000 THz ==   300.000000 THz
+  300.000000 THz ==    14.397729 KK
+================================================================================
+
+[2024-09-11T07:27:53Z INFO  rsgrad] Time used: 544.171µs
+
+ +
+ + +
+
+ + + +
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b/Vibration.html new file mode 100644 index 0000000..70dba66 --- /dev/null +++ b/Vibration.html @@ -0,0 +1,273 @@ + + + + + + Vibration - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +

+ +
+ +
+ + + + + + + +
+
+

Vibration

+

For systems enabled vibration calculation (phonon at Γ point only), rsgrad vib can

+
    +
  • Print the phonon eigenvalues;
  • +
  • Save the phonon eigenvectors;
  • +
  • Modulate the ground-state according to specified modes.
  • +
+

Help Message

+
$ rsgrad vib --help
+rsgrad-vib
+Tracking vibration information.
+
+For systems enabled vibration mode calculation, this command can extract phonon eigenvalues and
+phonon eigenvectors at Gamma point.
+
+USAGE:
+    rsgrad vib [OPTIONS] [--] [OUTCAR]
+
+ARGS:
+    <OUTCAR>
+            Specify the input OUTCAR file
+
+            [default: ./OUTCAR]
+
+OPTIONS:
+    -a, --amplitude <AMPLITUDE>
+            Modulation amplitude coefficient, to avoid precision issue, abs(amplitude) >= 0.01
+            should be satisfied
+
+            [default: 0.1]
+
+    -c, --cartesian
+            Catesian coordinate is used when writting POSCAR. Fractional coordinate is used by
+            default
+
+    -h, --help
+            Print help information
+
+    -i, --select-indices <SELECT_INDICES>...
+            Selects the mode indices to operate.
+
+            Step indices start from '1', if '0' is given, all the structures will be selected. Step
+            indices can be negative, where negative index means counting reversely. E.g. "-i -2 -1 1
+            2 3" means selecting the last two and first three steps.
+
+    -l, --list
+            Shows vibration modes in brief
+
+    -m, --modulate
+            Modulate the ground-state POSCAR with respect to a certern vibration frequencies
+
+    -p, --poscar <POSCAR>
+            Specify the input POSCAR file, the consntraints info is needed
+
+            [default: ./POSCAR]
+
+        --save-in <SAVE_IN>
+            Define where the files would be saved
+
+            [default: .]
+
+    -x, --save-as-xsfs
+            Saves each selected modes to XSF file
+
+

Example

+
    +
  • +

    Print the phonon eigenvalues; +

    +
  • +
  • +

    Save the phonon eigenvectors;

    +
  • +
+
$ rsgrad vib -i {1..3} {-3..-1} -x
+[2022-07-14T18:32:49Z INFO  rsgrad::commands::vib] Parsing file "./OUTCAR"
+[2022-07-14T18:32:49Z INFO  rsgrad::vasp_parsers::outcar] Saving mode #   1 as "./mode_0001_3682.13cm-1.xsf" ...
+[2022-07-14T18:32:49Z INFO  rsgrad::vasp_parsers::outcar] Saving mode #   3 as "./mode_0003_3679.99cm-1.xsf" ...
+[2022-07-14T18:32:49Z INFO  rsgrad::vasp_parsers::outcar] Saving mode #  44 as "./mode_0044_0010.79cm-1_imag.xsf" ...
+[2022-07-14T18:32:49Z INFO  rsgrad::vasp_parsers::outcar] Saving mode #  43 as "./mode_0043_0007.12cm-1_imag.xsf" ...
+[2022-07-14T18:32:49Z INFO  rsgrad::vasp_parsers::outcar] Saving mode #   2 as "./mode_0002_3680.83cm-1.xsf" ...
+[2022-07-14T18:32:49Z INFO  rsgrad::vasp_parsers::outcar] Saving mode #  45 as "./mode_0045_0047.20cm-1_imag.xsf" ...
+[2022-07-14T18:32:49Z INFO  rsgrad] Time used: 109.566967ms
+
+

+
    +
  • Modulate the ground-state according to specified modes.
  • +
+
$ rsgrad vib -i {-3..-1} --modulate --amplitude 0.1
+[2022-07-14T18:31:41Z INFO  rsgrad::commands::vib] Parsing file "./OUTCAR"
+[2022-07-14T18:31:41Z INFO  rsgrad::vasp_parsers::outcar] Saving modulated POSCAR of mode #  43 with amplitude coeff 0.100 as "./mode_0043_0007.12cm-1_0.100_imag.vasp" ...
+[2022-07-14T18:31:41Z INFO  rsgrad::vasp_parsers::outcar] Saving modulated POSCAR of mode #  44 with amplitude coeff 0.100 as "./mode_0044_0010.79cm-1_0.100_imag.vasp" ...
+[2022-07-14T18:31:41Z INFO  rsgrad::vasp_parsers::outcar] Saving modulated POSCAR of mode #  45 with amplitude coeff 0.100 as "./mode_0045_0047.20cm-1_0.100_imag.vasp" ...
+[2022-07-14T18:31:41Z INFO  rsgrad] Time used: 202.629805ms
+
+ +
+ + +
+
+ + + +
+ + + + + + + + + + + + diff --git a/Wave1D-example-inline.html b/Wave1D-example-inline.html new file mode 100644 index 0000000..4db494e --- /dev/null +++ b/Wave1D-example-inline.html @@ -0,0 +1,54 @@ +
+ diff --git a/Wave1D-example-inline0.html b/Wave1D-example-inline0.html new file mode 100644 index 0000000..a721f56 --- /dev/null +++ b/Wave1D-example-inline0.html @@ -0,0 +1,28 @@ +
+ diff --git a/Wavefunction1D.html b/Wavefunction1D.html new file mode 100644 index 0000000..7f3ba50 --- /dev/null +++ b/Wavefunction1D.html @@ -0,0 +1,354 @@ + + + + + + Wavefunction 1D - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
+ +
+ + + + + + + +
+
+

Wavefunction 1D

+

This command is similar to rsgrad wav3d. The only difference is that wav1d integrates +the wavefunction over specified plane, and produces the averaged one dimensional wavefunction.

+

This command is useful when you are looking for image potential states.

+
+ +

Help Message

+
$ rsgrad wav1d --help
+rsgrad-wav1d 
+Plot wavefunction in realspace, then integrate over some plane, and save it as '.txt' file
+
+USAGE:
+    rsgrad wav1d [OPTIONS]
+
+OPTIONS:
+        --axis <AXIS>
+            Integration direction. e.g. if 'z' is provided, the XoY plane is integrated
+            
+            [default: z]
+            [possible values: X, Y, Z]
+
+    -b, --ibands <IBANDS>...
+            Select band index, starting from 1
+
+    -d, --detail
+            Show the eigen values and band occupations of current WAVECAR.
+            
+            This flag should be used with `--list`
+
+        --gamma-half <GAMMA_HALF>
+            Gamma Half direction of WAVECAR. You need to set this to 'x' or 'z' when processing
+            WAVECAR produced by `vasp_gam`
+            
+            [possible values: x, z]
+
+    -h, --help
+            Print help information
+
+        --htmlout <HTMLOUT>
+            Specify the file name to be written with html wav1d data
+            
+            [default: wav1d.html]
+
+    -k, --ikpoints <IKPOINTS>...
+            Select kpoint index, starting from 1
+            
+            [default: 1]
+
+    -l, --list
+            List the brief info of current WAVECAR
+
+    -s, --ispins <ISPINS>...
+            Select spin index, starting from 1
+            
+            [default: 1]
+
+        --scale <SCALE>
+            Scale the wavefunction
+            
+            [default: 10]
+
+        --show
+            Open the browser and show the plot immediately
+
+        --to-inline-html
+            Render the plot and print thw rendered code to stdout
+
+        --txtout <TXTOUT>
+            Specify the file name to be written with raw wav1d data
+            
+            [default: wav1d.txt]
+
+    -w, --wavecar <WAVECAR>
+            WAVECAR file name
+            
+            [default: ./WAVECAR]
+
+

Example

+

The usage is similar to rsgrad wav3d, too.

+
$ rsgrad wav1d -b {20..27}
+[2022-07-14T12:54:35Z INFO  rsgrad::commands::wav1d] Reading WAVECAR: "./WAVECAR"
+[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Processing spin 1, k-point   1, band   20 ...
+[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Processing spin 1, k-point   1, band   24 ...
+[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Processing spin 1, k-point   1, band   22 ...
+[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Processing spin 1, k-point   1, band   23 ...
+[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Processing spin 1, k-point   1, band   21 ...
+[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Processing spin 1, k-point   1, band   26 ...
+[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Processing spin 1, k-point   1, band   27 ...
+[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Processing spin 1, k-point   1, band   25 ...
+[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Writing to "wav1d.html"
+[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Writing to "wav1d.txt"
+[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Printing inline html to stdout ...
+[2022-07-14T12:54:36Z INFO  rsgrad] Time used: 864.911523ms
+
+

Then produces

+
+ +

Note: The Fermi level is shiftted to 0.0 eV

+ +
+ + +
+
+ + + +
+ + + + + + + + + + + + diff --git a/Wavefunction3D-example.png b/Wavefunction3D-example.png new file mode 100644 index 0000000000000000000000000000000000000000..8c31f97b7e00ae5781088fe2254c8896f0de494b GIT binary patch literal 125147 zcmeFY^>ZCDw!*T|A*$IM5db(2F>*Gb|4>qN^7`7qe|+*?{kI=X zllVc&K~at0*O$In#6*$*J-BOVNS9^&UeG*^h{f}`EB|Fj0(kC9jC4#145p#Di z0*Is!sj@JC4)8|U?;}JtkeYZEhj(SLPGZem(#gi9p1km;PWtf+(7J^>Lo(;H(*KG> z$ZWbvJsFyZ)qLm8?^!+Dq-3{z> zEMAJuX*NF;#akzH({_F=NIQ|5S~tuMaCNZjs12~W89XBd8EhjT69b<8VO^SGEFM=n zO;?g4Jj^3*2Ln}n*>fT`*$Hzf_BAwTZ9%rSfb`Ceg^?ZG!9O{{D)Q5(^^XN3&wQTx z<7Td7n1Dtsh&(qxHS=0{fE6l$LHBz(r@2;G#=8O7H-!Ke1(;PqqI7_?0sQv>x@*X8 zVwB(jY7}HF2&C;G8Di+RJU|uLP#%U2w6@UCzlf*3U=BFnp+I>M+0aLQrVa$_(8z)U zIN(2esXdT~Nnra$Fv6kBMY!WhOpsQD5k?7aLjv<*sR^Y5l}Jd)L*Vk76lheCR7Je< zJde$fIbHDDVIPE_^1v)0Jt2HTQPUCV2DEBXd6CU}WjJAD1F`$cua!877y~)_RUH_- zVeJCs2hw)d90cCM2}J;;VP&N4;S~LXoe50jV84V0N2Q7&%SEjc#ES?{#O+8wMy2=B zp~LbGk8z}<=_mo{F*^pSMruav1{KUOObqD_=~?MulhlX!sey}wnZ~-c^fuqwF|(o= 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zm?Gxn#d0WFU1-DFBO=dH`3jg(ii}w9O>~>a18aBQi70ybN0O~DshQ4bP-kh(3GnTt zXG&olFV=4L?pJ9Vnp1uSKJo-`f2TVT_;39Y_SxFqc0+XZ(ZY|*^U|sFeo@05i^Yn? zmU)ffTxYqfZ={Tu+AEg$jdx_bi6R*?ZMIq#(=+%hmYQxLpCjvvYW&HtcyHTLz(S=G zJ8q4^d}-TAxTo<)z5dgUsWi|{ZRdS&lJR4+_q~2s*Vx$TQDh%WvY%jp^1fLR(F&eQ znN3stX!?{|cecIaM8oX6lKG^epP~>Tt9f4VOzG5w@2Al6Kp~($kut<(Z!#`lhnD%$zB#E%vn;IkJ0 zXK@+fdVGLgQ%<-ViJ` zXJ*Vnc5-5fgCk9pSI5=4nV6s)6Luu7ql$_;h^%XLHXd|8?V+NzHvh27@D-@UP^zKdF(LiWVv}J37JAeS?ZT^n zMyP_AP6W46GgS{6A{{_uu%^AN1&H8sLfivkbZZI4XPd z;#ql$e<;-dX+5_Y7eJRD%UnzTk#4v+0&pzX`3p*B!uzjj{2{dfsN;3jO4dK}VT8x}a}*%&VcLZM8y$%P(CwoSZ9@MU*5BDgsDLQ2 zrbrhE{*9)S1L(+dyN4?<|Nq_Y+&F;b$-jc@nf?pq1JH~X-^-(aCM=F?@fuigUKMi- uwf{nG|DdkVd&|IQ>3>`PKO^9dXB6hbeP2T*Mzj~e4 + + + + + Wavefunction 3D - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
+ +
+ + + + + + + +
+
+

Wavefunction 3D

+

Main functions of rsgrad wav3d

+
    +
  • List the brief information of WAVECAR;
  • +
  • Save the selected wavefunction to .vasp file.
  • +
+

Help Message

+
$ rsgrad wav3d --help
+Plot wavefunction in realspace, and save it as '.vasp' file
+
+Usage: rsgrad wav3d [OPTIONS]
+
+Options:
+  -w, --wavecar <WAVECAR>
+          WAVECAR file name
+          
+          [default: ./WAVECAR]
+
+  -p, --poscar <POSCAR>
+          POSCAR filename, POSCAR is needed to get the real-space wavefunction
+          
+          [default: ./POSCAR]
+
+  -s, --ispins [<ISPINS>...]
+          Select spin index, starting from 1
+          
+          [default: 1]
+
+  -k, --ikpoints [<IKPOINTS>...]
+          Select kpoint index, starting from 1.
+          
+          You can input ranges directly: `-k 1..4 5..10`
+          
+          [default: 1]
+
+  -b, --ibands [<IBANDS>...]
+          Select band index, starting from 1.
+          
+          You can input ranges directly: `-b 1..4 5..10`
+
+  -l, --list
+          List the brief info of current WAVECAR
+
+  -d, --detail
+          Show the eigen values and band occupations of current WAVECAR.
+          
+          This flag should be used with `--list`
+
+      --gamma-half <GAMMA_HALF>
+          Gamma Half direction of WAVECAR. You need to set this to 'x' or 'z' when processing WAVECAR produced by `vasp_gam`
+          
+          [possible values: x, z]
+
+      --ngrid <NGRID> <NGRID> <NGRID>
+          Grid size for realspace wavefunction, 3 numbers are required, i.e. NGXF NGYF and NGZF.
+          
+          If this argument is left empty, NG_F will be set as NG_F=2*NG_.
+          
+          Be aware that NG_F must be greater than or at least equal to corresponding NG_.
+
+  -o, --output-parts [<OUTPUT_PARTS>...]
+          Specify output part of the wavefunction.
+          
+          Detailed message:
+           - normsquared/ns: Perform `ρ(r) = |ѱ(r)|^2` action to get the spatial distribution of selected band.
+           - real/re: Real part of the wavefunction, suffix '_re.vasp' is added to the output filename.
+           - imag/im: Imaginary part of the wavefunction, suffix '_im.vasp' is added to the output filename.
+           - reim: Output both real part and imaginary parts of the wavefunction.
+           - uns/dns: Perform `ρ(r) = |ѱ(r)|^2` for spinor up/down only. **Note: this option works for `ncl` WAVECAR only.**
+          
+          [possible values: normsquared, ns, uns, dns, real, re, imag, im, reim]
+
+      --prefix <PREFIX>
+          Prefix of output filename
+          
+          [default: wav]
+
+  -e, --show-eigs-suffix
+          Add eigen value suffix to the filename
+
+      --sum-chgs
+          Perform sum-up of the charge densities for selected bands.
+          
+          With this flag open, only `normsquared` or `ns` or `uns` or `dns` are allowed for the `-o`/`--output-parts` option.
+           IMPORTANT NOTES:
+           - The prefix for output filename `sum-prefix` is also required and has no default prefix.
+           - The individual charge densities will not be saved to corresponding '.vasp' files if this flag is on.
+
+      --sum-prefix <SUM_PREFIX>
+          Specify the output file for the summed charge densities.
+          
+          This argument is required if `sum_chgs` is on.
+
+  -h, --help
+          Print help (see a summary with '-h')
+
+

Example

+
    +
  • List the brief information of WAVECAR
  • +
+
$ rsgrad wav3d -l
+
+[2022-07-14T09:19:51Z INFO  rsgrad::commands::wav3d] Reading WAVECAR: "./WAVECAR"
+LENGTH     =             54145104
+RECLEN     =              1388336
+TYPE       =             Standard
+NSPIN      =                    1
+NKPTS      =                    1
+NBANDS     =                   36
+ENCUT      =              450.000
+EFERMI     =               -5.368
+VOLUME     =             8000.000
+NGRID      = [  71,   71,   71]
+NPLWS      = [173541]
+ACELL      = [[  20.000,    0.000,    0.000], [   0.000,   20.000,    0.000], [   0.000,    0.000,   20.000]]
+BCELL      = [[   0.050,    0.000,    0.000], [   0.000,    0.050,    0.000], [   0.000,    0.000,    0.050]]
+
+
+[2022-07-14T09:19:51Z INFO  rsgrad] Time used: 160.337862ms
+
+

if you want the band eigen values information

+
$ rsgrad wav3d -ld
+
+...
+<BRIEF INFORMATION ABOUT WAVECAR>
+...
+
+ISPIN:  1  IKPOINT:    1  IBAND:     1 E-Efermi:    -19.991 Occupation: 1.000
+ISPIN:  1  IKPOINT:    1  IBAND:     2 E-Efermi:    -18.141 Occupation: 1.000
+ISPIN:  1  IKPOINT:    1  IBAND:     3 E-Efermi:    -18.141 Occupation: 1.000
+ISPIN:  1  IKPOINT:    1  IBAND:     4 E-Efermi:    -16.418 Occupation: 1.000
+ISPIN:  1  IKPOINT:    1  IBAND:     5 E-Efermi:    -15.534 Occupation: 1.000
+ISPIN:  1  IKPOINT:    1  IBAND:     6 E-Efermi:    -15.532 Occupation: 1.000
+ISPIN:  1  IKPOINT:    1  IBAND:     7 E-Efermi:    -10.662 Occupation: 1.000
+ISPIN:  1  IKPOINT:    1  IBAND:     8 E-Efermi:    -10.661 Occupation: 1.000
+...
+
+
    +
  • Save the selected wavefunction to .vasp file
  • +
+
$ rsgrad wav3d -b {10..20} -o ns -e
+
+[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Reading WAVECAR: "./WAVECAR"
+[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Reading POSCAR: "./POSCAR"
+[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   10 ...
+[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   13 ...
+[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   11 ...
+[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   14 ...
+[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   12 ...
+[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   15 ...
+[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-13_-5.740eV.vasp" ...
+[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-15_-5.601eV.vasp" ...
+[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-14_-5.728eV.vasp" ...
+[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-10_-8.376eV.vasp" ...
+[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-11_-7.385eV.vasp" ...
+[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-12_-7.380eV.vasp" ...
+[2022-07-14T09:23:08Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   18 ...
+[2022-07-14T09:23:08Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   19 ...
+[2022-07-14T09:23:09Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-18_-3.514eV.vasp" ...
+[2022-07-14T09:23:09Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   16 ...
+[2022-07-14T09:23:09Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   20 ...
+[2022-07-14T09:23:09Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-19_-3.265eV.vasp" ...
+[2022-07-14T09:23:09Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   17 ...
+[2022-07-14T09:23:10Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-16_-5.477eV.vasp" ...
+[2022-07-14T09:23:10Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-17_-3.546eV.vasp" ...
+[2022-07-14T09:23:10Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-20_-0.701eV.vasp" ...
+[2022-07-14T09:23:11Z INFO  rsgrad] Time used: 5.484733549s
+
+

Open the .vasp in VESTA

+

+

rsgrad wav3d supports extracting multiple bands at the same time, and the processes +executed in parallel, which can save a lot of time.

+ +
+ + +
+
+ + + +
+ + + + + + + + + + + + diff --git a/Workfunction-example0.html b/Workfunction-example0.html new file mode 100644 index 0000000..d3a2918 --- /dev/null +++ b/Workfunction-example0.html @@ -0,0 +1,18 @@ +
+ diff --git a/Workfunction-example1.html b/Workfunction-example1.html new file mode 100644 index 0000000..56cc798 --- /dev/null +++ b/Workfunction-example1.html @@ -0,0 +1,18 @@ +
+ diff --git a/Workfunction.html b/Workfunction.html new file mode 100644 index 0000000..a416a1f --- /dev/null +++ b/Workfunction.html @@ -0,0 +1,277 @@ + + + + + + Workfunction - RSGRAD'S BOOK + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
+ +
+ + + + + + + +
+
+

Workfunction

+

rsgrad workfunc reads LOCPOT to calculate the work function. For further discussion about +work function, please read this blog.

+
+ +

Note: rsgrad workfunc does not show the vacuum level directly, hence you need to find it by +hovering on the step of the work function. Take the work function above as an example, the +vacuum level should be about 4.048eV around 40Å.

+

Help Message

+
$ rsgrad workfunc --help
+rsgrad-workfunc
+Calculate work-function from LOCPOT file, OUTCAR is also needed to get the Fermi level.
+
+The work function is calculated by plannar integration of the data cube in LOCPOT. The selected axis
+should be perpendicular to the other two axises.
+
+USAGE:
+    rsgrad workfunc [OPTIONS] [LOCPOT]
+
+ARGS:
+    <LOCPOT>
+            LOCPOT file path. Turn on 'LVHAR' in INCAR to get the electro-static potential saved it
+
+            [default: ./LOCPOT]
+
+OPTIONS:
+        --axis <AXIS>
+            Integration direction. e.g. if 'z' is provided, the XoY plane is integrated
+
+            [default: z]
+            [possible values: X, Y, Z]
+
+    -h, --help
+            Print help information
+
+    -o, --htmlout <HTMLOUT>
+            Write the plot to html and view it in the web browser
+
+            [default: ./workfunction.html]
+
+        --outcar <OUTCAR>
+            OUTCAR file path. This file is needed to get the E-fermi level and lattice properties
+
+            [default: ./OUTCAR]
+
+        --show
+            Open default browser to see the plot immediately
+
+        --to-inline-html
+            Render the plot and print the rendered code to stdout
+
+        --txtout <TXTOUT>
+            Write the raw plot data as txt file in order to replot it with more advanced tools
+
+            [default: locpot.txt]
+
+

Example

+

In general, you don't need t provide additional arguments.

+
$ rsgrad workfunc
+[2022-07-14T14:41:38Z INFO  rsgrad::commands::workfunc] Reading "./OUTCAR"
+[2022-07-14T14:41:38Z INFO  rsgrad::commands::workfunc] Reading electro-static potential data from "./LOCPOT"
+[2022-07-14T14:41:39Z INFO  rsgrad::commands::workfunc] Writing raw plot data to "locpot.txt"
+[2022-07-14T14:41:39Z INFO  rsgrad::commands::workfunc] Writing to "./workfunction.html"
+[2022-07-14T14:41:39Z INFO  rsgrad] Time used: 1.352347116s
+
+
+ + +
+ + +
+
+ + + +
+ + + + + + + + + + + + diff --git a/ayu-highlight.css b/ayu-highlight.css new file mode 100644 index 0000000..0c45c6f --- /dev/null +++ b/ayu-highlight.css @@ -0,0 +1,79 @@ +/* +Based off of the Ayu theme +Original by Dempfi (https://github.com/dempfi/ayu) +*/ + +.hljs { + display: block; + overflow-x: auto; + background: #191f26; + color: #e6e1cf; + padding: 0.5em; +} + +.hljs-comment, +.hljs-quote { + color: #5c6773; + font-style: italic; +} + +.hljs-variable, +.hljs-template-variable, +.hljs-attribute, +.hljs-attr, +.hljs-regexp, +.hljs-link, +.hljs-selector-id, +.hljs-selector-class { + color: #ff7733; +} + +.hljs-number, +.hljs-meta, +.hljs-builtin-name, +.hljs-literal, +.hljs-type, +.hljs-params { + color: #ffee99; +} + +.hljs-string, +.hljs-bullet { + color: #b8cc52; +} + +.hljs-title, +.hljs-built_in, +.hljs-section { + color: #ffb454; +} + +.hljs-keyword, +.hljs-selector-tag, +.hljs-symbol { + color: #ff7733; +} + +.hljs-name { + color: #36a3d9; +} + +.hljs-tag { + color: #00568d; +} + +.hljs-emphasis { + font-style: italic; +} + +.hljs-strong { + font-weight: bold; +} + +.hljs-addition { + color: #91b362; +} + +.hljs-deletion { + color: #d96c75; +} diff --git a/book.js b/book.js new file mode 100644 index 0000000..d40440c --- /dev/null +++ b/book.js @@ -0,0 +1,679 @@ +"use strict"; + +// Fix back button cache problem +window.onunload = function () { }; + +// Global variable, shared between modules +function playground_text(playground) { + let code_block = playground.querySelector("code"); + + if (window.ace && code_block.classList.contains("editable")) { + let editor = window.ace.edit(code_block); + return editor.getValue(); + } else { + return code_block.textContent; + } +} + +(function codeSnippets() { + function fetch_with_timeout(url, options, timeout = 6000) { + return Promise.race([ + fetch(url, options), + new Promise((_, reject) => setTimeout(() => reject(new Error('timeout')), timeout)) + ]); + } + + var playgrounds = Array.from(document.querySelectorAll(".playground")); + if (playgrounds.length > 0) { + fetch_with_timeout("https://play.rust-lang.org/meta/crates", { + headers: { + 'Content-Type': "application/json", + }, + method: 'POST', + mode: 'cors', + }) + .then(response => response.json()) + .then(response => { + // get list of crates available in the rust playground + let playground_crates = response.crates.map(item => item["id"]); + playgrounds.forEach(block => handle_crate_list_update(block, playground_crates)); + }); + } + + function handle_crate_list_update(playground_block, playground_crates) { + // update the play buttons after receiving the response + update_play_button(playground_block, playground_crates); + + // and install on change listener to dynamically update ACE editors + if (window.ace) { + let code_block = playground_block.querySelector("code"); + if (code_block.classList.contains("editable")) { + let editor = window.ace.edit(code_block); + editor.addEventListener("change", function (e) { + update_play_button(playground_block, playground_crates); + }); + // add Ctrl-Enter command to execute rust code + editor.commands.addCommand({ + name: "run", + bindKey: { + win: "Ctrl-Enter", + mac: "Ctrl-Enter" + }, + exec: _editor => run_rust_code(playground_block) + }); + } + } + } + + // updates the visibility of play button based on `no_run` class and + // used crates vs ones available on http://play.rust-lang.org + function update_play_button(pre_block, playground_crates) { + var play_button = pre_block.querySelector(".play-button"); + + // skip if code is `no_run` + if (pre_block.querySelector('code').classList.contains("no_run")) { + play_button.classList.add("hidden"); + return; + } + + // get list of `extern crate`'s from snippet + var txt = playground_text(pre_block); + var re = /extern\s+crate\s+([a-zA-Z_0-9]+)\s*;/g; + var snippet_crates = []; + var item; + while (item = re.exec(txt)) { + snippet_crates.push(item[1]); + } + + // check if all used crates are available on play.rust-lang.org + var all_available = snippet_crates.every(function (elem) { + return playground_crates.indexOf(elem) > -1; + }); + + if (all_available) { + play_button.classList.remove("hidden"); + } else { + play_button.classList.add("hidden"); + } + } + + function run_rust_code(code_block) { + var result_block = code_block.querySelector(".result"); + if (!result_block) { + result_block = document.createElement('code'); + result_block.className = 'result hljs language-bash'; + + code_block.append(result_block); + } + + let text = playground_text(code_block); + let classes = code_block.querySelector('code').classList; + let edition = "2015"; + if(classes.contains("edition2018")) { + edition = "2018"; + } else if(classes.contains("edition2021")) { + edition = "2021"; + } + var params = { + version: "stable", + optimize: "0", + code: text, + edition: edition + }; + + if (text.indexOf("#![feature") !== -1) { + params.version = "nightly"; + } + + result_block.innerText = "Running..."; + + fetch_with_timeout("https://play.rust-lang.org/evaluate.json", { + headers: { + 'Content-Type': "application/json", + }, + method: 'POST', + mode: 'cors', + body: JSON.stringify(params) + }) + .then(response => response.json()) + .then(response => { + if (response.result.trim() === '') { + result_block.innerText = "No output"; + result_block.classList.add("result-no-output"); + } else { + result_block.innerText = response.result; + result_block.classList.remove("result-no-output"); + } + }) + .catch(error => result_block.innerText = "Playground Communication: " + error.message); + } + + // Syntax highlighting Configuration + hljs.configure({ + tabReplace: ' ', // 4 spaces + languages: [], // Languages used for auto-detection + }); + + let code_nodes = Array + .from(document.querySelectorAll('code')) + // Don't highlight `inline code` blocks in headers. + .filter(function (node) {return !node.parentElement.classList.contains("header"); }); + + if (window.ace) { + // language-rust class needs to be removed for editable + // blocks or highlightjs will capture events + code_nodes + .filter(function (node) {return node.classList.contains("editable"); }) + .forEach(function (block) { block.classList.remove('language-rust'); }); + + Array + code_nodes + .filter(function (node) {return !node.classList.contains("editable"); }) + .forEach(function (block) { hljs.highlightBlock(block); }); + } else { + code_nodes.forEach(function (block) { hljs.highlightBlock(block); }); + } + + // Adding the hljs class gives code blocks the color css + // even if highlighting doesn't apply + code_nodes.forEach(function (block) { block.classList.add('hljs'); }); + + Array.from(document.querySelectorAll("code.language-rust")).forEach(function (block) { + + var lines = Array.from(block.querySelectorAll('.boring')); + // If no lines were hidden, return + if (!lines.length) { return; } + block.classList.add("hide-boring"); + + var buttons = document.createElement('div'); + buttons.className = 'buttons'; + buttons.innerHTML = ""; + + // add expand button + var pre_block = block.parentNode; + pre_block.insertBefore(buttons, pre_block.firstChild); + + pre_block.querySelector('.buttons').addEventListener('click', function (e) { + if (e.target.classList.contains('fa-eye')) { + e.target.classList.remove('fa-eye'); + e.target.classList.add('fa-eye-slash'); + e.target.title = 'Hide lines'; + e.target.setAttribute('aria-label', e.target.title); + + block.classList.remove('hide-boring'); + } else if (e.target.classList.contains('fa-eye-slash')) { + e.target.classList.remove('fa-eye-slash'); + e.target.classList.add('fa-eye'); + e.target.title = 'Show hidden lines'; + e.target.setAttribute('aria-label', e.target.title); + + block.classList.add('hide-boring'); + } + }); + }); + + if (window.playground_copyable) { + Array.from(document.querySelectorAll('pre code')).forEach(function (block) { + var pre_block = block.parentNode; + if (!pre_block.classList.contains('playground')) { + var buttons = pre_block.querySelector(".buttons"); + if (!buttons) { + buttons = document.createElement('div'); + buttons.className = 'buttons'; + pre_block.insertBefore(buttons, pre_block.firstChild); + } + + var clipButton = document.createElement('button'); + clipButton.className = 'fa fa-copy clip-button'; + clipButton.title = 'Copy to clipboard'; + clipButton.setAttribute('aria-label', clipButton.title); + clipButton.innerHTML = ''; + + buttons.insertBefore(clipButton, buttons.firstChild); + } + }); + } + + // Process playground code blocks + Array.from(document.querySelectorAll(".playground")).forEach(function (pre_block) { + // Add play button + var buttons = pre_block.querySelector(".buttons"); + if (!buttons) { + buttons = document.createElement('div'); + buttons.className = 'buttons'; + pre_block.insertBefore(buttons, pre_block.firstChild); + } + + var runCodeButton = document.createElement('button'); + runCodeButton.className = 'fa fa-play play-button'; + runCodeButton.hidden = true; + runCodeButton.title = 'Run this code'; + runCodeButton.setAttribute('aria-label', runCodeButton.title); + + buttons.insertBefore(runCodeButton, buttons.firstChild); + runCodeButton.addEventListener('click', function (e) { + run_rust_code(pre_block); + }); + + if (window.playground_copyable) { + var copyCodeClipboardButton = document.createElement('button'); + copyCodeClipboardButton.className = 'fa fa-copy clip-button'; + copyCodeClipboardButton.innerHTML = ''; + copyCodeClipboardButton.title = 'Copy to clipboard'; + copyCodeClipboardButton.setAttribute('aria-label', copyCodeClipboardButton.title); + + buttons.insertBefore(copyCodeClipboardButton, buttons.firstChild); + } + + let code_block = pre_block.querySelector("code"); + if (window.ace && code_block.classList.contains("editable")) { + var undoChangesButton = document.createElement('button'); + undoChangesButton.className = 'fa fa-history reset-button'; + undoChangesButton.title = 'Undo changes'; + undoChangesButton.setAttribute('aria-label', undoChangesButton.title); + + buttons.insertBefore(undoChangesButton, buttons.firstChild); + + undoChangesButton.addEventListener('click', function () { + let editor = window.ace.edit(code_block); + editor.setValue(editor.originalCode); + editor.clearSelection(); + }); + } + }); +})(); + +(function themes() { + var html = document.querySelector('html'); + var themeToggleButton = document.getElementById('theme-toggle'); 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+ var nextTop = null; + var scrollDown = scrollTop > prevScrollTop; + var menuPosAbsoluteY = topCache - scrollTop; + if (scrollDown) { + nextSticky = false; + if (menuPosAbsoluteY > 0) { + nextTop = prevScrollTop; + } + } else { + if (menuPosAbsoluteY > 0) { + nextSticky = true; + } else if (menuPosAbsoluteY < minMenuY) { + nextTop = prevScrollTop + minMenuY; + } + } + if (nextSticky === true && stickyCache === false) { + menu.classList.add('sticky'); + stickyCache = true; + } else if (nextSticky === false && stickyCache === true) { + menu.classList.remove('sticky'); + stickyCache = false; + } + if (nextTop !== null) { + menu.style.top = nextTop + 'px'; + topCache = nextTop; + } + prevScrollTop = scrollTop; + }, { passive: true }); + })(); + (function controllBorder() { + menu.classList.remove('bordered'); + document.addEventListener('scroll', function () { + if (menu.offsetTop === 0) { + menu.classList.remove('bordered'); + } else { + menu.classList.add('bordered'); + } + }, { passive: true }); + })(); +})(); diff --git a/clipboard.min.js b/clipboard.min.js new file mode 100644 index 0000000..02c549e --- /dev/null +++ b/clipboard.min.js @@ -0,0 +1,7 @@ +/*! + * clipboard.js v2.0.4 + * https://zenorocha.github.io/clipboard.js + * + * Licensed MIT © Zeno Rocha + */ +!function(t,e){"object"==typeof exports&&"object"==typeof module?module.exports=e():"function"==typeof define&&define.amd?define([],e):"object"==typeof exports?exports.ClipboardJS=e():t.ClipboardJS=e()}(this,function(){return function(n){var o={};function r(t){if(o[t])return o[t].exports;var e=o[t]={i:t,l:!1,exports:{}};return n[t].call(e.exports,e,e.exports,r),e.l=!0,e.exports}return r.m=n,r.c=o,r.d=function(t,e,n){r.o(t,e)||Object.defineProperty(t,e,{enumerable:!0,get:n})},r.r=function(t){"undefined"!=typeof Symbol&&Symbol.toStringTag&&Object.defineProperty(t,Symbol.toStringTag,{value:"Module"}),Object.defineProperty(t,"__esModule",{value:!0})},r.t=function(e,t){if(1&t&&(e=r(e)),8&t)return e;if(4&t&&"object"==typeof e&&e&&e.__esModule)return e;var n=Object.create(null);if(r.r(n),Object.defineProperty(n,"default",{enumerable:!0,value:e}),2&t&&"string"!=typeof e)for(var o in e)r.d(n,o,function(t){return e[t]}.bind(null,o));return n},r.n=function(t){var e=t&&t.__esModule?function(){return t.default}:function(){return t};return r.d(e,"a",e),e},r.o=function(t,e){return Object.prototype.hasOwnProperty.call(t,e)},r.p="",r(r.s=0)}([function(t,e,n){"use strict";var r="function"==typeof Symbol&&"symbol"==typeof Symbol.iterator?function(t){return typeof t}:function(t){return t&&"function"==typeof Symbol&&t.constructor===Symbol&&t!==Symbol.prototype?"symbol":typeof t},i=function(){function o(t,e){for(var n=0;n .hljs { + color: var(--links); +} + +/* Menu Bar */ + +#menu-bar, +#menu-bar-hover-placeholder { + z-index: 101; + margin: auto calc(0px - var(--page-padding)); +} +#menu-bar { + position: relative; + display: flex; + flex-wrap: wrap; + background-color: var(--bg); + border-bottom-color: var(--bg); + border-bottom-width: 1px; + border-bottom-style: solid; +} +#menu-bar.sticky, +.js #menu-bar-hover-placeholder:hover + #menu-bar, +.js #menu-bar:hover, +.js.sidebar-visible #menu-bar { + position: -webkit-sticky; + position: sticky; + top: 0 !important; +} +#menu-bar-hover-placeholder { + position: sticky; + position: -webkit-sticky; + top: 0; + height: var(--menu-bar-height); +} +#menu-bar.bordered { + border-bottom-color: var(--table-border-color); +} +#menu-bar i, #menu-bar .icon-button { + position: relative; + padding: 0 8px; + z-index: 10; + line-height: var(--menu-bar-height); + cursor: pointer; + transition: color 0.5s; +} +@media only screen and (max-width: 420px) { + #menu-bar i, #menu-bar .icon-button { + padding: 0 5px; + } +} + +.icon-button { + border: none; + background: none; + padding: 0; + color: inherit; +} +.icon-button i { + margin: 0; +} + +.right-buttons { + margin: 0 15px; +} +.right-buttons a { + text-decoration: none; +} + +.left-buttons { + display: flex; + margin: 0 5px; +} +.no-js .left-buttons { + display: none; +} + +.menu-title { + display: inline-block; + font-weight: 200; + font-size: 2.4rem; + line-height: var(--menu-bar-height); + text-align: center; + margin: 0; + flex: 1; + white-space: nowrap; + overflow: hidden; + text-overflow: ellipsis; +} +.js .menu-title { + cursor: pointer; +} + +.menu-bar, +.menu-bar:visited, +.nav-chapters, +.nav-chapters:visited, +.mobile-nav-chapters, +.mobile-nav-chapters:visited, +.menu-bar .icon-button, +.menu-bar a i { + color: var(--icons); +} + +.menu-bar i:hover, +.menu-bar .icon-button:hover, +.nav-chapters:hover, +.mobile-nav-chapters i:hover { + color: var(--icons-hover); +} + +/* Nav Icons */ + +.nav-chapters { + font-size: 2.5em; + text-align: center; + text-decoration: none; + + position: fixed; + top: 0; + bottom: 0; + margin: 0; + max-width: 150px; + min-width: 90px; + + display: flex; + justify-content: center; + align-content: center; + flex-direction: column; + + transition: color 0.5s, background-color 0.5s; +} + +.nav-chapters:hover { + text-decoration: none; + background-color: var(--theme-hover); + transition: background-color 0.15s, color 0.15s; +} + +.nav-wrapper { + margin-top: 50px; + display: none; +} + +.mobile-nav-chapters { + font-size: 2.5em; + text-align: center; + text-decoration: none; + width: 90px; + border-radius: 5px; + background-color: var(--sidebar-bg); +} + +.previous { + float: left; +} + +.next { + float: right; + right: var(--page-padding); +} + +@media only screen and (max-width: 1080px) { + .nav-wide-wrapper { display: none; } + .nav-wrapper { display: block; } +} + +@media only screen and (max-width: 1380px) { + .sidebar-visible .nav-wide-wrapper { display: none; } + .sidebar-visible .nav-wrapper { display: block; } +} + +/* Inline code */ + +:not(pre) > .hljs { + display: inline; + padding: 0.1em 0.3em; + border-radius: 3px; +} + +:not(pre):not(a) > .hljs { + color: var(--inline-code-color); + overflow-x: initial; +} + +a:hover > .hljs { + text-decoration: underline; +} + +pre { + position: relative; +} +pre > .buttons { + position: absolute; + z-index: 100; + right: 5px; + top: 5px; + + color: var(--sidebar-fg); + cursor: pointer; +} +pre > .buttons :hover { + color: var(--sidebar-active); +} +pre > .buttons i { + margin-left: 8px; +} +pre > .buttons button { + color: inherit; + background: transparent; + border: none; + cursor: inherit; +} +pre > .result { + margin-top: 10px; +} + +/* Search */ + +#searchresults a { + text-decoration: none; +} + +mark { + border-radius: 2px; + padding: 0 3px 1px 3px; + margin: 0 -3px -1px -3px; + background-color: var(--search-mark-bg); + transition: background-color 300ms linear; + cursor: pointer; +} + +mark.fade-out { + background-color: rgba(0,0,0,0) !important; + cursor: auto; +} + +.searchbar-outer { + margin-left: auto; + margin-right: auto; + max-width: var(--content-max-width); +} + +#searchbar { + width: 100%; + margin: 5px auto 0px auto; + padding: 10px 16px; + transition: box-shadow 300ms ease-in-out; + border: 1px solid var(--searchbar-border-color); + border-radius: 3px; + background-color: var(--searchbar-bg); + color: var(--searchbar-fg); +} +#searchbar:focus, +#searchbar.active { + box-shadow: 0 0 3px var(--searchbar-shadow-color); +} + +.searchresults-header { + font-weight: bold; + font-size: 1em; + padding: 18px 0 0 5px; + color: var(--searchresults-header-fg); +} + +.searchresults-outer { + margin-left: auto; + margin-right: auto; + max-width: var(--content-max-width); + border-bottom: 1px dashed var(--searchresults-border-color); +} + +ul#searchresults { + list-style: none; + padding-left: 20px; +} +ul#searchresults li { + margin: 10px 0px; + padding: 2px; + border-radius: 2px; +} +ul#searchresults li.focus { + background-color: var(--searchresults-li-bg); +} +ul#searchresults span.teaser { + display: block; + clear: both; + margin: 5px 0 0 20px; + font-size: 0.8em; +} +ul#searchresults span.teaser em { + font-weight: bold; + font-style: normal; +} + +/* Sidebar */ + +.sidebar { + position: fixed; + left: 0; + top: 0; + bottom: 0; + width: var(--sidebar-width); + font-size: 0.875em; + box-sizing: border-box; + -webkit-overflow-scrolling: touch; + overscroll-behavior-y: contain; + background-color: var(--sidebar-bg); + color: var(--sidebar-fg); +} +.sidebar-resizing { + -moz-user-select: none; + -webkit-user-select: none; + -ms-user-select: none; + user-select: none; +} +.js:not(.sidebar-resizing) .sidebar { + transition: transform 0.3s; /* Animation: slide away */ +} +.sidebar code { + line-height: 2em; +} +.sidebar .sidebar-scrollbox { + overflow-y: auto; + position: absolute; + top: 0; + bottom: 0; + left: 0; + right: 0; + padding: 10px 10px; +} +.sidebar .sidebar-resize-handle { + position: absolute; + cursor: col-resize; + width: 0; + right: 0; + top: 0; + bottom: 0; +} +.js .sidebar .sidebar-resize-handle { + cursor: col-resize; + width: 5px; +} +.sidebar-hidden .sidebar { + transform: translateX(calc(0px - var(--sidebar-width))); +} +.sidebar::-webkit-scrollbar { + background: var(--sidebar-bg); +} +.sidebar::-webkit-scrollbar-thumb { + background: var(--scrollbar); +} + +.sidebar-visible .page-wrapper { + transform: translateX(var(--sidebar-width)); +} +@media only screen and (min-width: 620px) { + .sidebar-visible .page-wrapper { + transform: none; + margin-left: var(--sidebar-width); + } +} + +.chapter { + list-style: none outside none; + padding-left: 0; + line-height: 2.2em; +} + +.chapter ol { + width: 100%; +} + +.chapter li { + display: flex; + color: var(--sidebar-non-existant); +} +.chapter li a { + display: block; + padding: 0; + text-decoration: none; + color: var(--sidebar-fg); +} + +.chapter li a:hover { + color: var(--sidebar-active); +} + +.chapter li a.active { + color: var(--sidebar-active); +} + +.chapter li > a.toggle { + cursor: pointer; + display: block; + margin-left: auto; + padding: 0 10px; + user-select: none; + opacity: 0.68; +} + +.chapter li > a.toggle div { + transition: transform 0.5s; +} + +/* collapse the section */ +.chapter li:not(.expanded) + li > ol { + display: none; +} + +.chapter li.chapter-item { + line-height: 1.5em; + margin-top: 0.6em; +} + +.chapter li.expanded > a.toggle div { + transform: rotate(90deg); +} + +.spacer { + width: 100%; + height: 3px; + margin: 5px 0px; +} +.chapter .spacer { + background-color: var(--sidebar-spacer); +} + +@media (-moz-touch-enabled: 1), (pointer: coarse) { + .chapter li a { padding: 5px 0; } + .spacer { margin: 10px 0; } +} + +.section { + list-style: none outside none; + padding-left: 20px; + line-height: 1.9em; +} + +/* Theme Menu Popup */ + +.theme-popup { + position: absolute; + left: 10px; + top: var(--menu-bar-height); + z-index: 1000; + border-radius: 4px; + font-size: 0.7em; + color: var(--fg); + background: var(--theme-popup-bg); + border: 1px solid var(--theme-popup-border); + margin: 0; + padding: 0; + list-style: none; + display: none; +} +.theme-popup .default { + color: var(--icons); +} +.theme-popup .theme { + width: 100%; + border: 0; + margin: 0; + padding: 2px 10px; + line-height: 25px; + white-space: nowrap; + text-align: left; + cursor: pointer; + color: inherit; + background: inherit; + font-size: inherit; +} +.theme-popup .theme:hover { + background-color: var(--theme-hover); +} +.theme-popup .theme:hover:first-child, +.theme-popup .theme:hover:last-child { + border-top-left-radius: inherit; + border-top-right-radius: inherit; +} diff --git a/css/general.css b/css/general.css new file mode 100644 index 0000000..ef2ba50 --- /dev/null +++ b/css/general.css @@ -0,0 +1,182 @@ +/* Base styles and content styles */ + +@import 'variables.css'; + +:root { + /* Browser default font-size is 16px, this way 1 rem = 10px */ + font-size: 62.5%; +} + +html { + font-family: "Open Sans", sans-serif; + color: var(--fg); + background-color: var(--bg); + text-size-adjust: none; + -webkit-text-size-adjust: none; +} + +body { + margin: 0; + font-size: 1.6rem; + overflow-x: hidden; +} + +code { + font-family: "Source Code Pro", Consolas, "Ubuntu Mono", Menlo, "DejaVu Sans Mono", monospace, monospace !important; + font-size: 0.875em; /* please adjust the ace font size accordingly in editor.js */ +} + +/* Don't change font size in headers. */ +h1 code, h2 code, h3 code, h4 code, h5 code, h6 code { + font-size: unset; +} + +.left { float: left; } +.right { float: right; } +.boring { opacity: 0.6; } +.hide-boring .boring { display: none; } +.hidden { display: none !important; } + +h2, h3 { margin-top: 2.5em; } +h4, h5 { margin-top: 2em; } + +.header + .header h3, +.header + .header h4, +.header + .header h5 { + margin-top: 1em; +} + +h1:target::before, +h2:target::before, +h3:target::before, +h4:target::before, +h5:target::before, +h6:target::before { + display: inline-block; + content: "»"; + margin-left: -30px; + width: 30px; +} + +/* This is broken on Safari as of version 14, but is fixed + in Safari Technology Preview 117 which I think will be Safari 14.2. + https://bugs.webkit.org/show_bug.cgi?id=218076 +*/ +:target { + scroll-margin-top: calc(var(--menu-bar-height) + 0.5em); +} + +.page { + outline: 0; + padding: 0 var(--page-padding); + margin-top: calc(0px - var(--menu-bar-height)); /* Compensate for the #menu-bar-hover-placeholder */ +} +.page-wrapper { + box-sizing: border-box; +} +.js:not(.sidebar-resizing) .page-wrapper { + transition: margin-left 0.3s ease, transform 0.3s ease; /* Animation: slide away */ +} + +.content { + overflow-y: auto; + padding: 0 15px; + padding-bottom: 50px; +} +.content main { + margin-left: auto; + margin-right: auto; + max-width: var(--content-max-width); +} +.content p { line-height: 1.45em; } +.content ol { line-height: 1.45em; } +.content ul { line-height: 1.45em; } +.content a { text-decoration: none; } +.content a:hover { text-decoration: underline; } +.content img, .content video { max-width: 100%; } +.content .header:link, +.content .header:visited { + color: var(--fg); +} +.content .header:link, +.content .header:visited:hover { + text-decoration: none; +} + +table { + margin: 0 auto; + border-collapse: collapse; +} +table td { + padding: 3px 20px; + border: 1px var(--table-border-color) solid; +} +table thead { + background: var(--table-header-bg); +} +table thead td { + font-weight: 700; + border: none; +} +table thead th { + padding: 3px 20px; +} +table thead tr { + border: 1px var(--table-header-bg) solid; +} +/* Alternate background colors for rows */ +table tbody tr:nth-child(2n) { + background: var(--table-alternate-bg); +} + + +blockquote { + margin: 20px 0; + padding: 0 20px; + color: var(--fg); + background-color: var(--quote-bg); + border-top: .1em solid var(--quote-border); + border-bottom: .1em solid var(--quote-border); +} + + +:not(.footnote-definition) + .footnote-definition, +.footnote-definition + :not(.footnote-definition) { + margin-top: 2em; +} +.footnote-definition { + font-size: 0.9em; + margin: 0.5em 0; +} +.footnote-definition p { + display: inline; +} + +.tooltiptext { + position: absolute; + visibility: hidden; + color: #fff; + background-color: #333; + transform: translateX(-50%); /* Center by moving tooltip 50% of its width left */ + left: -8px; /* Half of the width of the icon */ + top: -35px; + font-size: 0.8em; + text-align: center; + border-radius: 6px; + padding: 5px 8px; + margin: 5px; + z-index: 1000; +} +.tooltipped .tooltiptext { + visibility: visible; +} + +.chapter li.part-title { + color: var(--sidebar-fg); + margin: 5px 0px; + font-weight: bold; +} + +.result-no-output { + font-style: italic; +} diff --git a/css/print.css b/css/print.css new file mode 100644 index 0000000..5e690f7 --- /dev/null +++ b/css/print.css @@ -0,0 +1,54 @@ + +#sidebar, +#menu-bar, +.nav-chapters, +.mobile-nav-chapters { + display: none; +} + +#page-wrapper.page-wrapper { + transform: none; + margin-left: 0px; + overflow-y: initial; +} + +#content { + max-width: none; + margin: 0; + padding: 0; +} + +.page { + overflow-y: initial; +} + +code { + background-color: #666666; + border-radius: 5px; + + /* Force background to be printed in Chrome */ + -webkit-print-color-adjust: exact; +} + +pre > .buttons { + z-index: 2; +} + +a, a:visited, a:active, a:hover { + color: #4183c4; + text-decoration: none; +} + +h1, h2, h3, h4, h5, h6 { + page-break-inside: avoid; + page-break-after: avoid; +} + +pre, code { + page-break-inside: avoid; + white-space: pre-wrap; +} + +.fa { + display: none !important; +} diff --git a/css/variables.css b/css/variables.css new file mode 100644 index 0000000..56b634b --- /dev/null +++ b/css/variables.css @@ -0,0 +1,253 @@ + +/* Globals */ + +:root { + --sidebar-width: 300px; + --page-padding: 15px; + --content-max-width: 750px; + --menu-bar-height: 50px; +} + +/* Themes */ + +.ayu { + --bg: hsl(210, 25%, 8%); + --fg: #c5c5c5; + + --sidebar-bg: #14191f; + --sidebar-fg: #c8c9db; + --sidebar-non-existant: #5c6773; + --sidebar-active: #ffb454; + --sidebar-spacer: #2d334f; + + --scrollbar: var(--sidebar-fg); + + --icons: #737480; + --icons-hover: #b7b9cc; + + --links: #0096cf; + + --inline-code-color: #ffb454; + + --theme-popup-bg: #14191f; + --theme-popup-border: #5c6773; + --theme-hover: #191f26; + + --quote-bg: hsl(226, 15%, 17%); + --quote-border: hsl(226, 15%, 22%); + + --table-border-color: hsl(210, 25%, 13%); + --table-header-bg: hsl(210, 25%, 28%); + --table-alternate-bg: hsl(210, 25%, 11%); + + --searchbar-border-color: #848484; + --searchbar-bg: #424242; + --searchbar-fg: #fff; + --searchbar-shadow-color: #d4c89f; + --searchresults-header-fg: #666; + --searchresults-border-color: #888; + --searchresults-li-bg: #252932; + --search-mark-bg: #e3b171; +} + +.coal { + --bg: hsl(200, 7%, 8%); + --fg: #98a3ad; + + --sidebar-bg: #292c2f; + --sidebar-fg: #a1adb8; + --sidebar-non-existant: #505254; + --sidebar-active: #3473ad; + --sidebar-spacer: #393939; + + --scrollbar: var(--sidebar-fg); + + --icons: #43484d; + --icons-hover: #b3c0cc; + + --links: #2b79a2; + + --inline-code-color: #c5c8c6; + + --theme-popup-bg: #141617; + --theme-popup-border: #43484d; + --theme-hover: #1f2124; + + --quote-bg: hsl(234, 21%, 18%); + --quote-border: hsl(234, 21%, 23%); + + --table-border-color: hsl(200, 7%, 13%); + --table-header-bg: hsl(200, 7%, 28%); + --table-alternate-bg: hsl(200, 7%, 11%); + + --searchbar-border-color: #aaa; + --searchbar-bg: #b7b7b7; + --searchbar-fg: #000; + --searchbar-shadow-color: #aaa; + --searchresults-header-fg: #666; + --searchresults-border-color: #98a3ad; + --searchresults-li-bg: #2b2b2f; + --search-mark-bg: #355c7d; +} + +.light { + --bg: hsl(0, 0%, 100%); + --fg: hsl(0, 0%, 0%); + + --sidebar-bg: #fafafa; + --sidebar-fg: hsl(0, 0%, 0%); + --sidebar-non-existant: #aaaaaa; + --sidebar-active: #1f1fff; + --sidebar-spacer: #f4f4f4; + + --scrollbar: #8F8F8F; + + --icons: #747474; + --icons-hover: #000000; + + --links: #20609f; + + --inline-code-color: #301900; + + --theme-popup-bg: #fafafa; + --theme-popup-border: #cccccc; + --theme-hover: #e6e6e6; + + --quote-bg: hsl(197, 37%, 96%); + --quote-border: hsl(197, 37%, 91%); + + --table-border-color: hsl(0, 0%, 95%); + --table-header-bg: hsl(0, 0%, 80%); + --table-alternate-bg: hsl(0, 0%, 97%); + + --searchbar-border-color: #aaa; + --searchbar-bg: #fafafa; + --searchbar-fg: #000; + --searchbar-shadow-color: #aaa; + --searchresults-header-fg: #666; + --searchresults-border-color: #888; + --searchresults-li-bg: #e4f2fe; + --search-mark-bg: #a2cff5; +} + +.navy { + --bg: hsl(226, 23%, 11%); + --fg: #bcbdd0; + + --sidebar-bg: #282d3f; + --sidebar-fg: #c8c9db; + --sidebar-non-existant: #505274; + --sidebar-active: #2b79a2; + --sidebar-spacer: #2d334f; + + --scrollbar: var(--sidebar-fg); + + --icons: #737480; + --icons-hover: #b7b9cc; + + --links: #2b79a2; + + --inline-code-color: #c5c8c6; + + --theme-popup-bg: #161923; + --theme-popup-border: #737480; + --theme-hover: #282e40; + + --quote-bg: hsl(226, 15%, 17%); + --quote-border: hsl(226, 15%, 22%); + + --table-border-color: hsl(226, 23%, 16%); + --table-header-bg: hsl(226, 23%, 31%); + --table-alternate-bg: hsl(226, 23%, 14%); + + --searchbar-border-color: #aaa; + --searchbar-bg: #aeaec6; + --searchbar-fg: #000; + --searchbar-shadow-color: #aaa; + --searchresults-header-fg: #5f5f71; + --searchresults-border-color: #5c5c68; + --searchresults-li-bg: #242430; + --search-mark-bg: #a2cff5; +} + +.rust { + --bg: hsl(60, 9%, 87%); + --fg: #262625; + + --sidebar-bg: #3b2e2a; + --sidebar-fg: #c8c9db; + --sidebar-non-existant: #505254; + --sidebar-active: #e69f67; + --sidebar-spacer: #45373a; + + --scrollbar: var(--sidebar-fg); + + --icons: #737480; + --icons-hover: #262625; + + --links: #2b79a2; + + --inline-code-color: #6e6b5e; + + --theme-popup-bg: #e1e1db; + --theme-popup-border: #b38f6b; + --theme-hover: #99908a; + + --quote-bg: hsl(60, 5%, 75%); + --quote-border: hsl(60, 5%, 70%); + + --table-border-color: hsl(60, 9%, 82%); + --table-header-bg: #b3a497; + --table-alternate-bg: hsl(60, 9%, 84%); + + --searchbar-border-color: #aaa; + --searchbar-bg: #fafafa; + --searchbar-fg: #000; + --searchbar-shadow-color: #aaa; + --searchresults-header-fg: #666; + --searchresults-border-color: #888; + --searchresults-li-bg: #dec2a2; + --search-mark-bg: #e69f67; +} + +@media (prefers-color-scheme: dark) { + .light.no-js { + --bg: hsl(200, 7%, 8%); + --fg: #98a3ad; + + --sidebar-bg: #292c2f; + --sidebar-fg: #a1adb8; + --sidebar-non-existant: #505254; + --sidebar-active: #3473ad; + --sidebar-spacer: #393939; + + --scrollbar: var(--sidebar-fg); + + --icons: #43484d; + --icons-hover: #b3c0cc; + + --links: #2b79a2; + + --inline-code-color: #c5c8c6; + + --theme-popup-bg: #141617; + --theme-popup-border: #43484d; + --theme-hover: #1f2124; + + --quote-bg: hsl(234, 21%, 18%); + --quote-border: hsl(234, 21%, 23%); + + --table-border-color: hsl(200, 7%, 13%); + --table-header-bg: hsl(200, 7%, 28%); + --table-alternate-bg: hsl(200, 7%, 11%); + + --searchbar-border-color: #aaa; + --searchbar-bg: #b7b7b7; + --searchbar-fg: #000; + --searchbar-shadow-color: #aaa; + --searchresults-header-fg: #666; + --searchresults-border-color: #98a3ad; + --searchresults-li-bg: #2b2b2f; + --search-mark-bg: #355c7d; + } +} diff --git a/dos-example-inline.html b/dos-example-inline.html new file mode 100644 index 0000000..3174796 --- /dev/null +++ b/dos-example-inline.html @@ -0,0 +1,16 @@ +
+ diff --git a/dos-example-pdos-inline.html b/dos-example-pdos-inline.html new file mode 100644 index 0000000..3f5d79c --- /dev/null +++ b/dos-example-pdos-inline.html @@ -0,0 +1,26 @@ +
+ diff --git a/dos-example-pdos-inline2.html b/dos-example-pdos-inline2.html new file mode 100644 index 0000000..d80f614 --- /dev/null +++ b/dos-example-pdos-inline2.html @@ -0,0 +1,26 @@ +
+ diff --git a/dos-example-raw.txt b/dos-example-raw.txt new file mode 100644 index 0000000..6fcf3a9 --- /dev/null +++ b/dos-example-raw.txt @@ -0,0 +1,1201 @@ +# E-Ef TotDOS Benzene AgSurf + -19.808844 0.000000 0.000000 0.000000 + -19.786203 0.000000 0.000000 0.000000 + -19.763561 0.000000 0.000000 0.000000 + -19.740919 0.000000 0.000000 0.000000 + -19.718277 0.000000 0.000000 0.000000 + -19.695636 0.000000 0.000000 0.000000 + -19.672994 0.000000 0.000000 0.000000 + -19.650352 0.000000 0.000000 0.000000 + -19.627711 0.000000 0.000000 0.000000 + -19.605069 0.000000 0.000000 0.000000 + -19.582427 0.000000 0.000000 0.000000 + -19.559785 0.000000 0.000000 0.000000 + -19.537144 0.000000 0.000000 0.000000 + -19.514502 0.000000 0.000000 0.000000 + -19.491860 0.000000 0.000000 0.000000 + -19.469218 0.000000 0.000000 0.000000 + -19.446577 0.000000 0.000000 0.000000 + -19.423935 0.000000 0.000000 0.000000 + -19.401293 0.000000 0.000000 0.000000 + -19.378652 0.000000 0.000000 0.000000 + 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@license + */ +!function(){function e(e){if(null===e||"object"!=typeof e)return e;var t=e.constructor();for(var n in e)e.hasOwnProperty(n)&&(t[n]=e[n]);return t}var t=function(e){var n=new t.Index;return n.pipeline.add(t.trimmer,t.stopWordFilter,t.stemmer),e&&e.call(n,n),n};t.version="0.9.5",lunr=t,t.utils={},t.utils.warn=function(e){return function(t){e.console&&console.warn&&console.warn(t)}}(this),t.utils.toString=function(e){return void 0===e||null===e?"":e.toString()},t.EventEmitter=function(){this.events={}},t.EventEmitter.prototype.addListener=function(){var e=Array.prototype.slice.call(arguments),t=e.pop(),n=e;if("function"!=typeof t)throw new TypeError("last argument must be a function");n.forEach(function(e){this.hasHandler(e)||(this.events[e]=[]),this.events[e].push(t)},this)},t.EventEmitter.prototype.removeListener=function(e,t){if(this.hasHandler(e)){var n=this.events[e].indexOf(t);-1!==n&&(this.events[e].splice(n,1),0==this.events[e].length&&delete 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We also recommend that a + file or class name and description of purpose be included on the + same "printed page" as the copyright notice for easier + identification within third-party archives. + + Copyright [yyyy] [name of copyright owner] + + Licensed under the Apache License, Version 2.0 (the "License"); + you may not use this file except in compliance with the License. + You may obtain a copy of the License at + + http://www.apache.org/licenses/LICENSE-2.0 + + Unless required by applicable law or agreed to in writing, software + distributed under the License is distributed on an "AS IS" BASIS, + WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied. + See the License for the specific language governing permissions and + limitations under the License. diff --git a/fonts/SOURCE-CODE-PRO-LICENSE.txt b/fonts/SOURCE-CODE-PRO-LICENSE.txt new file mode 100644 index 0000000..366206f --- /dev/null +++ b/fonts/SOURCE-CODE-PRO-LICENSE.txt @@ -0,0 +1,93 @@ +Copyright 2010, 2012 Adobe Systems Incorporated (http://www.adobe.com/), with Reserved Font Name 'Source'. All Rights Reserved. Source is a trademark of Adobe Systems Incorporated in the United States and/or other countries. + +This Font Software is licensed under the SIL Open Font License, Version 1.1. +This license is copied below, and is also available with a FAQ at: +http://scripts.sil.org/OFL + + +----------------------------------------------------------- +SIL OPEN FONT LICENSE Version 1.1 - 26 February 2007 +----------------------------------------------------------- + +PREAMBLE +The goals of the Open Font License (OFL) are to stimulate worldwide +development of collaborative font projects, to support the font creation +efforts of academic and linguistic communities, and to provide a free and +open framework in which fonts may be shared and improved in partnership +with others. + +The OFL allows the licensed fonts to be used, studied, modified and +redistributed freely as long as they are not sold by themselves. The +fonts, including any derivative works, can be bundled, embedded, +redistributed and/or sold with any software provided that any reserved +names are not used by derivative works. The fonts and derivatives, +however, cannot be released under any other type of license. The +requirement for fonts to remain under this license does not apply +to any document created using the fonts or their derivatives. + +DEFINITIONS +"Font Software" refers to the set of files released by the Copyright +Holder(s) under this license and clearly marked as such. This may +include source files, build scripts and documentation. + +"Reserved Font Name" refers to any names specified as such after the +copyright statement(s). + +"Original Version" refers to the collection of Font Software components as +distributed by the Copyright Holder(s). + +"Modified Version" refers to any derivative made by adding to, deleting, +or substituting -- in part or in whole -- any of the components of the +Original Version, by changing formats or by porting the Font Software to a +new environment. + +"Author" refers to any designer, engineer, programmer, technical +writer or other person who contributed to the Font Software. + +PERMISSION & CONDITIONS +Permission is hereby granted, free of charge, to any person obtaining +a copy of the Font Software, to use, study, copy, merge, embed, modify, +redistribute, and sell modified and unmodified copies of the Font +Software, subject to the following conditions: + +1) Neither the Font Software nor any of its individual components, +in Original or Modified Versions, may be sold by itself. + +2) Original or Modified Versions of the Font Software may be bundled, +redistributed and/or sold with any software, provided that each copy +contains the above copyright notice and this license. These can be +included either as stand-alone text files, human-readable headers or +in the appropriate machine-readable metadata fields within text or +binary files as long as those fields can be easily viewed by the user. + +3) No Modified Version of the Font Software may use the Reserved Font +Name(s) unless explicit written permission is granted by the corresponding +Copyright Holder. This restriction only applies to the primary font name as +presented to the users. + +4) The name(s) of the Copyright Holder(s) or the Author(s) of the Font +Software shall not be used to promote, endorse or advertise any +Modified Version, except to acknowledge the contribution(s) of the +Copyright Holder(s) and the Author(s) or with their explicit written +permission. + +5) The Font Software, modified or unmodified, in part or in whole, +must be distributed entirely under this license, and must not be +distributed under any other license. The requirement for fonts to +remain under this license does not apply to any document created +using the Font Software. + +TERMINATION +This license becomes null and void if any of the above conditions are +not met. + +DISCLAIMER +THE FONT SOFTWARE IS PROVIDED "AS IS", WITHOUT WARRANTY OF ANY KIND, +EXPRESS OR IMPLIED, INCLUDING BUT NOT LIMITED TO ANY WARRANTIES OF +MERCHANTABILITY, FITNESS FOR A PARTICULAR PURPOSE AND NONINFRINGEMENT +OF COPYRIGHT, PATENT, TRADEMARK, OR OTHER RIGHT. IN NO EVENT SHALL THE +COPYRIGHT HOLDER BE LIABLE FOR ANY CLAIM, DAMAGES OR OTHER LIABILITY, +INCLUDING ANY GENERAL, SPECIAL, INDIRECT, INCIDENTAL, OR CONSEQUENTIAL +DAMAGES, WHETHER IN AN ACTION OF CONTRACT, TORT OR OTHERWISE, ARISING +FROM, OUT OF THE USE OR INABILITY TO USE THE FONT SOFTWARE OR FROM +OTHER DEALINGS IN THE FONT SOFTWARE. diff --git a/fonts/fonts.css b/fonts/fonts.css new file mode 100644 index 0000000..858efa5 --- /dev/null +++ b/fonts/fonts.css @@ -0,0 +1,100 @@ +/* Open Sans is licensed under the Apache License, Version 2.0. See http://www.apache.org/licenses/LICENSE-2.0 */ +/* Source Code Pro is under the Open Font License. See https://scripts.sil.org/cms/scripts/page.php?site_id=nrsi&id=OFL */ + +/* open-sans-300 - latin_vietnamese_latin-ext_greek-ext_greek_cyrillic-ext_cyrillic */ +@font-face { + font-family: 'Open Sans'; + font-style: normal; + font-weight: 300; + src: local('Open Sans Light'), local('OpenSans-Light'), + url('open-sans-v17-all-charsets-300.woff2') format('woff2'); +} + +/* open-sans-300italic - latin_vietnamese_latin-ext_greek-ext_greek_cyrillic-ext_cyrillic */ +@font-face { + font-family: 'Open Sans'; + font-style: italic; + font-weight: 300; + src: local('Open Sans Light Italic'), local('OpenSans-LightItalic'), + url('open-sans-v17-all-charsets-300italic.woff2') format('woff2'); +} + +/* open-sans-regular - latin_vietnamese_latin-ext_greek-ext_greek_cyrillic-ext_cyrillic */ +@font-face { + font-family: 'Open Sans'; + font-style: normal; + font-weight: 400; + src: local('Open Sans Regular'), local('OpenSans-Regular'), + url('open-sans-v17-all-charsets-regular.woff2') format('woff2'); +} + +/* open-sans-italic - latin_vietnamese_latin-ext_greek-ext_greek_cyrillic-ext_cyrillic */ +@font-face { + font-family: 'Open Sans'; + font-style: italic; + font-weight: 400; + src: local('Open Sans Italic'), local('OpenSans-Italic'), + url('open-sans-v17-all-charsets-italic.woff2') format('woff2'); +} + +/* open-sans-600 - latin_vietnamese_latin-ext_greek-ext_greek_cyrillic-ext_cyrillic */ +@font-face { + font-family: 'Open Sans'; + font-style: normal; + font-weight: 600; + src: local('Open Sans SemiBold'), local('OpenSans-SemiBold'), + url('open-sans-v17-all-charsets-600.woff2') format('woff2'); +} + +/* open-sans-600italic - latin_vietnamese_latin-ext_greek-ext_greek_cyrillic-ext_cyrillic */ +@font-face { + font-family: 'Open Sans'; + font-style: italic; + font-weight: 600; + src: local('Open Sans SemiBold Italic'), local('OpenSans-SemiBoldItalic'), + url('open-sans-v17-all-charsets-600italic.woff2') format('woff2'); +} + +/* open-sans-700 - latin_vietnamese_latin-ext_greek-ext_greek_cyrillic-ext_cyrillic */ +@font-face { + font-family: 'Open Sans'; + font-style: normal; + font-weight: 700; + src: local('Open Sans Bold'), local('OpenSans-Bold'), + url('open-sans-v17-all-charsets-700.woff2') format('woff2'); +} + +/* open-sans-700italic - latin_vietnamese_latin-ext_greek-ext_greek_cyrillic-ext_cyrillic */ +@font-face { + font-family: 'Open Sans'; + font-style: italic; + font-weight: 700; + src: local('Open Sans Bold Italic'), local('OpenSans-BoldItalic'), + url('open-sans-v17-all-charsets-700italic.woff2') format('woff2'); +} + +/* open-sans-800 - latin_vietnamese_latin-ext_greek-ext_greek_cyrillic-ext_cyrillic */ +@font-face { + font-family: 'Open Sans'; + font-style: normal; + font-weight: 800; + src: local('Open Sans ExtraBold'), local('OpenSans-ExtraBold'), + url('open-sans-v17-all-charsets-800.woff2') format('woff2'); +} + +/* open-sans-800italic - latin_vietnamese_latin-ext_greek-ext_greek_cyrillic-ext_cyrillic */ +@font-face { + font-family: 'Open Sans'; + font-style: italic; + font-weight: 800; + src: local('Open Sans ExtraBold Italic'), local('OpenSans-ExtraBoldItalic'), + url('open-sans-v17-all-charsets-800italic.woff2') format('woff2'); +} + +/* source-code-pro-500 - latin_vietnamese_latin-ext_greek_cyrillic-ext_cyrillic */ +@font-face { + font-family: 'Source Code Pro'; + font-style: normal; + font-weight: 500; + src: url('source-code-pro-v11-all-charsets-500.woff2') format('woff2'); +} diff --git a/fonts/open-sans-v17-all-charsets-300.woff2 b/fonts/open-sans-v17-all-charsets-300.woff2 new file mode 100644 index 0000000000000000000000000000000000000000..9f51be370fa913ce6de2922b580c262c4822b337 GIT binary patch literal 44352 zcmV(;K-<4}Pew8T0RR910Ifg(5dZ)H0f7hr0Ib{q0RR9100000000000000000000 z0000QE*lUWfmQ}!0EY+&fhq})G!YOAg!yQMtSAeP3IG8%0we>R0t6rhgFFYi4Ge-h zTM$x_K;*{m=TyO<(oF`$dr#+gT@uRz<@OP72f1way{Ld4djxa`IG0*=K;{4c|Nq>i zF~-^s+Z{rPn$}0zLzV=G*ddk#MfRZCOSo7Svxg)@O1QTM(GtC{-8am>TkfXJ&}5JO 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    + +
    + +
    + + + + + + + +
    +
    +

    Introduction

    +

    rsgrad is an open-source command-line tool to help VASP players play better with VASP.
    +rsgrad is written proudly in pure Rust.

    +

    Now rsgrad provides several features:

    +
      +
    1. Track the relaxation and MD (molecular dynamics) progress;
    2. +
    3. Calculate and visualize the DOS (density of states) and pDOS (projected DOS);
    4. +
    5. Plot and visualize the band structure and fat band structure;
    6. +
    7. Save the frames with given MD or relaxation trajectory;
    8. +
    9. Calculate charge density difference;
    10. +
    11. Analyze the vibration eigen values and eigen vectors;
    12. +
    13. Plot the wave function at given bands in real-space;
    14. +
    15. Plot the wave function at given bands in real-space then integrate it over specified plane;
    16. +
    17. Plot and visualize the work function;
    18. +
    19. Split POSCAR;
      +Convert between fractional coordinates and Cartesian coordinates;
      +Format POSCAR;
    20. +
    21. Generate POTCAR according to POSCAR;
    22. +
    23. Calculate Transition Dipole Moment from WAVECAR;
    24. +
    25. Calculate band gap and print locations of CBM and VBM.
    26. +
    27. Convert one quantity to other units that representing same energy.
    28. +
    +

    Wish you have a good time with rsgrad ^_^

    + +
    + + +
    +
    + + + +
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    + +
    + + + + + + + +
    +
    +

    Introduction

    +

    rsgrad is an open-source command-line tool to help VASP players play better with VASP.
    +rsgrad is written proudly in pure Rust.

    +

    Now rsgrad provides several features:

    +
      +
    1. Track the relaxation and MD (molecular dynamics) progress;
    2. +
    3. Calculate and visualize the DOS (density of states) and pDOS (projected DOS);
    4. +
    5. Plot and visualize the band structure and fat band structure;
    6. +
    7. Save the frames with given MD or relaxation trajectory;
    8. +
    9. Calculate charge density difference;
    10. +
    11. Analyze the vibration eigen values and eigen vectors;
    12. +
    13. Plot the wave function at given bands in real-space;
    14. +
    15. Plot the wave function at given bands in real-space then integrate it over specified plane;
    16. +
    17. Plot and visualize the work function;
    18. +
    19. Split POSCAR;
      +Convert between fractional coordinates and Cartesian coordinates;
      +Format POSCAR;
    20. +
    21. Generate POTCAR according to POSCAR;
    22. +
    23. Calculate Transition Dipole Moment from WAVECAR;
    24. +
    25. Calculate band gap and print locations of CBM and VBM.
    26. +
    27. Convert one quantity to other units that representing same energy.
    28. +
    +

    Wish you have a good time with rsgrad ^_^

    +

    Installation

    +

    There are two ways to install rsgrad, downloading the pre-built binaries and building from scratch.

    +

    Download the Binary from GitHub Release

    +

    We provide the pre-built binaries at GitHub Release.

    +

    There are four platforms we support with pre-built binaries

    +
      +
    • +

      rsgrad-<VERSION>-linux-x86_64-musl.tar.gz: Statically linked binary. Can run on almost all Linux distros. +However, the musl libc may have performance issues in some scenes like wave1d, wav3d etc.

      +
    • +
    • +

      rsgrad-<VERSION>-linux-x86_64.tar.gz: Dynamically linked against glibc and other fundamental +system libraries.
      +For the binaries with 0.3.6_ci-test or upper version, they can run on most Linux distros +(e.g. CentOS 7, Ubuntu 18.04).
      +If it still complains with message like /lib64/libc.so.6: version 'GLIBC_2.18' not found, just switch to -musl +binary or build from scratch.

      +
    • +
    • +

      rsgrad-<VERSION>-macos-x86_64.tar.gz: Binary for macOS (Intel). rsgrad is developed on macOS 13, which +means you are don't need to worry about the availability if you are using macOS.

      +
    • +
    • +

      rsgrad-<VERSION>-macos-aarch64.tar.gz: Binary for macOS (Apple Silicon).

      +
    • +
    • +

      rsgrad-<VERSION>-windows-x86_64.zip: Binary for Windows system. We have no plan to support 32-bit systems.

      +
    • +
    +

    Download the corresponding binary and put it in $PATH (or %PATH% on Windows), and have fun!

    +

    Build from Scratch

    +

    The build requires Internet accessibility.

    +
      +
    • +

      If you haven't installed Rust toolchain, run curl --proto '=https' --tlsv1.2 -sSf https://sh.rustup.rs | sh +and follow the instructions to configure it. When you finished the toolchain installation, you should be able to +run cargo in command-line. Detailed instructions can be found here.

      +
    • +
    • +

      If you have installed Rust toolchain already, just run cargo install --git https://github.com/Ionizing/rsgrad. +Several minutes later, the rsgrad should be installed to ~/.cargo/bin, no need to modify the $PATH (or %PATH% on Windows).

      +
    • +
    +

    Relaxation

    +

    To track the relaxation or MD process, use rsgrad rlx. This command is useful if you want to know the progress +of geometry optimization (aka relaxation) or molecular dynamics.

    +

    This commands extract the following tags from OUTCAR:

    +
      +
    • TOTEN
    • +
    • TOTEN without entropy
    • +
    • TOTEN difference between two ionic steps
    • +
    • Maximum of atom forces (The negative EDIFFG is the threshold of this tag)
    • +
    • The index of the atom with the maximum of force
    • +
    • Number of SCF steps of each ionic step
    • +
    • Time usage of each ionic step
    • +
    • Volume of the cell
    • +
    • Total magnetic moment
    • +
    +

    Help Message

    +
    $ rsgrad rlx -h
    +rsgrad-rlx
    +Tracking relaxation or MD progress
    +
    +USAGE:
    +    rsgrad rlx [OPTIONS] [OUTCAR]
    +
    +ARGS:
    +    <OUTCAR>    Specify the input OUTCAR file [default: ./OUTCAR]
    +
    +OPTIONS:
    +    -a, --favg               Prints averaged total force in eV/A
    +    -e, --toten              Prints TOTEN in eV
    +    -h, --help               Print help information
    +    -i, --fmidx              Prints the index of ion with maximum total force load. Starts from 1
    +        --no-fmax            Don't print maximum total force in A^3
    +        --no-lgde            Don't print Log10(delta(TOTEN without entropy))
    +        --no-magmom          Don't print total magnetic moment in muB
    +        --no-nscf            Don't print number of SCF iteration for each ionic step
    +        --no-time            Don't print time elapsed for each ionic step in minutes
    +        --no-totenz          Don't print TOTEN without entropy in eV
    +    -p, --poscar <POSCAR>    Specify the input POSCAR file [default: ./POSCAR]
    +    -v, --volume             Prints lattice volume in A^3
    +    -x, --fmaxis             Prints the axis where the strongest total force component lies on.
    +                             [XYZ]
    +
    +

    Example

    +

    +

    Density of States

    +

    The rsgrad dos command calculates the Density of States (DOS) of current system.

    +
    + +

    rsgrad DOES NOT read the DOSCAR, but calculates the DOS from PROCAR instead by

    +

    $$ +D(E) = \frac{1}{V} \sum_{i=1}^{N} \delta(E-E(\mathbf{k}_i)) +$$

    +

    Because rsgrad uses arbitrary unit, the factor \(\frac{1}{V}\) is omitted. The \(\delta(x)\) +is replaced by Gaussian function or Lorentzian function:

    +

    $$ +g(x) = \frac{1}{\sigma\sqrt{2\pi}} \exp \left( -\frac{1}{2} \frac{(x-\mu)^2}{\sigma^2} \right) \\ +l(x) = \frac{1}{\pi} \frac{\sigma}{(x-\mu)^2 + \sigma^2} +$$

    +

    where \(\mu\) is \(E(\mathbf{k}_i)\) and \(\sigma\) is sigma of configuration in the implementation.

    +

    This method makes it easier to calculate projected DOS with projection of specific atoms, angular moments and k-points. +However, this method sometimes differs from DOSCAR with ISMEAR = -5. For detailed explaination, see the +document here.

    +

    The OUTCAR is also needed to get the Fermi level.

    +

    Help Message

    +
    $ rsgrad dos -h
    +rsgrad-dos
    +Calculate density of states from PROCAR and OUTCAR
    +
    +USAGE:
    +    rsgrad dos [OPTIONS]
    +
    +OPTIONS:
    +    -c, --config <CONFIG>       Projected DOS configuration file path
    +        --gen-template          Generate projected DOS configuration template
    +    -h, --help                  Print help information
    +        --htmlout <HTMLOUT>     Save the projected DOS plot as HTML. Then you can view it in the
    +                                browser [default: dos.html]
    +        --outcar <OUTCAR>       OUTCAR path [default: ./OUTCAR]
    +        --procar <PROCAR>       PROCAR path [default: ./PROCAR]
    +        --show                  Open the browser and show the plot immediately
    +        --show-brief            Print brief info of PROCAR, this may be helpful when you write the
    +                                configuration
    +        --to-inline-html        Render the plot and print the rendered code to stdout
    +        --txtout <TXTOUT>       Save the raw data of projected DOS. Then you can replot it with more
    +                                advanced tools [default: dos_raw.txt]
    +        --xlim <XLIM> <XLIM>    Set the x-range of the plot [default: -1 6]
    +
    +

    Configuration Template

    +

    The configuration template can be generated by running rsgrad dos --gen-template. The following configuration +is written to pband.toml by default:

    +
    # rsgrad DOS configuration in toml format.
    +# multiple tokens inside string are seperated by whitespace
    +method      = "Gaussian"        # smearing method
    +sigma       = 0.05              # smearing width, (eV)
    +procar      = "PROCAR"          # PROCAR path
    +outcar      = "OUTCAR"          # OUTCAR path
    +txtout      = "dos_raw.txt"     # save the raw data as "dos_raw.txt"
    +htmlout     = "dos.html"        # save the pdos plot as "dos.html"
    +totdos      = true              # plot the total dos
    +fill        = true              # fill the plot to x axis or not
    +xlim        = [-1, 6]           # x-range of plot
    +
    +[pdos.plot1]                  # One label produces one plot, the labels CANNOT be repetitive.
    +                              # This label is 'plot1', to add more pdos, write '[pdos.plot2]' and so on.
    +kpoints = "1 3..7 -1"         # selects 1 3 4 5 6 7 and the last kpoint for pdos plot.
    +atoms   = "1 3..7 -1"         # selects 1 3 4 5 6 7 and the last atoms' projection for pdos plot.
    +orbits  = "s px dxy"          # selects the s px and dx orbits' projection for pdos plot.
    +factor  = 1.01                # the factor multiplied to this pdos
    +
    +[pdos.plot2]                  # One label produces one plot, the labels CANNOT be repetitive.
    +                              # This label is 'plot2', to add more pdos, write '[pdos.plot2]' and so on.
    +kpoints = "1 3..7 -1"         # selects 1 3 4 5 6 7 and the last kpoint for pdos plot.
    +atoms   = "1 3..7 -1"         # selects 1 3 4 5 6 7 and the last atoms' projection for pdos plot.
    +orbits  = "s px dxy"          # selects the s px and dx orbits' projection for pdos plot.
    +factor  = 1.01                # the factor multiplied to this pdos
    +
    +# The fields can be left blank, if you want select all the components for some fields,
    +# just comment them. You can comment fields with '#'
    +
    + +

    Example (without configuration file)

    +

    This command can calculate total DOS only. To calculate projected DOS, +use configuration instead (see next section).

    +
    $ rsgrad dos
    +[2022-07-14T18:42:55Z INFO  rsgrad::commands::dos] Parsing PROCAR file "./PROCAR"
    +[2022-07-14T18:42:55Z INFO  rsgrad::commands::dos] Parsing OUTCAR file "./OUTCAR" for Fermi level
    +[2022-07-14T18:42:55Z INFO  rsgrad::commands::dos] Found Fermi level = -1.9018, eigenvalues will be shifted.
    +[2022-07-14T18:42:55Z INFO  rsgrad::commands::dos] Plotting Total DOS ...
    +[2022-07-14T18:42:55Z INFO  rsgrad::commands::dos] Total DOS plot time usage: 29.055µs
    +[2022-07-14T18:42:55Z INFO  rsgrad::commands::dos] Writing DOS plot to "dos.html"
    +[2022-07-14T18:42:55Z INFO  rsgrad::commands::dos] Writing raw DOS data to "dos_raw.txt"
    +[2022-07-14T18:42:55Z INFO  rsgrad] Time used: 124.426652ms
    +
    +

    The output html should be like something in the following

    +
    + +

    Example (with configuration file)

    +

    To plot multiple PDOS, using configuration file is suggested.

    +

    With the configuration (pdos.toml) in the following

    +
    method      = "Gaussian"
    +sigma       = 0.05
    +procar      = "PROCAR"
    +outcar      = "OUTCAR"
    +txtout      = "dos_raw.txt"
    +htmlout     = "dos.html"
    +totdos      = true
    +fill        = true
    +xlim        = [-1, 6]
    +
    +[pdos.Benzene]
    +atoms   = "37..48"
    +
    +[pdos.AgSurf]
    +atoms   = "3 6 10 14 21 23 25 33 36"
    +
    +

    then rsgrad dos -c pdos.toml

    +
    $ rsgrad dos -c pdos.toml
    +[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Reading PDOS configuration from Some("pdos.toml")
    +[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Parsing PROCAR file "PROCAR"
    +[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Parsing OUTCAR file "OUTCAR" for Fermi level
    +[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Found Fermi level = -1.9018, eigenvalues will be shifted.
    +[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Plotting Total DOS ...
    +[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Total DOS plot time usage: 42.878µs
    +[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Plotting PDOS ...
    +[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] PDOS plot time usage: 6.223076ms
    +[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Writing DOS plot to "dos.html"
    +[2022-07-14T18:43:34Z INFO  rsgrad::commands::dos] Writing raw DOS data to "dos_raw.txt"
    +[2022-07-14T18:43:34Z INFO  rsgrad] Time used: 61.982958ms
    +
    +

    you will get something in the following

    +
    + +

    Usage of txtout

    +

    rsgrad can write the raw data of plot by setting txtout (dos_raw.txt by default). The organization of it +shows the energy, total DOS and projected dos respectively:

    +
    # E-Ef TotDOS Benzene AgSurf
    +...
    +        -7.921938         0.002969         0.002158         0.000004
    +        -7.899296         0.016032         0.011655         0.000019
    +        -7.876654         0.070713         0.051408         0.000085
    +        -7.854012         0.254749         0.185212         0.000307
    +        -7.831371         0.749573         0.544998         0.000910
    +        -7.808729         1.801235         1.309709         0.002202
    +        -7.786087         3.534640         2.570233         0.004349
    +        -7.763446         5.663677         4.118580         0.007011
    +        -7.740804         7.409459         5.388357         0.009226
    +        -7.718162         7.913407         5.755104         0.009908
    +        -7.695520         6.898991         5.017578         0.008683
    +        -7.672879         4.909619         3.570876         0.006208
    +        -7.650237         2.854880         2.076535         0.003622
    +        -7.627595         1.373037         0.998928         0.001724
    +        -7.604953         0.617183         0.449840         0.000672
    +        -7.582312         0.494734         0.362904         0.000231
    +        -7.559670         0.977346         0.718873         0.000173
    +        -7.537028         2.169137         1.593003         0.000599
    +        -7.514387         4.077126         2.981347         0.002383
    +        -7.491745         6.295459         4.560748         0.007858
    +        -7.469103         8.005154         5.685401         0.021128
    +...
    +
    +

    The first line shows the labels of each series and have a hastag # in the beginning in order to let numpy.loadtxt +can read it directly.

    +

    Then you can throw it into other plotters like Excel, Matplotlib, OriginPro GnuPlot etc. and do whatever fancy things you prefer.

    +

    Band Structure

    +

    rsgrad band can plot the band structure from PROCAR and OUTCAR.

    +
    + +

    Help Message

    +
    $ rsgrad band -h
    +rsgrad-band
    +Plot bandstructure and projected bandstructure
    +
    +USAGE:
    +    rsgrad band [OPTIONS]
    +
    +OPTIONS:
    +    -c, --config <CONFIG>
    +            Band structure plot configuration file path
    +
    +        --colormap <COLORMAP>
    +            [default: jet]
    +
    +        --efermi <EFERMI>
    +            Set the E-fermi given from SCF's OUTCAR and it will be the reference energy level
    +
    +        --gen-template
    +            Generate band structure plot configuration template
    +
    +    -h, --help
    +            Print help information
    +
    +        --htmlout <HTMLOUT>
    +            Save the band structure plot as HTML [default: band.html]
    +
    +    -k, --kpoint-labels <KPOINT_LABELS>
    +            Symbols for high symmetry points on the kpoint path
    +
    +        --ncl-spinor <NCL_SPINOR>
    +            [possible values: X, Y, Z]
    +
    +        --outcar <OUTCAR>
    +            OUTCAR path [default: ./OUTCAR]
    +
    +        --procar <PROCAR>
    +            PROCAR path [default: ./PROCAR]
    +
    +        --show
    +            Open the browser and show the plot immediately
    +
    +        --to-inline-html
    +            Render the plot and print the rendered code to stdout
    +
    +        --txtout-prefix <TXTOUT_PREFIX>
    +            Save the raw data of band structure [default: band_raw]
    +
    +        --ylim <YLIM> <YLIM>
    +            Set the y-range of the plot [default: "-1 6"]
    +
    +

    Configuration Template

    +
    # rsgrad Band plot configuration in toml format.
    +# multiple tokens inside string are seperated by whitespace, if you 
    +
    +# kpoint-labels   = ["G", "K", "M", "G"]   # should be consistant with the boundaries in KPOINTS
    +procar          = "PROCAR"
    +outcar          = "OUTCAR"
    +txtout-prefix   = "band_raw"
    +htmlout         = "band.html"
    +# segment-ranges  = [[1, 40], [41, 80], [81, 120]]  # if commented, rsgrad will find the boundaries by judging if k[i] == k[i+1]
    +# ncl-spinor      = "Z"     # for vasp_ncl calculation
    +# colormap        = "jet"     # the colormap specified to plot ncl-band
    +# efermi          = 0.0       # if commented, rsgrad will read the efermi from OUTCAR, but if may be slightly different from scf's
    +# ylim            = [-1, 6]
    +
    +# [pband.plot1]
    +# spins   = "up down"     # "u d" are also ok, for ncl system, "tot x y z" are available
    +# atoms   = "1 3..7 -1"   # which atoms to project on, if commented, all atoms are selected
    +# orbits  = "s px dxy"    # which orbits to project on, if commented, all orbits are selected
    +# color   = "red"         # the color of marker
    +
    +

    Example (without configuration file)

    +

    Simply run rsgrad band can plot the band structure.

    +
    $ rsgrad band
    +[2022-07-14T18:40:18Z INFO  rsgrad::commands::band] Reading fermi level and lattice data from "./OUTCAR"
    +[2022-07-14T18:40:18Z INFO  rsgrad::commands::band] Reading band data from "./PROCAR"
    +[2022-07-14T18:40:18Z INFO  rsgrad::commands::band] Found Fermi level: 12.7626, shifting eigenvalues ...
    +[2022-07-14T18:40:18Z WARN  rsgrad::commands::band] No k-point labels found, use empty labels instead
    +[2022-07-14T18:40:18Z INFO  rsgrad::commands::band] Plotting raw bands ...
    +[2022-07-14T18:40:18Z INFO  rsgrad::commands::band] Writing Bandstructure to "band.html"
    +[2022-07-14T18:40:18Z INFO  rsgrad::commands::band] Writing raw band data to "band_raw.txt"
    +[2022-07-14T18:40:18Z INFO  rsgrad] Time used: 79.644034ms
    +
    +

    There may be a warning reminds you provide the labels of each high-symmetry point.
    +rsgrad identifies high-symmetry points by calculate the difference of consecutive k-points. +If the difference equals zero, these two points are labelled as one high-symmetry point.

    +

    For example:

    +
    ...
    +k-point    38 :       0.0000    0.0256    0.0000
    +k-point    39 :       0.0000    0.0128    0.0000
    +k-point    40 :       0.0000    0.0000    0.0000
    +k-point    41 :       0.0000    0.0000    0.0000
    +k-point    42 :      -0.0085    0.0171    0.0000
    +k-point    43 :      -0.0171    0.0342    0.0000
    +...
    +
    +

    k-point 40 and k-point 41 are same, thus be identified as one high-symmetry point. Each of the high-symmetry +points need a label. You may either left the --kpoint-labels empty or provide the correct labels seperated +by white spaces. Sometimes it may produce wrong band structure due to the special k-point path like

    +
    kpoints for bandstructure L-G-X-U K-G
    + 10
    +line
    +reciprocal
    +  0.50000  0.50000  0.50000    1
    +  0.00000  0.00000  0.00000    1
    +
    +  0.00000  0.00000  0.00000    1
    +  0.00000  0.50000  0.50000    1
    +
    +  0.00000  0.50000  0.50000    1
    +  0.25000  0.62500  0.62500    1
    +
    +  0.37500  0.7500   0.37500    1
    +  0.00000  0.00000  0.00000    1
    +
    +

    The end of third segment (0.25000, 0.62500, 0.62500) and the beginning of fourth segment (0.37500, 0.7500, 0.37500) +are not consistent, which produces wrong k-path, leading to wrong band structure:

    +
    + +

    To solve this issue, you need to try the configuration file.

    +

    Example (with configuration file)

    +

    With the configuration in the following

    +
    kpoint-labels   = ["L", "Γ", "X", "U|K", "Γ"]
    +procar          = "PROCAR"
    +outcar          = "OUTCAR"
    +txtout-prefix   = "pband_raw"
    +htmlout         = "pband.html"
    +segment-ranges  = [[1, 10], [11, 20], [21, 30], [31, 40]]
    +
    +[pband.Si-p-orbit]
    +orbits  = "px py pz"
    +color   = "red"
    +
    +

    and run rsgrad -c pband.toml

    +
    $ rsgrad band -c pband.toml
    +[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Reading porjected band configuration fomr Some("pband.toml")
    +[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Reading fermi level and lattice data from "OUTCAR"
    +[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Reading band data from "PROCAR"
    +[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Found Fermi level: 12.7626, shifting eigenvalues ...
    +[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Plotting raw bands ...
    +[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Plotting projected bands ...
    +[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Writting projected band Si-p-orbit to "pband_raw_Si-p-orbit.txt" ...
    +[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Projected band plot time usage: 1.220401ms
    +[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Writing Bandstructure to "band.html"
    +[2022-07-14T18:41:02Z INFO  rsgrad::commands::band] Writing raw band data to "pband_raw.txt"
    +[2022-07-14T18:41:02Z INFO  rsgrad] Time used: 77.804627ms
    +
    +

    then it produces

    +
    + +

    Example (for non-collinear system)

    +

    For the results produced by vasp_ncl, rsgrad supports plotting the \(z\) (\(x\) and \(y\) are also OK) projection to +analyze the spin angular moments.

    +
    kpoint-labels   = ["M", "Γ", "K", "M"]
    +procar          = "PROCAR"
    +outcar          = "OUTCAR"
    +txtout-prefix   = "band_ncl_raw"
    +htmlout         = "band_ncl.html"
    +segment-ranges  = [[81, 120], [1, 40], [41, 80]]
    +ncl-spinor      = "Z"
    +colormap        = "jet"
    +
    +

    then it produces

    +
    + +

    Trajectory

    +

    rsgrad reads OUTCAR then provide some operations in the following.

    +
      +
    • Save selected steps as XDATCAR.
    • +
    • Save selected steps as POSCAR files.
    • +
    • Save selected steps as XSF files. With XSF, VESTA can show the force vectors on every atom.
    • +
    +

    Help Message

    +
    $ rsgrad traj --help
    +rsgrad-traj
    +Operations about relaxation/MD trajectory.
    +
    +POSCAR is needed if you want to preserve the constraints when saving frames to POSCAR.
    +
    +USAGE:
    +    rsgrad traj [OPTIONS] [--] [OUTCAR]
    +
    +ARGS:
    +    <OUTCAR>
    +            Specify the input OUTCAR file
    +
    +            [default: ./OUTCAR]
    +
    +OPTIONS:
    +        --cartesian
    +            Save to POSCAR in cartesian coordinates, the coordinates written is direct/fractional by
    +            default
    +
    +    -d, --save-as-xdatcar
    +            Save whole trajectory in XDATCAR format
    +
    +    -h, --help
    +            Print help information
    +
    +    -i, --select-indices <SELECT_INDICES>...
    +            Selects the indices to operate.
    +
    +            Step indices start from '1', if '0' is given, all the structures will be selected. Step
    +            indices can be negative, where negative index means counting reversely. E.g.
    +            "-i -2 -1 1 2 3" means selecting the last two and first three steps.
    +
    +        --no-add-symbol-tags
    +            Don't add chemical symbol to each line of coordinates
    +
    +        --no-preserve-constraints
    +            Don't preverse constraints when saving trajectory to POSCAR
    +
    +    -p, --poscar <POSCAR>
    +            Specify the input POSCAR file
    +
    +            [default: ./POSCAR]
    +
    +    -s, --save-as-poscar
    +            Save selected steps as POSCARs
    +
    +        --save-in <SAVE_IN>
    +            Define where the files would be saved
    +
    +            [default: .]
    +
    +    -x, --save-as-xsfs
    +            Saves each selected modes to XSF file, this file includes each atom's force information
    +
    +

    Examples

    +
      +
    • Take the last step and save as XSF file
      +rsgrad traj -i -1 -x
    • +
    +
    $ rsgrad traj -i -1 -x
    +[2022-07-14T18:37:35Z INFO  rsgrad::commands::traj] Parsing file "./OUTCAR" and "./POSCAR"
    +[2022-07-14T18:37:35Z INFO  rsgrad::vasp_parsers::outcar] Saving ionic step to "./step_0003.xsf" ...
    +[2022-07-14T18:37:35Z INFO  rsgrad] Time used: 11.223561ms
    +
    +

    +
      +
    • Take the first step and save as POSCAR file
      +rsgrad traj -i 1 -s
    • +
    +
    $ rsgrad traj -i 1 -s
    +[2022-07-14T18:38:51Z INFO  rsgrad::commands::traj] Parsing file "./OUTCAR" and "./POSCAR"
    +[2022-07-14T18:38:51Z INFO  rsgrad::vasp_parsers::outcar] Saving trajectory step #    1 to "./POSCAR_00001.vasp" ...
    +[2022-07-14T18:38:51Z INFO  rsgrad] Time used: 8.64197ms
    +
    +

    Charge Density Difference

    +

    rsgrad chgdiff can calculate the charge density difference from CHGCAR files:

    +

    $$ +\Delta \rho = \rho_{A+B} - (\rho_A + \rho_B) +$$

    +

    Where \(\rho_{A+B}\), \(\rho_A\) and \(\rho_B\) are the charge densities of total structure, +A structure and B structure, respectively.

    +

    You may also need rsgrad poscar --split ... to generate +the structure of A and B from A+B.

    +

    Help message

    +
    $ rsgrad chgdiff --help
    +rsgrad-chgdiff
    +Calculate charge density difference.
    +
    +The operation is performed by `chgdiff = chgcar_ab - (chgcar_a + chgcar_b)`.
    +
    +USAGE:
    +    rsgrad chgdiff [OPTIONS] <CHGCAR_AB> <CHGCAR_A> <CHGCAR_B>
    +
    +ARGS:
    +    <CHGCAR_AB>
    +            The CHGCAR of A+B system
    +
    +    <CHGCAR_A>
    +            The CHGCAR of A system
    +
    +    <CHGCAR_B>
    +            The CHGCAR of B system
    +
    +OPTIONS:
    +    -h, --help
    +            Print help information
    +
    +    -o, --output <OUTPUT>
    +            The output charge density difference file path
    +
    +            [default: CHGDIFF.vasp]
    +
    +

    Example

    +

    You need to calculate the electronic structure of the three structures (A+B, A and B) first, +then rsgrad chgdiff CHGCAR_A+B CHGCAR_A CHGCAR_B like

    +
    $ rsgrad chgdiff ../scf/CHGCAR Ag/CHGCAR noAg/CHGCAR
    +[2022-07-14T18:34:59Z INFO  rsgrad::commands::chgdiff] Reading charge density from "Ag/CHGCAR"
    +[2022-07-14T18:34:59Z INFO  rsgrad::commands::chgdiff] Reading charge density from "noAg/CHGCAR"
    +[2022-07-14T18:34:59Z INFO  rsgrad::commands::chgdiff] Reading charge density from "../scf/CHGCAR"
    +[2022-07-14T18:35:06Z INFO  rsgrad::commands::chgdiff] Calculating charge density difference by `CHGDIFF = "../scf/CHGCAR" - ("Ag/CHGCAR" + "noAg/CHGCAR")`
    +[2022-07-14T18:35:06Z INFO  rsgrad::commands::chgdiff] Writing charge difference to "CHGDIFF.vasp"
    +[2022-07-14T18:35:10Z INFO  rsgrad] Time used: 11.189259653s
    +
    +

    finally use VESTA to visualize the data

    +

    +

    Vibration

    +

    For systems enabled vibration calculation (phonon at Γ point only), rsgrad vib can

    +
      +
    • Print the phonon eigenvalues;
    • +
    • Save the phonon eigenvectors;
    • +
    • Modulate the ground-state according to specified modes.
    • +
    +

    Help Message

    +
    $ rsgrad vib --help
    +rsgrad-vib
    +Tracking vibration information.
    +
    +For systems enabled vibration mode calculation, this command can extract phonon eigenvalues and
    +phonon eigenvectors at Gamma point.
    +
    +USAGE:
    +    rsgrad vib [OPTIONS] [--] [OUTCAR]
    +
    +ARGS:
    +    <OUTCAR>
    +            Specify the input OUTCAR file
    +
    +            [default: ./OUTCAR]
    +
    +OPTIONS:
    +    -a, --amplitude <AMPLITUDE>
    +            Modulation amplitude coefficient, to avoid precision issue, abs(amplitude) >= 0.01
    +            should be satisfied
    +
    +            [default: 0.1]
    +
    +    -c, --cartesian
    +            Catesian coordinate is used when writting POSCAR. Fractional coordinate is used by
    +            default
    +
    +    -h, --help
    +            Print help information
    +
    +    -i, --select-indices <SELECT_INDICES>...
    +            Selects the mode indices to operate.
    +
    +            Step indices start from '1', if '0' is given, all the structures will be selected. Step
    +            indices can be negative, where negative index means counting reversely. E.g. "-i -2 -1 1
    +            2 3" means selecting the last two and first three steps.
    +
    +    -l, --list
    +            Shows vibration modes in brief
    +
    +    -m, --modulate
    +            Modulate the ground-state POSCAR with respect to a certern vibration frequencies
    +
    +    -p, --poscar <POSCAR>
    +            Specify the input POSCAR file, the consntraints info is needed
    +
    +            [default: ./POSCAR]
    +
    +        --save-in <SAVE_IN>
    +            Define where the files would be saved
    +
    +            [default: .]
    +
    +    -x, --save-as-xsfs
    +            Saves each selected modes to XSF file
    +
    +

    Example

    +
      +
    • +

      Print the phonon eigenvalues; +

      +
    • +
    • +

      Save the phonon eigenvectors;

      +
    • +
    +
    $ rsgrad vib -i {1..3} {-3..-1} -x
    +[2022-07-14T18:32:49Z INFO  rsgrad::commands::vib] Parsing file "./OUTCAR"
    +[2022-07-14T18:32:49Z INFO  rsgrad::vasp_parsers::outcar] Saving mode #   1 as "./mode_0001_3682.13cm-1.xsf" ...
    +[2022-07-14T18:32:49Z INFO  rsgrad::vasp_parsers::outcar] Saving mode #   3 as "./mode_0003_3679.99cm-1.xsf" ...
    +[2022-07-14T18:32:49Z INFO  rsgrad::vasp_parsers::outcar] Saving mode #  44 as "./mode_0044_0010.79cm-1_imag.xsf" ...
    +[2022-07-14T18:32:49Z INFO  rsgrad::vasp_parsers::outcar] Saving mode #  43 as "./mode_0043_0007.12cm-1_imag.xsf" ...
    +[2022-07-14T18:32:49Z INFO  rsgrad::vasp_parsers::outcar] Saving mode #   2 as "./mode_0002_3680.83cm-1.xsf" ...
    +[2022-07-14T18:32:49Z INFO  rsgrad::vasp_parsers::outcar] Saving mode #  45 as "./mode_0045_0047.20cm-1_imag.xsf" ...
    +[2022-07-14T18:32:49Z INFO  rsgrad] Time used: 109.566967ms
    +
    +

    +
      +
    • Modulate the ground-state according to specified modes.
    • +
    +
    $ rsgrad vib -i {-3..-1} --modulate --amplitude 0.1
    +[2022-07-14T18:31:41Z INFO  rsgrad::commands::vib] Parsing file "./OUTCAR"
    +[2022-07-14T18:31:41Z INFO  rsgrad::vasp_parsers::outcar] Saving modulated POSCAR of mode #  43 with amplitude coeff 0.100 as "./mode_0043_0007.12cm-1_0.100_imag.vasp" ...
    +[2022-07-14T18:31:41Z INFO  rsgrad::vasp_parsers::outcar] Saving modulated POSCAR of mode #  44 with amplitude coeff 0.100 as "./mode_0044_0010.79cm-1_0.100_imag.vasp" ...
    +[2022-07-14T18:31:41Z INFO  rsgrad::vasp_parsers::outcar] Saving modulated POSCAR of mode #  45 with amplitude coeff 0.100 as "./mode_0045_0047.20cm-1_0.100_imag.vasp" ...
    +[2022-07-14T18:31:41Z INFO  rsgrad] Time used: 202.629805ms
    +
    +

    Wavefunction 3D

    +

    Main functions of rsgrad wav3d

    +
      +
    • List the brief information of WAVECAR;
    • +
    • Save the selected wavefunction to .vasp file.
    • +
    +

    Help Message

    +
    $ rsgrad wav3d --help
    +Plot wavefunction in realspace, and save it as '.vasp' file
    +
    +Usage: rsgrad wav3d [OPTIONS]
    +
    +Options:
    +  -w, --wavecar <WAVECAR>
    +          WAVECAR file name
    +          
    +          [default: ./WAVECAR]
    +
    +  -p, --poscar <POSCAR>
    +          POSCAR filename, POSCAR is needed to get the real-space wavefunction
    +          
    +          [default: ./POSCAR]
    +
    +  -s, --ispins [<ISPINS>...]
    +          Select spin index, starting from 1
    +          
    +          [default: 1]
    +
    +  -k, --ikpoints [<IKPOINTS>...]
    +          Select kpoint index, starting from 1.
    +          
    +          You can input ranges directly: `-k 1..4 5..10`
    +          
    +          [default: 1]
    +
    +  -b, --ibands [<IBANDS>...]
    +          Select band index, starting from 1.
    +          
    +          You can input ranges directly: `-b 1..4 5..10`
    +
    +  -l, --list
    +          List the brief info of current WAVECAR
    +
    +  -d, --detail
    +          Show the eigen values and band occupations of current WAVECAR.
    +          
    +          This flag should be used with `--list`
    +
    +      --gamma-half <GAMMA_HALF>
    +          Gamma Half direction of WAVECAR. You need to set this to 'x' or 'z' when processing WAVECAR produced by `vasp_gam`
    +          
    +          [possible values: x, z]
    +
    +      --ngrid <NGRID> <NGRID> <NGRID>
    +          Grid size for realspace wavefunction, 3 numbers are required, i.e. NGXF NGYF and NGZF.
    +          
    +          If this argument is left empty, NG_F will be set as NG_F=2*NG_.
    +          
    +          Be aware that NG_F must be greater than or at least equal to corresponding NG_.
    +
    +  -o, --output-parts [<OUTPUT_PARTS>...]
    +          Specify output part of the wavefunction.
    +          
    +          Detailed message:
    +           - normsquared/ns: Perform `ρ(r) = |ѱ(r)|^2` action to get the spatial distribution of selected band.
    +           - real/re: Real part of the wavefunction, suffix '_re.vasp' is added to the output filename.
    +           - imag/im: Imaginary part of the wavefunction, suffix '_im.vasp' is added to the output filename.
    +           - reim: Output both real part and imaginary parts of the wavefunction.
    +           - uns/dns: Perform `ρ(r) = |ѱ(r)|^2` for spinor up/down only. **Note: this option works for `ncl` WAVECAR only.**
    +          
    +          [possible values: normsquared, ns, uns, dns, real, re, imag, im, reim]
    +
    +      --prefix <PREFIX>
    +          Prefix of output filename
    +          
    +          [default: wav]
    +
    +  -e, --show-eigs-suffix
    +          Add eigen value suffix to the filename
    +
    +      --sum-chgs
    +          Perform sum-up of the charge densities for selected bands.
    +          
    +          With this flag open, only `normsquared` or `ns` or `uns` or `dns` are allowed for the `-o`/`--output-parts` option.
    +           IMPORTANT NOTES:
    +           - The prefix for output filename `sum-prefix` is also required and has no default prefix.
    +           - The individual charge densities will not be saved to corresponding '.vasp' files if this flag is on.
    +
    +      --sum-prefix <SUM_PREFIX>
    +          Specify the output file for the summed charge densities.
    +          
    +          This argument is required if `sum_chgs` is on.
    +
    +  -h, --help
    +          Print help (see a summary with '-h')
    +
    +

    Example

    +
      +
    • List the brief information of WAVECAR
    • +
    +
    $ rsgrad wav3d -l
    +
    +[2022-07-14T09:19:51Z INFO  rsgrad::commands::wav3d] Reading WAVECAR: "./WAVECAR"
    +LENGTH     =             54145104
    +RECLEN     =              1388336
    +TYPE       =             Standard
    +NSPIN      =                    1
    +NKPTS      =                    1
    +NBANDS     =                   36
    +ENCUT      =              450.000
    +EFERMI     =               -5.368
    +VOLUME     =             8000.000
    +NGRID      = [  71,   71,   71]
    +NPLWS      = [173541]
    +ACELL      = [[  20.000,    0.000,    0.000], [   0.000,   20.000,    0.000], [   0.000,    0.000,   20.000]]
    +BCELL      = [[   0.050,    0.000,    0.000], [   0.000,    0.050,    0.000], [   0.000,    0.000,    0.050]]
    +
    +
    +[2022-07-14T09:19:51Z INFO  rsgrad] Time used: 160.337862ms
    +
    +

    if you want the band eigen values information

    +
    $ rsgrad wav3d -ld
    +
    +...
    +<BRIEF INFORMATION ABOUT WAVECAR>
    +...
    +
    +ISPIN:  1  IKPOINT:    1  IBAND:     1 E-Efermi:    -19.991 Occupation: 1.000
    +ISPIN:  1  IKPOINT:    1  IBAND:     2 E-Efermi:    -18.141 Occupation: 1.000
    +ISPIN:  1  IKPOINT:    1  IBAND:     3 E-Efermi:    -18.141 Occupation: 1.000
    +ISPIN:  1  IKPOINT:    1  IBAND:     4 E-Efermi:    -16.418 Occupation: 1.000
    +ISPIN:  1  IKPOINT:    1  IBAND:     5 E-Efermi:    -15.534 Occupation: 1.000
    +ISPIN:  1  IKPOINT:    1  IBAND:     6 E-Efermi:    -15.532 Occupation: 1.000
    +ISPIN:  1  IKPOINT:    1  IBAND:     7 E-Efermi:    -10.662 Occupation: 1.000
    +ISPIN:  1  IKPOINT:    1  IBAND:     8 E-Efermi:    -10.661 Occupation: 1.000
    +...
    +
    +
      +
    • Save the selected wavefunction to .vasp file
    • +
    +
    $ rsgrad wav3d -b {10..20} -o ns -e
    +
    +[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Reading WAVECAR: "./WAVECAR"
    +[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Reading POSCAR: "./POSCAR"
    +[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   10 ...
    +[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   13 ...
    +[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   11 ...
    +[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   14 ...
    +[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   12 ...
    +[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   15 ...
    +[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-13_-5.740eV.vasp" ...
    +[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-15_-5.601eV.vasp" ...
    +[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-14_-5.728eV.vasp" ...
    +[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-10_-8.376eV.vasp" ...
    +[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-11_-7.385eV.vasp" ...
    +[2022-07-14T09:23:06Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-12_-7.380eV.vasp" ...
    +[2022-07-14T09:23:08Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   18 ...
    +[2022-07-14T09:23:08Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   19 ...
    +[2022-07-14T09:23:09Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-18_-3.514eV.vasp" ...
    +[2022-07-14T09:23:09Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   16 ...
    +[2022-07-14T09:23:09Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   20 ...
    +[2022-07-14T09:23:09Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-19_-3.265eV.vasp" ...
    +[2022-07-14T09:23:09Z INFO  rsgrad::commands::wav3d] Processing spin 1, k-point   1, band   17 ...
    +[2022-07-14T09:23:10Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-16_-5.477eV.vasp" ...
    +[2022-07-14T09:23:10Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-17_-3.546eV.vasp" ...
    +[2022-07-14T09:23:10Z INFO  rsgrad::commands::wav3d] Writing "wav_1-1-20_-0.701eV.vasp" ...
    +[2022-07-14T09:23:11Z INFO  rsgrad] Time used: 5.484733549s
    +
    +

    Open the .vasp in VESTA

    +

    +

    rsgrad wav3d supports extracting multiple bands at the same time, and the processes +executed in parallel, which can save a lot of time.

    +

    Wavefunction 1D

    +

    This command is similar to rsgrad wav3d. The only difference is that wav1d integrates +the wavefunction over specified plane, and produces the averaged one dimensional wavefunction.

    +

    This command is useful when you are looking for image potential states.

    +
    + +

    Help Message

    +
    $ rsgrad wav1d --help
    +rsgrad-wav1d 
    +Plot wavefunction in realspace, then integrate over some plane, and save it as '.txt' file
    +
    +USAGE:
    +    rsgrad wav1d [OPTIONS]
    +
    +OPTIONS:
    +        --axis <AXIS>
    +            Integration direction. e.g. if 'z' is provided, the XoY plane is integrated
    +            
    +            [default: z]
    +            [possible values: X, Y, Z]
    +
    +    -b, --ibands <IBANDS>...
    +            Select band index, starting from 1
    +
    +    -d, --detail
    +            Show the eigen values and band occupations of current WAVECAR.
    +            
    +            This flag should be used with `--list`
    +
    +        --gamma-half <GAMMA_HALF>
    +            Gamma Half direction of WAVECAR. You need to set this to 'x' or 'z' when processing
    +            WAVECAR produced by `vasp_gam`
    +            
    +            [possible values: x, z]
    +
    +    -h, --help
    +            Print help information
    +
    +        --htmlout <HTMLOUT>
    +            Specify the file name to be written with html wav1d data
    +            
    +            [default: wav1d.html]
    +
    +    -k, --ikpoints <IKPOINTS>...
    +            Select kpoint index, starting from 1
    +            
    +            [default: 1]
    +
    +    -l, --list
    +            List the brief info of current WAVECAR
    +
    +    -s, --ispins <ISPINS>...
    +            Select spin index, starting from 1
    +            
    +            [default: 1]
    +
    +        --scale <SCALE>
    +            Scale the wavefunction
    +            
    +            [default: 10]
    +
    +        --show
    +            Open the browser and show the plot immediately
    +
    +        --to-inline-html
    +            Render the plot and print thw rendered code to stdout
    +
    +        --txtout <TXTOUT>
    +            Specify the file name to be written with raw wav1d data
    +            
    +            [default: wav1d.txt]
    +
    +    -w, --wavecar <WAVECAR>
    +            WAVECAR file name
    +            
    +            [default: ./WAVECAR]
    +
    +

    Example

    +

    The usage is similar to rsgrad wav3d, too.

    +
    $ rsgrad wav1d -b {20..27}
    +[2022-07-14T12:54:35Z INFO  rsgrad::commands::wav1d] Reading WAVECAR: "./WAVECAR"
    +[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Processing spin 1, k-point   1, band   20 ...
    +[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Processing spin 1, k-point   1, band   24 ...
    +[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Processing spin 1, k-point   1, band   22 ...
    +[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Processing spin 1, k-point   1, band   23 ...
    +[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Processing spin 1, k-point   1, band   21 ...
    +[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Processing spin 1, k-point   1, band   26 ...
    +[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Processing spin 1, k-point   1, band   27 ...
    +[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Processing spin 1, k-point   1, band   25 ...
    +[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Writing to "wav1d.html"
    +[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Writing to "wav1d.txt"
    +[2022-07-14T12:54:36Z INFO  rsgrad::commands::wav1d] Printing inline html to stdout ...
    +[2022-07-14T12:54:36Z INFO  rsgrad] Time used: 864.911523ms
    +
    +

    Then produces

    +
    + +

    Note: The Fermi level is shiftted to 0.0 eV

    +

    Workfunction

    +

    rsgrad workfunc reads LOCPOT to calculate the work function. For further discussion about +work function, please read this blog.

    +
    + +

    Note: rsgrad workfunc does not show the vacuum level directly, hence you need to find it by +hovering on the step of the work function. Take the work function above as an example, the +vacuum level should be about 4.048eV around 40Å.

    +

    Help Message

    +
    $ rsgrad workfunc --help
    +rsgrad-workfunc
    +Calculate work-function from LOCPOT file, OUTCAR is also needed to get the Fermi level.
    +
    +The work function is calculated by plannar integration of the data cube in LOCPOT. The selected axis
    +should be perpendicular to the other two axises.
    +
    +USAGE:
    +    rsgrad workfunc [OPTIONS] [LOCPOT]
    +
    +ARGS:
    +    <LOCPOT>
    +            LOCPOT file path. Turn on 'LVHAR' in INCAR to get the electro-static potential saved it
    +
    +            [default: ./LOCPOT]
    +
    +OPTIONS:
    +        --axis <AXIS>
    +            Integration direction. e.g. if 'z' is provided, the XoY plane is integrated
    +
    +            [default: z]
    +            [possible values: X, Y, Z]
    +
    +    -h, --help
    +            Print help information
    +
    +    -o, --htmlout <HTMLOUT>
    +            Write the plot to html and view it in the web browser
    +
    +            [default: ./workfunction.html]
    +
    +        --outcar <OUTCAR>
    +            OUTCAR file path. This file is needed to get the E-fermi level and lattice properties
    +
    +            [default: ./OUTCAR]
    +
    +        --show
    +            Open default browser to see the plot immediately
    +
    +        --to-inline-html
    +            Render the plot and print the rendered code to stdout
    +
    +        --txtout <TXTOUT>
    +            Write the raw plot data as txt file in order to replot it with more advanced tools
    +
    +            [default: locpot.txt]
    +
    +

    Example

    +

    In general, you don't need t provide additional arguments.

    +
    $ rsgrad workfunc
    +[2022-07-14T14:41:38Z INFO  rsgrad::commands::workfunc] Reading "./OUTCAR"
    +[2022-07-14T14:41:38Z INFO  rsgrad::commands::workfunc] Reading electro-static potential data from "./LOCPOT"
    +[2022-07-14T14:41:39Z INFO  rsgrad::commands::workfunc] Writing raw plot data to "locpot.txt"
    +[2022-07-14T14:41:39Z INFO  rsgrad::commands::workfunc] Writing to "./workfunction.html"
    +[2022-07-14T14:41:39Z INFO  rsgrad] Time used: 1.352347116s
    +
    +
    + +

    POSCAR

    +

    There are several operations that rsgrad pos can do

    +
      +
    • Convert the fractional coordinates to Cartesian coordinates or convert reversely;
    • +
    • Split the POSCAR and save the two parts;
      +This command is useful when you want to calculate charge density difference and adsorption energy.
    • +
    • Format the POSCAR and add element symbol tags to each atom.
    • +
    +

    Help Message

    +
    $ rsgrad pos --help
    +rsgrad-pos 
    +Operation(s) about POSCAR, including split it into two POSCARs
    +
    +USAGE:
    +    rsgrad pos [OPTIONS] [--] [POSCAR]
    +
    +ARGS:
    +    <POSCAR>
    +            Specify the input POSCAR file
    +            
    +            [default: ./POSCAR]
    +
    +OPTIONS:
    +    -a, --a-name <A_NAME>
    +            Splitted POSCAR path with selected atoms
    +            
    +            [default: POSCAR_A]
    +
    +    -b, --b-name <B_NAME>
    +            Splitted POSCAR path with complement of `a_name`
    +            
    +            [default: POSCAR_B]
    +
    +    -c, --cartesian
    +            Cartesian coordinates is used in writting POSCAR
    +
    +        --convert
    +            Convert POSCAR to cartesian coordinates or fractional coordinates
    +
    +        --converted <CONVERTED>
    +            The target path of converted POSCAR
    +            
    +            [default: POSCAR_new]
    +
    +    -h, --help
    +            Print help information
    +
    +    -i, --select-indices <SELECT_INDICES>...
    +            Selects the indices to operate.
    +            
    +            Step indices start from '1', if '0' is given, all the structures will be selected. Step
    +            indices can be negative, where negative index means counting reversely. E.g. "-i -2 -1 1
    +            2 3" means selecting the last two and the first three atom.
    +
    +        --no-add-symbols-tags
    +            The symbols of each atom will not be written as comment in POSCAR
    +
    +        --no-preserve-constraints
    +            Atom constraints will be dropped when writting POSCAR
    +
    +    -s, --split
    +            Split POSCAR according to selected_indices
    +
    +

    Examples

    +
      +
    • Format the POSCAR to add element symbol tags
    • +
    +

    The original POSCAR of CO2:

    +
     C  O 
    + 1.0000000000000000
    +    20.0000000000000000    0.0000000000000000    0.0000000000000000
    +     0.0000000000000000   20.0000000000000000    0.0000000000000000
    +     0.0000000000000000    0.0000000000000000   20.0000000000000000
    + C   O  
    +   1   2
    +Direct
    +  0.5000000000000000  0.5000000000000000 -0.5000000000000000
    +  0.5754584707965210  0.4974961803083730  0.5000000000000000
    +  0.4249089651951450  0.5078477015701101  0.5000000000000000
    +
    +

    Then run rsgrad pos POSCAR --convert

    +
    $ rsgrad pos POSCAR --convert
    +[2022-07-14T15:38:47Z INFO  rsgrad::commands::pos] Reading POSCAR file "POSCAR" ...
    +[2022-07-14T15:38:47Z INFO  rsgrad::commands::pos] Converting it to "POSCAR_new"
    +[2022-07-14T15:38:47Z INFO  rsgrad::commands::pos] Done
    +[2022-07-14T15:38:47Z INFO  rsgrad] Time used: 1.96796ms
    +
    +

    The formatted file should be POSCAR_new

    +
    C  O
    + 1.0000000
    +      20.000000000       0.000000000       0.000000000
    +       0.000000000      20.000000000       0.000000000
    +       0.000000000       0.000000000      20.000000000
    +      C      O
    +      1      2
    +Direct
    +      0.5000000000      0.5000000000     -0.5000000000 !      C-001    1
    +      0.5754584708      0.4974961803      0.5000000000 !      O-001    2
    +      0.4249089652      0.5078477016      0.5000000000 !      O-002    3
    +
    +
      +
    • Convert POSCAR to Cartesian coordinates
    • +
    +

    Just run rsgrad pos POSCAR --convert --cartesian

    +
    $ rsgrad pos POSCAR --convert --cartesian
    +[2022-07-14T15:40:33Z INFO  rsgrad::commands::pos] Reading POSCAR file "POSCAR" ...
    +[2022-07-14T15:40:33Z INFO  rsgrad::commands::pos] Converting it to "POSCAR_new"
    +[2022-07-14T15:40:33Z INFO  rsgrad::commands::pos] Done
    +[2022-07-14T15:40:33Z INFO  rsgrad] Time used: 1.57861ms
    +
    +

    The converted file POSCAR_new should be like

    +
    C  O
    + 1.0000000
    +      20.000000000       0.000000000       0.000000000
    +       0.000000000      20.000000000       0.000000000
    +       0.000000000       0.000000000      20.000000000
    +      C      O
    +      1      2
    +Cartesian
    +     10.0000000000     10.0000000000    -10.0000000000 !      C-001    1
    +     11.5091694159      9.9499236062     10.0000000000 !      O-001    2
    +      8.4981793039     10.1569540314     10.0000000000 !      O-002    3
    +
    +
      +
    • Split the POSCAR
    • +
    +

    Let take the CO2 structure as the example again. Here we will take the +C atom out to see what the operation does.

    +

    The C atom index is 1, so we should run rsgrad pos POSCAR -s -i 1

    +
    $ rsgrad pos POSCAR -s -i 1
    +[2022-07-14T15:49:32Z INFO  rsgrad::commands::pos] Reading POSCAR file "POSCAR" ...
    +[2022-07-14T15:49:32Z INFO  rsgrad::commands::pos] Splitting it to "POSCAR_A" and "POSCAR_B" ...
    +[2022-07-14T15:49:32Z INFO  rsgrad::commands::pos] "POSCAR_A" contains
    +[2022-07-14T15:49:32Z INFO  rsgrad::commands::pos]       C     1
    +[2022-07-14T15:49:32Z INFO  rsgrad::commands::pos] "POSCAR_B" contains
    +[2022-07-14T15:49:32Z INFO  rsgrad::commands::pos]       O     2
    +[2022-07-14T15:49:32Z INFO  rsgrad::commands::pos] "POSCAR_A" written
    +[2022-07-14T15:49:32Z INFO  rsgrad::commands::pos] "POSCAR_B" written
    +[2022-07-14T15:49:32Z INFO  rsgrad] Time used: 2.11275ms
    +
    +

    The separated files should be like

    +
    $ bat POSCAR_A POSCAR_B
    +───────┬──────────────────────────────────────────────────────────────────────────
    +       │ File: POSCAR_A
    +───────┼──────────────────────────────────────────────────────────────────────────
    +   1   │ Generated by rsgrad, POSCAR with selected atoms
    +   2   │  1.0000000
    +   3   │       20.000000000       0.000000000       0.000000000
    +   4   │        0.000000000      20.000000000       0.000000000
    +   5   │        0.000000000       0.000000000      20.000000000
    +   6   │       C
    +   7   │       1
    +   8   │ Direct
    +   9   │       0.5000000000      0.5000000000     -0.5000000000 !      C-001    1
    +───────┴──────────────────────────────────────────────────────────────────────────
    +───────┬──────────────────────────────────────────────────────────────────────────
    +       │ File: POSCAR_B
    +───────┼──────────────────────────────────────────────────────────────────────────
    +   1   │ Generated by rsgrad, POSCAR complement
    +   2   │  1.0000000
    +   3   │       20.000000000       0.000000000       0.000000000
    +   4   │        0.000000000      20.000000000       0.000000000
    +   5   │        0.000000000       0.000000000      20.000000000
    +   6   │       O
    +   7   │       2
    +   8   │ Direct
    +   9   │       0.5754584708      0.4974961803      0.5000000000 !      O-001    1
    +  10   │       0.4249089652      0.5078477016      0.5000000000 !      O-002    2
    +───────┴──────────────────────────────────────────────────────────────────────────
    +
    +

    The process schema:

    +

    +

    Pseudo Potential

    +

    This command generates POTCAR according to POSCAR. The usage is simple: rsgrad pot in the directory with POSCAR presents.

    +

    To use this command, a configuration file is required like:

    +
    [functional-path]
    +PAW_PBE = "<path of PAW_PBE>"
    +PAW_LDA = "<path of PAW_LDA>"
    +
    +

    and you need to put it at ~/.rsgrad for Linux/macOS, +and C:\Users\<YourUserName>\.rsgrad.toml for Windows.

    +

    Note: rsgrad pot will give some hint if you have no idea on how to write the file.

    +

    Then you can specify the element type in POSCAR, for example:

    +
    Cd2 S2 HSE optimized
    +   1.00000000000000
    +     4.1704589747753724    0.0000000049514629    0.0000000000000000
    +    -2.0852299788115007    3.6117232476351271   -0.0000000000000000
    +     0.0000000000000000   -0.0000000000000000    6.7822968954189937
    +   Cd   S
    +     2     2
    +Direct
    +  0.6666669999999968  0.3333330000000032  0.5001535716160643
    +  0.3333330000000032  0.6666669999999968  0.0001535716160644
    +  0.6666669999999968  0.3333330000000032  0.8768464283839381
    +  0.3333330000000032  0.6666669999999968  0.3768464283839381
    +
    +

    Finally rsgrad-pot will read the line " Cd S ", and find the corresponding POTCAR and merge them.

    +

    In some cases, several elements does not have "standard" POTCAR that without suffix. E.g. the K/POTCAR +is not available for PBE functional. We provide two solutions for it:

    +
      +
    • Write K_sv or other available K-related functionals in POSCAR +
      Cd2 S2 HSE optimized
      +   1.00000000000000
      +     4.1704589747753724    0.0000000049514629    0.0000000000000000
      +    -2.0852299788115007    3.6117232476351271   -0.0000000000000000
      +     0.0000000000000000   -0.0000000000000000    6.7822968954189937
      +   Cd   K_sv
      +     2     2
      +Direct
      +  0.6666669999999968  0.3333330000000032  0.5001535716160643
      +  ...
      +
      +
    • +
    • Use aliases field in .rsgrad.toml +
      [functional-path]
      +...
      +aliases = { K = "K_sv" }
      +
      +or +
      [functional-path]
      +...
      +[functional-path.aliases]
      +K = "K_sv"
      +
      +
    • +
    +

    Help Message

    +
    rsgrad-pot
    +Generate the POTCAR according to POSCAR
    +
    +USAGE:
    +    rsgrad pot [OPTIONS] [FUNCTIONAL]
    +
    +ARGS:
    +    <FUNCTIONAL>
    +            Specify the functional type, now only "PAW_PBE"(or "paw_pbe") and "PAW_LDA"(or
    +            "paw_lda") are available
    +
    +            [default: PAW_PBE]
    +
    +OPTIONS:
    +    -c, --config <CONFIG>
    +            Specify the configuration file, if left blank, rsgrad will read `.rsgrad.toml` at your
    +            home dir
    +
    +    -h, --help
    +            Print help information
    +
    +    -p, --poscar <POSCAR>
    +            Specify the POSCAR file
    +
    +            Note: the elements symbols' line should involve the specified valence configuration if
    +            you need. For example, if you need a `K_sv` POTCAR for `K`, just write `K_sv` in the
    +            POSCAR
    +
    +            [default: ./POSCAR]
    +
    +    -s, --save-in <SAVE_IN>
    +            Specify where the `POTCAR` would be written
    +
    +            [default: ./]
    +
    +

    Example

    +
    $ rsgrad pot
    +[2023-10-20T16:19:48Z INFO  rsgrad::settings] Reading rsgrad settings from "/Users/ionizing/.rsgrad.toml" ...
    +[2023-10-20T16:19:48Z INFO  rsgrad::settings] Checking rsgrad setting availability ...
    +[2023-10-20T16:19:48Z INFO  rsgrad::commands::pot] Reading POSCAR file "../tests/POSCAR.CdS_HSE" ...
    +[2023-10-20T16:19:48Z INFO  rsgrad::vasp_parsers::potcar] Reading POTCAR from "/Users/ionizing/apps/vasp/pp/potpaw_PBE.54/Cd/POTCAR"
    +[2023-10-20T16:19:48Z INFO  rsgrad::vasp_parsers::potcar] Reading POTCAR from "/Users/ionizing/apps/vasp/pp/potpaw_PBE.54/S/POTCAR"
    +[2023-10-20T16:19:48Z INFO  rsgrad::commands::pot] Writing POTCAR to "./POTCAR" ...
    +[2023-10-20T16:19:48Z INFO  rsgrad] Time used: 5.524643ms
    +
    +

    Transition Dipole Moment

    +

    This command (rsgrad tdm) calculates the transition dipole moment(tdm) +between given bands, and then plot the peaks with plotly.

    +
    + +

    Note: This command can only calculate the TDM between bands in same k-point. The inter-kpoint +transition is not supported yet. Also, this commands calculates the TDM in reciprocal space by

    +

    \[ +TDM_{i\to j} = \langle \phi_j | e\cdot\vec{r} | \phi_i \rangle = e\cdot\frac{i\hbar}{m_e\Delta E_{ij}} \langle \phi_j | \vec{p} | \phi_i \rangle +\]

    +

    Also, this command only calculates the TDM if \(j > i\), otherwise it will ignore the invalid \(i\to j\) pairs.

    +

    Help Message

    +
    $ rsgrad tdm --help
    +rsgrad-tdm
    +Calculate Transition Dipole Moment (TDM) between given bands.
    +
    +Note: This command can only calculate the TDM between bands in same k-point. The inter-kpoint
    +transition is not supported yet. Also, this commands calculates the TDM in reciprocal space by
    +
    +tdm_{i->j} = <phi_j|e*r|phi_i> = i*ħ/(ΔE*m)*<phi_j|p|phi_i>
    +
    +USAGE:
    +    rsgrad tdm [OPTIONS] --ibands <IBANDS>... --jbands <JBANDS>...
    +
    +OPTIONS:
    +        --barwidth <BARWIDTH>
    +            Specify the width of bars in the center of peaks. (eV)
    +
    +            [default: 0.1]
    +
    +        --gamma-half <GAMMA_HALF>
    +            Gamma Half direction of WAVECAR. You need to set this to 'x' or 'z' when processing
    +            WAVECAR produced by `vasp_gam`
    +
    +            [possible values: x, z]
    +
    +    -h, --help
    +            Print help information
    +
    +        --htmlout <HTMLOUT>
    +            Write the plot of TDM to html file
    +
    +            [default: tdm_smeared.html]
    +
    +    -i, --ibands <IBANDS>...
    +            Initial band indices, start from 1
    +
    +    -j, --jbands <JBANDS>...
    +            Final band indices, starts from 1
    +
    +    -k, --ikpoint <IKPOINT>
    +            K-point index, starts from 1
    +
    +            [default: 1]
    +
    +        --npoints <NPOINTS>
    +            How many points in the x axis PER eV
    +
    +            [default: 500]
    +
    +        --peakout <PEAKOUT>
    +            Write the TDM peaks to raw txt file
    +
    +            [default: tdm_peaks.txt]
    +
    +    -s, --ispin <ISPIN>
    +            Spin index, 1 for up, 2 for down
    +
    +            [default: 1]
    +            [possible values: 1, 2]
    +
    +        --show
    +            Open the default browser to show the plot
    +
    +        --sigma <SIGMA>
    +            Smearing width, in eV
    +
    +            [default: 0.05]
    +
    +        --to-inline-html
    +            Print the inline HTML to stdout
    +
    +        --txtout <TXTOUT>
    +            Write the summed and smeared TDM to raw txt file
    +
    +            [default: tdm_smeared.txt]
    +
    +    -v, --verbose
    +            Print the calculated TDM to screen
    +
    +    -w, --wavecar <WAVECAR>
    +            WAVECAR file path
    +
    +            [default: ./WAVECAR]
    +
    +        --xmax <XMAX>
    +            Highest energy scale for tdm_smeared.txt, default for max(dE) + 2.0
    +
    +        --xmin <XMIN>
    +            Lowest energy scale for tdm_smeared.txt, default for min(dE) - 2.0
    +
    +

    Example

    +

    The -i and -j arguments are required, or it will complain with error.

    +
    $ rsgrad tdm -i 2 -j {3..5}
    +[2022-08-10T07:26:46Z INFO  rsgrad::commands::tdm] Reading "./WAVECAR"
    +[2022-08-10T07:26:46Z INFO  rsgrad::commands::tdm] Writing peaks info to "tdm_peaks.txt" ...
    +[2022-08-10T07:26:46Z INFO  rsgrad::commands::tdm] Writing smeared TDM data to "tdm_smeared.txt"
    +[2022-08-10T07:26:46Z INFO  rsgrad::commands::tdm] Writing plot to "tdm_smeared.html"
    +[2022-08-10T07:26:46Z INFO  rsgrad] Time used: 56.655387ms
    +
    +

    It produces the HTML like:

    +
    + +

    You can view the \(x\), \(y\) and \(z\) components of each peak by hovering on the thin bars +at the center of peaks.

    +

    Note: If two peaks are in the same x position, one of them will be covered.

    +

    Then the tdm_peaks.txt should be like:

    +
    # iband jband     E_i     E_j      ΔE        Tx       Ty       Tz
    +      2     3  -5.974  -3.675   2.298     1.311    2.556    0.000
    +      2     4  -5.974  -3.675   2.298     2.556    1.311    0.000
    +      2     5  -5.974  -0.975   4.999     0.000    0.000    5.309
    +
    +

    And the tdm_smeared.txt should be like:

    +
    # E(eV)    Tx(Debye)   Ty(Debye)   Tz(Debye)
    +         0.298325         0.007692         0.007692         0.001912         0.017295
    +         0.300240         0.007706         0.007706         0.001914         0.017326
    +         0.302155         0.007721         0.007721         0.001915         0.017357
    +         0.304070         0.007736         0.007736         0.001917         0.017389
    +         0.305985         0.007751         0.007751         0.001918         0.017420
    +         0.307900         0.007766         0.007766         0.001920         0.017451
    +...
    +...
    +
    +

    Then you can plot the TDM peaks with other tools like OriginPro.

    +

    If your WAVECAR is produced by vasp_gam, you'd better specify the gamma half direction by --gamma-half x or --gamma-half z, +or rsgrad tdm will produce wrong results.

    +

    Gap

    +

    This command (rsgrad gap) calculates the band gap and prints positions of VBM and CBM.

    +

    There are two ways to run this command:

    +
      +
    1. Use WAVECAR only. All required information can be extracted from WAVECAR.
    2. +
    3. Or use PROCAR and OUTCAR instead. PROCAR is read for the band energies, band occupations and k-point coordinates; +OUTCAR is read for the Fermi level only.
    4. +
    +

    Note: Usually it's faster to parse results from WAVECAR.

    +

    If your system is a non-SCF calculation for band structure, you may need to specify the correct Fermi level by +rsgrad gap -e <put the correct E-fermi here>, the correct Fermi level can be obtained from the OUTCAR of SCF calculation.

    +

    Help Message

    +
    $ rsgrad gap --help
    +rsgrad-gap
    +Find band gap and print positions of VBM and CBM
    +
    +USAGE:
    +    rsgrad gap [OPTIONS]
    +
    +OPTIONS:
    +    -e, --efermi <EFERMI>      Specify Fermi level, if left empty, this value would be read from
    +                               WAVECAR or OUTCAR
    +    -h, --help                 Print help information
    +    -o, --outcar <OUTCAR>      OUTCAR file name, this file is parsed to get Fermi level only
    +                               [default: OUTCAR]
    +    -p, --procar <PROCAR>      PROCAR file name, OUTCAR is also needed to get Fermi level [default:
    +                               PROCAR]
    +    -w, --wavecar <WAVECAR>    WAVECAR file name, no more files needed [default: WAVECAR]
    +
    +

    Example

    +
      +
    1. For metal system:
    2. +
    +
    [2022-12-01T11:30:49Z INFO  rsgrad::commands::gap] Trying to parse "WAVECAR" ...
    +----------------------------------------
    + Current system is         Metal
    +----------------------------------------
    +[2022-12-01T11:30:49Z INFO  rsgrad] Time used: 166.251241ms
    +
    +
      +
    1. For non-spin-polarized direct gap system:
    2. +
    +
    [2022-12-01T11:37:15Z INFO  rsgrad::commands::gap] Trying to parse "WAVECAR" ...
    +--------------------------------------------------------------------------------
    + Current system has    Direct Gap    of   0.328    eV
    +  CBM @ k-point     1 of ( 0.000, 0.000, 0.000) , band   819 of    0.322 eV
    +  VBM @ k-point     1 of ( 0.000, 0.000, 0.000) , band   818 of   -0.006 eV
    +--------------------------------------------------------------------------------
    +[2022-12-01T11:37:15Z INFO  rsgrad] Time used: 253.556682ms
    +
    +
      +
    1. For spin-polarized direct gap system:
    2. +
    +
    $ rsgrad gap
    +[2022-12-01T11:38:16Z INFO  rsgrad::commands::gap] Trying to parse "WAVECAR" ...
    +--------------------------------------------------------------------------------
    +    ====================  Gap Info For     SPIN UP      ====================
    + Current system has    Direct Gap    of   0.976    eV
    +  CBM @ k-point     1 of ( 0.000, 0.000, 0.000) , band   129 of    0.498 eV
    +  VBM @ k-point     1 of ( 0.000, 0.000, 0.000) , band   128 of   -0.478 eV
    +    ====================  Gap Info For    SPIN DOWN     ====================
    + Current system has    Direct Gap    of   0.980    eV
    +  CBM @ k-point     1 of ( 0.000, 0.000, 0.000) , band   129 of    0.499 eV
    +  VBM @ k-point     1 of ( 0.000, 0.000, 0.000) , band   128 of   -0.481 eV
    +--------------------------------------------------------------------------------
    +[2022-12-01T11:38:16Z INFO  rsgrad] Time used: 31.744371ms
    +
    +
      +
    1. For non-spin-polarized indirect gap system:
    2. +
    +
    $ rsgrad gap
    +[2022-12-01T11:40:52Z INFO  rsgrad::commands::gap] Trying to parse "WAVECAR" ...
    +--------------------------------------------------------------------------------
    + Current system has   Indirect Gap   of   1.160    eV
    +  CBM @ k-point    25 of ( 0.000, 0.444, 0.444) , band     5 of    1.097 eV
    +  VBM @ k-point    17 of ( 0.000, 0.000, 0.000) , band     4 of   -0.062 eV
    +--------------------------------------------------------------------------------
    +[2022-12-01T11:40:52Z INFO  rsgrad] Time used: 22.565948ms
    +
    +

    UnitConversion

    +

    This command (rsgrad uc) converts input quantity to units representing same energy.

    +

    Metric prefixes are supported, from Atto(a, 10-18) to Exa(E, 1018).

    +

    Here are supported prefixes and corresponding acronyms:

    + + + + + + + + + + + + + + +
    Metric prefixAcronymBase 10
    attoa10-18
    femtof10-15
    picop10-12
    nanon10-9
    microμ10-6
    millim10-3
    ----100
    KiloK103
    MegaM106
    GigaG109
    TeraT1012
    PetaP1015
    exaE1018
    +

    If you use acronyms, note that prefixes smaller than 1 (from a, atto to m, micro) must be +lowercased whereas the prefixes lager than 1 (from K, Kilo to E, Exa) must be uppercased.

    +

    Supported units:

    + + + + + + + + + + +
    UnitSymbol
    HartreeHa
    Wavenumbercm-1
    Temperature(Kelvin)K
    Calorie per moleCal/mol
    Joule per moleJ/mol
    Wavelengthm
    Periods
    Electron volteV
    FrequencyHz
    +

    Help Message

    +
    $ rsgrad uc
    +Conversion between various energy units
    +
    +Usage: rsgrad uc [INPUT]...
    +
    +Arguments:
    +  [INPUT]...  Input energy quantity to be converted. Multiple input are supported
    +
    +Options:
    +  -h, --help  Print help
    +
    +Try `rsgrad uc 298K` to see what happens.
    +
    +

    Examples

    +
    $ rsgrad uc 298K
    +==================== Processing input "298K" ====================
    +  298.000000 K ==   943.709369 μHa
    +  298.000000 K ==   207.125149 cm-1
    +  298.000000 K ==   298.000000 K
    +  298.000000 K ==   592.202785 Cal/mol
    +  298.000000 K ==     2.477776 KJ/mol
    +  298.000000 K ==    48.281101 μm
    +  298.000000 K ==   161.048425 fs
    +  298.000000 K ==    25.679653 meV
    +  298.000000 K ==     6.209312 THz
    +================================================================================
    +
    +[2024-09-11T07:21:07Z INFO  rsgrad] Time used: 470.398µs
    +
    +

    You can also input multiple quantities at a time

    +
    $ rsgrad uc 298K 25meV 300THz
    +==================== Processing input "298K" ====================
    +  298.000000 K ==   161.048425 fs
    +  298.000000 K ==   207.125149 cm-1
    +  298.000000 K ==     2.477776 KJ/mol
    +  298.000000 K ==    25.679653 meV
    +  298.000000 K ==    48.281101 μm
    +  298.000000 K ==   943.709369 μHa
    +  298.000000 K ==   592.202785 Cal/mol
    +  298.000000 K ==     6.209312 THz
    +  298.000000 K ==   298.000000 K
    +================================================================================
    +
    +==================== Processing input "25meV" ====================
    +   25.000000 meV ==   165.426708 fs
    +   25.000000 meV ==   201.643250 cm-1
    +   25.000000 meV ==     2.412198 KJ/mol
    +   25.000000 meV ==    25.000000 meV
    +   25.000000 meV ==    49.593677 μm
    +   25.000000 meV ==   918.732590 μHa
    +   25.000000 meV ==   576.529191 Cal/mol
    +   25.000000 meV ==     6.044973 THz
    +   25.000000 meV ==   290.112953 K
    +================================================================================
    +
    +==================== Processing input "300THz" ====================
    +  300.000000 THz ==     3.333333 fs
    +  300.000000 THz ==    10.007154 Kcm-1
    +  300.000000 THz ==   119.712599 KJ/mol
    +  300.000000 THz ==     1.240700 eV
    +  300.000000 THz ==   999.308150 nm
    +  300.000000 THz ==    45.594872 mHa
    +  300.000000 THz ==    28.611998 KCal/mol
    +  300.000000 THz ==   300.000000 THz
    +  300.000000 THz ==    14.397729 KK
    +================================================================================
    +
    +[2024-09-11T07:27:53Z INFO  rsgrad] Time used: 544.171µs
    +
    +

    Feedback

    +

    We are happy that you reach here. As an open-source project, rsgrad welcomes feedback.

    +
      +
    • +

      If you have want to add features to rsgrad, just open an issue at +GitHub Issues. We also created a feature-requests list, +you can follow it at this page.

      +
    • +
    • +

      If rsgrad complains something or produces wrong result, just open an issue at +GitHub Issues. We are grateful if you can provide +the input files in order that we can reproduce the issue conveniently, +thus solve the issue as soon as possible.

      +
    • +
    • +

      If you are interested in rsgrad and want to contribute to the source code, just fork rsgrad and create pull requests at +Pull Requests. We are super grateful if you can contribute +to rsgrad.

      +
    • +
    +

    Acknowledgements

    +
      +
    • Qijing Zheng: The WAVECAR related function are written with the help of this code.
    • +
    • pymatgen and ASE: Some test files are copied from these two repositories.
    • +
    • RustFFT and ndrustfft: +These two crates make wav3d and wav1d become possible.
    • +
    • plotly.rs: This crate makes the visualization possible.
    • +
    + +
    + + +
    +
    + + + +
    + + + + + + + + + + + + + diff --git a/relaxation-example.png b/relaxation-example.png new file mode 100644 index 0000000000000000000000000000000000000000..303386b1358591d49ed9fc1f83f437118afda57d GIT binary patch literal 123467 zcmd?QWpEtLmMtn~mSwTUWJwk?GqWtPn3^>>6w_j9FwVxfKg%c4K zU5~C;v=ez0n})~7)AtP$5VtZCj+x^nyD0>tl7*e?kh<-$p$q27B^{ zb8dn)e^}`-SxJa+H;cIK4^;JK&x+V&|B^+quc0|@Q)OcVmfF!iH?(8ZKc5w>sxW!_ z`yqemiO*AS)YN4J3#{QYWUi~9nprI(m?b(Gy$(Scr`eCNv{!v_c*Ou_Mc7qAqEs*$ zeMEu)+H0szVzl4@YBbc(kSNJfpsR8rGhvQ; zOza8QVNeAHa3C1EsohZrN#J@#K83@SiE#fSF-BPtMj9r(4GGMHqy8cts7yja9)ghD zs7RxV@?FF$*Ynuyn9~`r4enm}F&Eq%$`jHj6g?G*w(mzRIxnhew=5@IOdxho*|jn! z(YHX3-tYGG-f*@73VkU%YxV-K5MM;VNW)4=+rlY&1v}yx$-$+B`iG?pp~^%pFr#<$lMU4j+4akrU>WIC>r*pQ!N;i&@sk4=`qPbc zYU!*A*s(Gq=?B#e9}P0nnsIm6P%EWbIp;^-*s$gil};;-Vil&L?F{iLD@h?iTDEGx;(<1O}1 zEE&-nso!tCt=PBP*V?xm?#jm~3st3bVPebqA;l;DN8G1OP?b^nT1}s}QngfxvwFIO zu~<^2K?zA^Ty;IyUGXM=w-!TpL~=wuqC&M$wZvK6;#cT2z+#gX#fIL7;ex8jOP9vPI$t!O~q{^DPTUl_wN83O!ZtV@{8_emJE%xjQXR 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HcmV?d00001 diff --git a/searcher.js b/searcher.js new file mode 100644 index 0000000..d2b0aee --- /dev/null +++ b/searcher.js @@ -0,0 +1,483 @@ +"use strict"; +window.search = window.search || {}; +(function search(search) { + // Search functionality + // + // You can use !hasFocus() to prevent keyhandling in your key + // event handlers while the user is typing their search. + + if (!Mark || !elasticlunr) { + return; + } + + //IE 11 Compatibility from https://developer.mozilla.org/en-US/docs/Web/JavaScript/Reference/Global_Objects/String/startsWith + if (!String.prototype.startsWith) { + String.prototype.startsWith = function(search, pos) { + return this.substr(!pos || pos < 0 ? 0 : +pos, search.length) === search; + }; + } + + var search_wrap = document.getElementById('search-wrapper'), + searchbar = document.getElementById('searchbar'), + searchbar_outer = document.getElementById('searchbar-outer'), + searchresults = document.getElementById('searchresults'), + searchresults_outer = document.getElementById('searchresults-outer'), + searchresults_header = document.getElementById('searchresults-header'), + searchicon = document.getElementById('search-toggle'), + content = document.getElementById('content'), + + searchindex = null, + doc_urls = [], + results_options = { + teaser_word_count: 30, + limit_results: 30, + }, + search_options = { + bool: "AND", + expand: true, + fields: { + title: {boost: 1}, + body: {boost: 1}, + breadcrumbs: {boost: 0} + } + }, + mark_exclude = [], + marker = new Mark(content), + current_searchterm = "", + URL_SEARCH_PARAM = 'search', + URL_MARK_PARAM = 'highlight', + teaser_count = 0, + + SEARCH_HOTKEY_KEYCODE = 83, + ESCAPE_KEYCODE = 27, + DOWN_KEYCODE = 40, + UP_KEYCODE = 38, + SELECT_KEYCODE = 13; + + function hasFocus() { + return searchbar === document.activeElement; + } + + function removeChildren(elem) { + while (elem.firstChild) { + elem.removeChild(elem.firstChild); + } + } + + // Helper to parse a url into its building blocks. + function parseURL(url) { + var a = document.createElement('a'); + a.href = url; + return { + source: url, + protocol: a.protocol.replace(':',''), + host: a.hostname, + port: a.port, + params: (function(){ + var ret = {}; + var seg = a.search.replace(/^\?/,'').split('&'); + var len = seg.length, i = 0, s; + for (;i': '>', + '"': '"', + "'": ''' + }; + var repl = function(c) { return MAP[c]; }; + return function(s) { + return s.replace(/[&<>'"]/g, repl); + }; + })(); + + function formatSearchMetric(count, searchterm) { + if (count == 1) { + return count + " search result for '" + searchterm + "':"; + } else if (count == 0) { + return "No search results for '" + searchterm + "'."; + } else { + return count + " search results for '" + searchterm + "':"; + } + } + + function formatSearchResult(result, searchterms) { + var teaser = makeTeaser(escapeHTML(result.doc.body), searchterms); + teaser_count++; + + // The ?URL_MARK_PARAM= parameter belongs inbetween the page and the #heading-anchor + var url = doc_urls[result.ref].split("#"); + if (url.length == 1) { // no anchor found + url.push(""); + } + + // encodeURIComponent escapes all chars that could allow an XSS except + // for '. Due to that we also manually replace ' with its url-encoded + // representation (%27). + var searchterms = encodeURIComponent(searchterms.join(" ")).replace(/\'/g, "%27"); + + return '' + result.doc.breadcrumbs + '' + + '' + + teaser + ''; + } + + function makeTeaser(body, searchterms) { + // The strategy is as follows: + // First, assign a value to each word in the document: + // Words that correspond to search terms (stemmer aware): 40 + // Normal words: 2 + // First word in a sentence: 8 + // Then use a sliding window with a constant number of words and count the + // sum of the values of the words within the window. Then use the window that got the + // maximum sum. If there are multiple maximas, then get the last one. + // Enclose the terms in . + var stemmed_searchterms = searchterms.map(function(w) { + return elasticlunr.stemmer(w.toLowerCase()); + }); + var searchterm_weight = 40; + var weighted = []; // contains elements of ["word", weight, index_in_document] + // split in sentences, then words + var sentences = body.toLowerCase().split('. '); + var index = 0; + var value = 0; + var searchterm_found = false; + for (var sentenceindex in sentences) { + var words = sentences[sentenceindex].split(' '); + value = 8; + for (var wordindex in words) { + var word = words[wordindex]; + if (word.length > 0) { + for (var searchtermindex in stemmed_searchterms) { + if (elasticlunr.stemmer(word).startsWith(stemmed_searchterms[searchtermindex])) { + value = searchterm_weight; + searchterm_found = true; + } + }; + weighted.push([word, value, index]); + value = 2; + } + index += word.length; + index += 1; // ' ' or '.' if last word in sentence + }; + index += 1; // because we split at a two-char boundary '. ' + }; + + if (weighted.length == 0) { + return body; + } + + var window_weight = []; + var window_size = Math.min(weighted.length, results_options.teaser_word_count); + + var cur_sum = 0; + for (var wordindex = 0; wordindex < window_size; wordindex++) { + cur_sum += weighted[wordindex][1]; + }; + window_weight.push(cur_sum); + for (var wordindex = 0; wordindex < weighted.length - window_size; wordindex++) { + cur_sum -= weighted[wordindex][1]; + cur_sum += weighted[wordindex + window_size][1]; + window_weight.push(cur_sum); + }; + + if (searchterm_found) { + var max_sum = 0; + var max_sum_window_index = 0; + // backwards + for (var i = window_weight.length - 1; i >= 0; i--) { + if (window_weight[i] > max_sum) { + max_sum = window_weight[i]; + max_sum_window_index = i; + } + }; + } else { + max_sum_window_index = 0; + } + + // add around searchterms + var teaser_split = []; + var index = weighted[max_sum_window_index][2]; + for (var i = max_sum_window_index; i < max_sum_window_index+window_size; i++) { + var word = weighted[i]; + if (index < word[2]) { + // missing text from index to start of `word` + teaser_split.push(body.substring(index, word[2])); + index = word[2]; + } + if (word[1] == searchterm_weight) { + teaser_split.push("") + } + index = word[2] + word[0].length; + teaser_split.push(body.substring(word[2], index)); + if (word[1] == searchterm_weight) { + teaser_split.push("") + } + }; + + return teaser_split.join(''); + } + + function init(config) { + results_options = config.results_options; + search_options = config.search_options; + searchbar_outer = config.searchbar_outer; + doc_urls = config.doc_urls; + searchindex = elasticlunr.Index.load(config.index); + + // Set up events + searchicon.addEventListener('click', function(e) { searchIconClickHandler(); }, false); + searchbar.addEventListener('keyup', function(e) { searchbarKeyUpHandler(); }, false); + document.addEventListener('keydown', function(e) { globalKeyHandler(e); }, false); + // If the user uses the browser buttons, do the same as if a reload happened + window.onpopstate = function(e) { doSearchOrMarkFromUrl(); }; + // Suppress "submit" events so the page doesn't reload when the user presses Enter + document.addEventListener('submit', function(e) { e.preventDefault(); }, false); + + // If reloaded, do the search or mark again, depending on the current url parameters + doSearchOrMarkFromUrl(); + } + + function unfocusSearchbar() { + // hacky, but just focusing a div only works once + var tmp = document.createElement('input'); + tmp.setAttribute('style', 'position: absolute; opacity: 0;'); + searchicon.appendChild(tmp); + tmp.focus(); + tmp.remove(); + } + + // On reload or browser history backwards/forwards events, parse the url and do search or mark + function doSearchOrMarkFromUrl() { + // Check current URL for search request + var url = parseURL(window.location.href); + if (url.params.hasOwnProperty(URL_SEARCH_PARAM) + && url.params[URL_SEARCH_PARAM] != "") { + showSearch(true); + searchbar.value = decodeURIComponent( + (url.params[URL_SEARCH_PARAM]+'').replace(/\+/g, '%20')); + searchbarKeyUpHandler(); // -> doSearch() + } else { + showSearch(false); + } + + if (url.params.hasOwnProperty(URL_MARK_PARAM)) { + var words = decodeURIComponent(url.params[URL_MARK_PARAM]).split(' '); + marker.mark(words, { + exclude: mark_exclude + }); + + var markers = document.querySelectorAll("mark"); + function hide() { + for (var i = 0; i < markers.length; i++) { + markers[i].classList.add("fade-out"); + window.setTimeout(function(e) { marker.unmark(); }, 300); + } + } + for (var i = 0; i < markers.length; i++) { + markers[i].addEventListener('click', hide); + } + } + } + + // Eventhandler for keyevents on `document` + function globalKeyHandler(e) { + if (e.altKey || e.ctrlKey || e.metaKey || e.shiftKey || e.target.type === 'textarea' || e.target.type === 'text') { return; } + + if (e.keyCode === ESCAPE_KEYCODE) { + e.preventDefault(); + searchbar.classList.remove("active"); + setSearchUrlParameters("", + (searchbar.value.trim() !== "") ? "push" : "replace"); + if (hasFocus()) { + unfocusSearchbar(); + } + showSearch(false); + marker.unmark(); + } else if (!hasFocus() && e.keyCode === SEARCH_HOTKEY_KEYCODE) { + e.preventDefault(); + showSearch(true); + window.scrollTo(0, 0); + searchbar.select(); + } else if (hasFocus() && e.keyCode === DOWN_KEYCODE) { + e.preventDefault(); + unfocusSearchbar(); + searchresults.firstElementChild.classList.add("focus"); + } else if (!hasFocus() && (e.keyCode === DOWN_KEYCODE + || e.keyCode === UP_KEYCODE + || e.keyCode === SELECT_KEYCODE)) { + // not `:focus` because browser does annoying scrolling + var focused = searchresults.querySelector("li.focus"); + if (!focused) return; + e.preventDefault(); + if (e.keyCode === DOWN_KEYCODE) { + var next = focused.nextElementSibling; + if (next) { + focused.classList.remove("focus"); + next.classList.add("focus"); + } + } else if (e.keyCode === UP_KEYCODE) { + focused.classList.remove("focus"); + var prev = focused.previousElementSibling; + if (prev) { + prev.classList.add("focus"); + } else { + searchbar.select(); + } + } else { // SELECT_KEYCODE + window.location.assign(focused.querySelector('a')); + } + } + } + + function showSearch(yes) { + if (yes) { + search_wrap.classList.remove('hidden'); + searchicon.setAttribute('aria-expanded', 'true'); + } else { + search_wrap.classList.add('hidden'); + searchicon.setAttribute('aria-expanded', 'false'); + var results = searchresults.children; + for (var i = 0; i < results.length; i++) { + results[i].classList.remove("focus"); + } + } + } + + function showResults(yes) { + if (yes) { + searchresults_outer.classList.remove('hidden'); + } else { + searchresults_outer.classList.add('hidden'); + } + } + + // Eventhandler for search icon + function searchIconClickHandler() { + if (search_wrap.classList.contains('hidden')) { + showSearch(true); + window.scrollTo(0, 0); + searchbar.select(); + } else { + showSearch(false); + } + } + + // Eventhandler for keyevents while the searchbar is focused + function searchbarKeyUpHandler() { + var searchterm = searchbar.value.trim(); + if (searchterm != "") { + searchbar.classList.add("active"); + doSearch(searchterm); + } else { + searchbar.classList.remove("active"); + showResults(false); + removeChildren(searchresults); + } + + setSearchUrlParameters(searchterm, "push_if_new_search_else_replace"); + + // Remove marks + marker.unmark(); + } + + // Update current url with ?URL_SEARCH_PARAM= parameter, remove ?URL_MARK_PARAM and #heading-anchor . + // `action` can be one of "push", "replace", "push_if_new_search_else_replace" + // and replaces or pushes a new browser history item. + // "push_if_new_search_else_replace" pushes if there is no `?URL_SEARCH_PARAM=abc` yet. + function setSearchUrlParameters(searchterm, action) { + var url = parseURL(window.location.href); + var first_search = ! url.params.hasOwnProperty(URL_SEARCH_PARAM); + if (searchterm != "" || action == "push_if_new_search_else_replace") { + url.params[URL_SEARCH_PARAM] = searchterm; + delete url.params[URL_MARK_PARAM]; + url.hash = ""; + } else { + delete url.params[URL_MARK_PARAM]; + delete url.params[URL_SEARCH_PARAM]; + } + // A new search will also add a new history item, so the user can go back + // to the page prior to searching. A updated search term will only replace + // the url. + if (action == "push" || (action == "push_if_new_search_else_replace" && first_search) ) { + history.pushState({}, document.title, renderURL(url)); + } else if (action == "replace" || (action == "push_if_new_search_else_replace" && !first_search) ) { + history.replaceState({}, document.title, renderURL(url)); + } + } + + function doSearch(searchterm) { + + // Don't search the same twice + if (current_searchterm == searchterm) { return; } + else { current_searchterm = searchterm; } + + if (searchindex == null) { return; } + + // Do the actual search + var results = searchindex.search(searchterm, search_options); + var resultcount = Math.min(results.length, results_options.limit_results); + + // Display search metrics + searchresults_header.innerText = formatSearchMetric(resultcount, searchterm); + + // Clear and insert results + var searchterms = searchterm.split(' '); + removeChildren(searchresults); + for(var i = 0; i < resultcount ; i++){ + var resultElem = document.createElement('li'); + resultElem.innerHTML = formatSearchResult(results[i], searchterms); + searchresults.appendChild(resultElem); + } + + // Display results + showResults(true); + } + + fetch(path_to_root + 'searchindex.json') + .then(response => response.json()) + .then(json => init(json)) + .catch(error => { // Try to load searchindex.js if fetch failed + var script = document.createElement('script'); + script.src = path_to_root + 'searchindex.js'; + script.onload = () => init(window.search); + document.head.appendChild(script); + }); + + // Exported functions + search.hasFocus = hasFocus; +})(window.search); diff --git a/searchindex.js b/searchindex.js new file mode 100644 index 0000000..71cd630 --- /dev/null +++ b/searchindex.js @@ -0,0 +1 @@ +Object.assign(window.search, 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is an open-source command-line tool to help VASP players play better with VASP. rsgrad is written proudly in pure Rust . Now rsgrad provides several features: Track the relaxation and MD (molecular dynamics) progress; Calculate and visualize the DOS (density of states) and pDOS (projected DOS); Plot and visualize the band structure and fat band structure; Save the frames with given MD or relaxation trajectory; Calculate charge density difference; Analyze the vibration eigen values and eigen vectors; Plot the wave function at given bands in real-space; Plot the wave function at given bands in real-space then integrate it over specified plane; Plot and visualize the work function; Split POSCAR ; Convert between fractional coordinates and Cartesian coordinates; Format POSCAR ; Generate POTCAR according to POSCAR ; Calculate Transition Dipole Moment from WAVECAR ; Calculate band gap and print locations of CBM and VBM. Convert one quantity to other units that representing same energy. Wish you have a good time with rsgrad ^_^","breadcrumbs":"Introduction » Introduction","id":"0","title":"Introduction"},"1":{"body":"There are two ways to install rsgrad, downloading the pre-built binaries and building from scratch.","breadcrumbs":"Installation » Installation","id":"1","title":"Installation"},"10":{"body":"This command can calculate total DOS only. To calculate projected DOS, use configuration instead (see next section). $ rsgrad dos\n[2022-07-14T18:42:55Z INFO rsgrad::commands::dos] Parsing PROCAR file \"./PROCAR\"\n[2022-07-14T18:42:55Z INFO rsgrad::commands::dos] Parsing OUTCAR file \"./OUTCAR\" for Fermi level\n[2022-07-14T18:42:55Z INFO rsgrad::commands::dos] Found Fermi level = -1.9018, eigenvalues will be shifted.\n[2022-07-14T18:42:55Z INFO rsgrad::commands::dos] Plotting Total DOS ...\n[2022-07-14T18:42:55Z INFO rsgrad::commands::dos] Total DOS plot time usage: 29.055µs\n[2022-07-14T18:42:55Z INFO rsgrad::commands::dos] Writing DOS plot to \"dos.html\"\n[2022-07-14T18:42:55Z INFO rsgrad::commands::dos] Writing raw DOS data to \"dos_raw.txt\"\n[2022-07-14T18:42:55Z INFO rsgrad] Time used: 124.426652ms The output html should be like something in the following","breadcrumbs":"Density of States » Example (without configuration file)","id":"10","title":"Example (without configuration file)"},"11":{"body":"To plot multiple PDOS, using configuration file is suggested. With the configuration (pdos.toml) in the following method = \"Gaussian\"\nsigma = 0.05\nprocar = \"PROCAR\"\noutcar = \"OUTCAR\"\ntxtout = \"dos_raw.txt\"\nhtmlout = \"dos.html\"\ntotdos = true\nfill = true\nxlim = [-1, 6] [pdos.Benzene]\natoms = \"37..48\" [pdos.AgSurf]\natoms = \"3 6 10 14 21 23 25 33 36\" then rsgrad dos -c pdos.toml $ rsgrad dos -c pdos.toml\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Reading PDOS configuration from Some(\"pdos.toml\")\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Parsing PROCAR file \"PROCAR\"\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Parsing OUTCAR file \"OUTCAR\" for Fermi level\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Found Fermi level = -1.9018, eigenvalues will be shifted.\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Plotting Total DOS ...\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Total DOS plot time usage: 42.878µs\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Plotting PDOS ...\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] PDOS plot time usage: 6.223076ms\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Writing DOS plot to \"dos.html\"\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Writing raw DOS data to \"dos_raw.txt\"\n[2022-07-14T18:43:34Z INFO rsgrad] Time used: 61.982958ms you will get something in the following","breadcrumbs":"Density of States » Example (with configuration file)","id":"11","title":"Example (with configuration file)"},"12":{"body":"rsgrad can write the raw data of plot by setting txtout (dos_raw.txt by default). The organization of it shows the energy, total DOS and projected dos respectively: # E-Ef TotDOS Benzene AgSurf\n... -7.921938 0.002969 0.002158 0.000004 -7.899296 0.016032 0.011655 0.000019 -7.876654 0.070713 0.051408 0.000085 -7.854012 0.254749 0.185212 0.000307 -7.831371 0.749573 0.544998 0.000910 -7.808729 1.801235 1.309709 0.002202 -7.786087 3.534640 2.570233 0.004349 -7.763446 5.663677 4.118580 0.007011 -7.740804 7.409459 5.388357 0.009226 -7.718162 7.913407 5.755104 0.009908 -7.695520 6.898991 5.017578 0.008683 -7.672879 4.909619 3.570876 0.006208 -7.650237 2.854880 2.076535 0.003622 -7.627595 1.373037 0.998928 0.001724 -7.604953 0.617183 0.449840 0.000672 -7.582312 0.494734 0.362904 0.000231 -7.559670 0.977346 0.718873 0.000173 -7.537028 2.169137 1.593003 0.000599 -7.514387 4.077126 2.981347 0.002383 -7.491745 6.295459 4.560748 0.007858 -7.469103 8.005154 5.685401 0.021128\n... The first line shows the labels of each series and have a hastag # in the beginning in order to let numpy.loadtxt can read it directly. Then you can throw it into other plotters like Excel, Matplotlib, OriginPro GnuPlot etc. and do whatever fancy things you prefer.","breadcrumbs":"Density of States » Usage of txtout","id":"12","title":"Usage of txtout"},"13":{"body":"rsgrad band can plot the band structure from PROCAR and OUTCAR .","breadcrumbs":"Band Structure » Band Structure","id":"13","title":"Band Structure"},"14":{"body":"$ rsgrad band -h\nrsgrad-band\nPlot bandstructure and projected bandstructure USAGE: rsgrad band [OPTIONS] OPTIONS: -c, --config Band structure plot configuration file path --colormap [default: jet] --efermi Set the E-fermi given from SCF's OUTCAR and it will be the reference energy level --gen-template Generate band structure plot configuration template -h, --help Print help information --htmlout Save the band structure plot as HTML [default: band.html] -k, --kpoint-labels Symbols for high symmetry points on the kpoint path --ncl-spinor [possible values: X, Y, Z] --outcar OUTCAR path [default: ./OUTCAR] --procar PROCAR path [default: ./PROCAR] --show Open the browser and show the plot immediately --to-inline-html Render the plot and print the rendered code to stdout --txtout-prefix Save the raw data of band structure [default: band_raw] --ylim Set the y-range of the plot [default: \"-1 6\"]","breadcrumbs":"Band Structure » Help Message","id":"14","title":"Help Message"},"15":{"body":"# rsgrad Band plot configuration in toml format.\n# multiple tokens inside string are seperated by whitespace, if you # kpoint-labels = [\"G\", \"K\", \"M\", \"G\"] # should be consistant with the boundaries in KPOINTS\nprocar = \"PROCAR\"\noutcar = \"OUTCAR\"\ntxtout-prefix = \"band_raw\"\nhtmlout = \"band.html\"\n# segment-ranges = [[1, 40], [41, 80], [81, 120]] # if commented, rsgrad will find the boundaries by judging if k[i] == k[i+1]\n# ncl-spinor = \"Z\" # for vasp_ncl calculation\n# colormap = \"jet\" # the colormap specified to plot ncl-band\n# efermi = 0.0 # if commented, rsgrad will read the efermi from OUTCAR, but if may be slightly different from scf's\n# ylim = [-1, 6] # [pband.plot1]\n# spins = \"up down\" # \"u d\" are also ok, for ncl system, \"tot x y z\" are available\n# atoms = \"1 3..7 -1\" # which atoms to project on, if commented, all atoms are selected\n# orbits = \"s px dxy\" # which orbits to project on, if commented, all orbits are selected\n# color = \"red\" # the color of marker","breadcrumbs":"Band Structure » Configuration Template","id":"15","title":"Configuration Template"},"16":{"body":"Simply run rsgrad band can plot the band structure. $ rsgrad band\n[2022-07-14T18:40:18Z INFO rsgrad::commands::band] Reading fermi level and lattice data from \"./OUTCAR\"\n[2022-07-14T18:40:18Z INFO rsgrad::commands::band] Reading band data from \"./PROCAR\"\n[2022-07-14T18:40:18Z INFO rsgrad::commands::band] Found Fermi level: 12.7626, shifting eigenvalues ...\n[2022-07-14T18:40:18Z WARN rsgrad::commands::band] No k-point labels found, use empty labels instead\n[2022-07-14T18:40:18Z INFO rsgrad::commands::band] Plotting raw bands ...\n[2022-07-14T18:40:18Z INFO rsgrad::commands::band] Writing Bandstructure to \"band.html\"\n[2022-07-14T18:40:18Z INFO rsgrad::commands::band] Writing raw band data to \"band_raw.txt\"\n[2022-07-14T18:40:18Z INFO rsgrad] Time used: 79.644034ms There may be a warning reminds you provide the labels of each high-symmetry point. rsgrad identifies high-symmetry points by calculate the difference of consecutive k-points. If the difference equals zero, these two points are labelled as one high-symmetry point. For example: ...\nk-point 38 : 0.0000 0.0256 0.0000\nk-point 39 : 0.0000 0.0128 0.0000\nk-point 40 : 0.0000 0.0000 0.0000\nk-point 41 : 0.0000 0.0000 0.0000\nk-point 42 : -0.0085 0.0171 0.0000\nk-point 43 : -0.0171 0.0342 0.0000\n... k-point 40 and k-point 41 are same, thus be identified as one high-symmetry point. Each of the high-symmetry points need a label. You may either left the --kpoint-labels empty or provide the correct labels seperated by white spaces. Sometimes it may produce wrong band structure due to the special k-point path like kpoints for bandstructure L-G-X-U K-G 10\nline\nreciprocal 0.50000 0.50000 0.50000 1 0.00000 0.00000 0.00000 1 0.00000 0.00000 0.00000 1 0.00000 0.50000 0.50000 1 0.00000 0.50000 0.50000 1 0.25000 0.62500 0.62500 1 0.37500 0.7500 0.37500 1 0.00000 0.00000 0.00000 1 The end of third segment (0.25000, 0.62500, 0.62500) and the beginning of fourth segment (0.37500, 0.7500, 0.37500) are not consistent, which produces wrong k-path, leading to wrong band structure: To solve this issue, you need to try the configuration file.","breadcrumbs":"Band Structure » Example (without configuration file)","id":"16","title":"Example (without configuration file)"},"17":{"body":"With the configuration in the following kpoint-labels = [\"L\", \"Γ\", \"X\", \"U|K\", \"Γ\"]\nprocar = \"PROCAR\"\noutcar = \"OUTCAR\"\ntxtout-prefix = \"pband_raw\"\nhtmlout = \"pband.html\"\nsegment-ranges = [[1, 10], [11, 20], [21, 30], [31, 40]] [pband.Si-p-orbit]\norbits = \"px py pz\"\ncolor = \"red\" and run rsgrad -c pband.toml $ rsgrad band -c pband.toml\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Reading porjected band configuration fomr Some(\"pband.toml\")\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Reading fermi level and lattice data from \"OUTCAR\"\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Reading band data from \"PROCAR\"\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Found Fermi level: 12.7626, shifting eigenvalues ...\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Plotting raw bands ...\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Plotting projected bands ...\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Writting projected band Si-p-orbit to \"pband_raw_Si-p-orbit.txt\" ...\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Projected band plot time usage: 1.220401ms\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Writing Bandstructure to \"band.html\"\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Writing raw band data to \"pband_raw.txt\"\n[2022-07-14T18:41:02Z INFO rsgrad] Time used: 77.804627ms then it produces","breadcrumbs":"Band Structure » Example (with configuration file)","id":"17","title":"Example (with configuration file)"},"18":{"body":"For the results produced by vasp_ncl, rsgrad supports plotting the \\(z\\) (\\(x\\) and \\(y\\) are also OK) projection to analyze the spin angular moments. kpoint-labels = [\"M\", \"Γ\", \"K\", \"M\"]\nprocar = \"PROCAR\"\noutcar = \"OUTCAR\"\ntxtout-prefix = \"band_ncl_raw\"\nhtmlout = \"band_ncl.html\"\nsegment-ranges = [[81, 120], [1, 40], [41, 80]]\nncl-spinor = \"Z\"\ncolormap = \"jet\" then it produces","breadcrumbs":"Band Structure » Example (for non-collinear system)","id":"18","title":"Example (for non-collinear system)"},"19":{"body":"rsgrad reads OUTCAR then provide some operations in the following. Save selected steps as XDATCAR . Save selected steps as POSCAR files. Save selected steps as XSF files. With XSF , VESTA can show the force vectors on every atom.","breadcrumbs":"Trajectory » Trajectory","id":"19","title":"Trajectory"},"2":{"body":"We provide the pre-built binaries at GitHub Release . There are four platforms we support with pre-built binaries rsgrad--linux-x86_64-musl.tar.gz: Statically linked binary. Can run on almost all Linux distros. However, the musl libc may have performance issues in some scenes like wave1d, wav3d etc. rsgrad--linux-x86_64.tar.gz: Dynamically linked against glibc and other fundamental system libraries. For the binaries with 0.3.6_ci-test or upper version, they can run on most Linux distros (e.g. CentOS 7, Ubuntu 18.04). If it still complains with message like /lib64/libc.so.6: version 'GLIBC_2.18' not found, just switch to -musl binary or build from scratch. rsgrad--macos-x86_64.tar.gz: Binary for macOS (Intel). rsgrad is developed on macOS 13, which means you are don't need to worry about the availability if you are using macOS. rsgrad--macos-aarch64.tar.gz: Binary for macOS (Apple Silicon). rsgrad--windows-x86_64.zip: Binary for Windows system. We have no plan to support 32-bit systems. Download the corresponding binary and put it in $PATH (or %PATH% on Windows), and have fun!","breadcrumbs":"Installation » Download the Binary from GitHub Release","id":"2","title":"Download the Binary from GitHub Release"},"20":{"body":"$ rsgrad traj --help\nrsgrad-traj\nOperations about relaxation/MD trajectory. POSCAR is needed if you want to preserve the constraints when saving frames to POSCAR. USAGE: rsgrad traj [OPTIONS] [--] [OUTCAR] ARGS: Specify the input OUTCAR file [default: ./OUTCAR] OPTIONS: --cartesian Save to POSCAR in cartesian coordinates, the coordinates written is direct/fractional by default -d, --save-as-xdatcar Save whole trajectory in XDATCAR format -h, --help Print help information -i, --select-indices ... Selects the indices to operate. Step indices start from '1', if '0' is given, all the structures will be selected. Step indices can be negative, where negative index means counting reversely. E.g. \"-i -2 -1 1 2 3\" means selecting the last two and first three steps. --no-add-symbol-tags Don't add chemical symbol to each line of coordinates --no-preserve-constraints Don't preverse constraints when saving trajectory to POSCAR -p, --poscar Specify the input POSCAR file [default: ./POSCAR] -s, --save-as-poscar Save selected steps as POSCARs --save-in Define where the files would be saved [default: .] -x, --save-as-xsfs Saves each selected modes to XSF file, this file includes each atom's force information","breadcrumbs":"Trajectory » Help Message","id":"20","title":"Help Message"},"21":{"body":"Take the last step and save as XSF file rsgrad traj -i -1 -x $ rsgrad traj -i -1 -x\n[2022-07-14T18:37:35Z INFO rsgrad::commands::traj] Parsing file \"./OUTCAR\" and \"./POSCAR\"\n[2022-07-14T18:37:35Z INFO rsgrad::vasp_parsers::outcar] Saving ionic step to \"./step_0003.xsf\" ...\n[2022-07-14T18:37:35Z INFO rsgrad] Time used: 11.223561ms Take the first step and save as POSCAR file rsgrad traj -i 1 -s $ rsgrad traj -i 1 -s\n[2022-07-14T18:38:51Z INFO rsgrad::commands::traj] Parsing file \"./OUTCAR\" and \"./POSCAR\"\n[2022-07-14T18:38:51Z INFO rsgrad::vasp_parsers::outcar] Saving trajectory step # 1 to \"./POSCAR_00001.vasp\" ...\n[2022-07-14T18:38:51Z INFO rsgrad] Time used: 8.64197ms","breadcrumbs":"Trajectory » Examples","id":"21","title":"Examples"},"22":{"body":"rsgrad chgdiff can calculate the charge density difference from CHGCAR files: $$ \\Delta \\rho = \\rho_{A+B} - (\\rho_A + \\rho_B) $$ Where \\(\\rho_{A+B}\\), \\(\\rho_A\\) and \\(\\rho_B\\) are the charge densities of total structure, A structure and B structure, respectively. You may also need rsgrad poscar --split ... to generate the structure of A and B from A+B.","breadcrumbs":"Charge Density Difference » Charge Density Difference","id":"22","title":"Charge Density Difference"},"23":{"body":"$ rsgrad chgdiff --help\nrsgrad-chgdiff\nCalculate charge density difference. The operation is performed by `chgdiff = chgcar_ab - (chgcar_a + chgcar_b)`. USAGE: rsgrad chgdiff [OPTIONS] ARGS: The CHGCAR of A+B system The CHGCAR of A system The CHGCAR of B system OPTIONS: -h, --help Print help information -o, --output The output charge density difference file path [default: CHGDIFF.vasp]","breadcrumbs":"Charge Density Difference » Help message","id":"23","title":"Help message"},"24":{"body":"You need to calculate the electronic structure of the three structures (A+B, A and B) first, then rsgrad chgdiff CHGCAR_A+B CHGCAR_A CHGCAR_B like $ rsgrad chgdiff ../scf/CHGCAR Ag/CHGCAR noAg/CHGCAR\n[2022-07-14T18:34:59Z INFO rsgrad::commands::chgdiff] Reading charge density from \"Ag/CHGCAR\"\n[2022-07-14T18:34:59Z INFO rsgrad::commands::chgdiff] Reading charge density from \"noAg/CHGCAR\"\n[2022-07-14T18:34:59Z INFO rsgrad::commands::chgdiff] Reading charge density from \"../scf/CHGCAR\"\n[2022-07-14T18:35:06Z INFO rsgrad::commands::chgdiff] Calculating charge density difference by `CHGDIFF = \"../scf/CHGCAR\" - (\"Ag/CHGCAR\" + \"noAg/CHGCAR\")`\n[2022-07-14T18:35:06Z INFO rsgrad::commands::chgdiff] Writing charge difference to \"CHGDIFF.vasp\"\n[2022-07-14T18:35:10Z INFO rsgrad] Time used: 11.189259653s finally use VESTA to visualize the data","breadcrumbs":"Charge Density Difference » Example","id":"24","title":"Example"},"25":{"body":"For systems enabled vibration calculation (phonon at Γ point only), rsgrad vib can Print the phonon eigenvalues; Save the phonon eigenvectors; Modulate the ground-state according to specified modes.","breadcrumbs":"Vibration » Vibration","id":"25","title":"Vibration"},"26":{"body":"$ rsgrad vib --help\nrsgrad-vib\nTracking vibration information. For systems enabled vibration mode calculation, this command can extract phonon eigenvalues and\nphonon eigenvectors at Gamma point. USAGE: rsgrad vib [OPTIONS] [--] [OUTCAR] ARGS: Specify the input OUTCAR file [default: ./OUTCAR] OPTIONS: -a, --amplitude Modulation amplitude coefficient, to avoid precision issue, abs(amplitude) >= 0.01 should be satisfied [default: 0.1] -c, --cartesian Catesian coordinate is used when writting POSCAR. Fractional coordinate is used by default -h, --help Print help information -i, --select-indices ... Selects the mode indices to operate. Step indices start from '1', if '0' is given, all the structures will be selected. Step indices can be negative, where negative index means counting reversely. E.g. \"-i -2 -1 1 2 3\" means selecting the last two and first three steps. -l, --list Shows vibration modes in brief -m, --modulate Modulate the ground-state POSCAR with respect to a certern vibration frequencies -p, --poscar Specify the input POSCAR file, the consntraints info is needed [default: ./POSCAR] --save-in Define where the files would be saved [default: .] -x, --save-as-xsfs Saves each selected modes to XSF file","breadcrumbs":"Vibration » Help Message","id":"26","title":"Help Message"},"27":{"body":"Print the phonon eigenvalues; Save the phonon eigenvectors; $ rsgrad vib -i {1..3} {-3..-1} -x\n[2022-07-14T18:32:49Z INFO rsgrad::commands::vib] Parsing file \"./OUTCAR\"\n[2022-07-14T18:32:49Z INFO rsgrad::vasp_parsers::outcar] Saving mode # 1 as \"./mode_0001_3682.13cm-1.xsf\" ...\n[2022-07-14T18:32:49Z INFO rsgrad::vasp_parsers::outcar] Saving mode # 3 as \"./mode_0003_3679.99cm-1.xsf\" ...\n[2022-07-14T18:32:49Z INFO rsgrad::vasp_parsers::outcar] Saving mode # 44 as \"./mode_0044_0010.79cm-1_imag.xsf\" ...\n[2022-07-14T18:32:49Z INFO rsgrad::vasp_parsers::outcar] Saving mode # 43 as \"./mode_0043_0007.12cm-1_imag.xsf\" ...\n[2022-07-14T18:32:49Z INFO rsgrad::vasp_parsers::outcar] Saving mode # 2 as \"./mode_0002_3680.83cm-1.xsf\" ...\n[2022-07-14T18:32:49Z INFO rsgrad::vasp_parsers::outcar] Saving mode # 45 as \"./mode_0045_0047.20cm-1_imag.xsf\" ...\n[2022-07-14T18:32:49Z INFO rsgrad] Time used: 109.566967ms Modulate the ground-state according to specified modes. $ rsgrad vib -i {-3..-1} --modulate --amplitude 0.1\n[2022-07-14T18:31:41Z INFO rsgrad::commands::vib] Parsing file \"./OUTCAR\"\n[2022-07-14T18:31:41Z INFO rsgrad::vasp_parsers::outcar] Saving modulated POSCAR of mode # 43 with amplitude coeff 0.100 as \"./mode_0043_0007.12cm-1_0.100_imag.vasp\" ...\n[2022-07-14T18:31:41Z INFO rsgrad::vasp_parsers::outcar] Saving modulated POSCAR of mode # 44 with amplitude coeff 0.100 as \"./mode_0044_0010.79cm-1_0.100_imag.vasp\" ...\n[2022-07-14T18:31:41Z INFO rsgrad::vasp_parsers::outcar] Saving modulated POSCAR of mode # 45 with amplitude coeff 0.100 as \"./mode_0045_0047.20cm-1_0.100_imag.vasp\" ...\n[2022-07-14T18:31:41Z INFO rsgrad] Time used: 202.629805ms","breadcrumbs":"Vibration » Example","id":"27","title":"Example"},"28":{"body":"Main functions of rsgrad wav3d List the brief information of WAVECAR ; Save the selected wavefunction to .vasp file.","breadcrumbs":"Wavefunction 3D » Wavefunction 3D","id":"28","title":"Wavefunction 3D"},"29":{"body":"$ rsgrad wav3d --help\nPlot wavefunction in realspace, and save it as '.vasp' file Usage: rsgrad wav3d [OPTIONS] Options: -w, --wavecar WAVECAR file name [default: ./WAVECAR] -p, --poscar POSCAR filename, POSCAR is needed to get the real-space wavefunction [default: ./POSCAR] -s, --ispins [...] Select spin index, starting from 1 [default: 1] -k, --ikpoints [...] Select kpoint index, starting from 1. You can input ranges directly: `-k 1..4 5..10` [default: 1] -b, --ibands [...] Select band index, starting from 1. You can input ranges directly: `-b 1..4 5..10` -l, --list List the brief info of current WAVECAR -d, --detail Show the eigen values and band occupations of current WAVECAR. This flag should be used with `--list` --gamma-half Gamma Half direction of WAVECAR. You need to set this to 'x' or 'z' when processing WAVECAR produced by `vasp_gam` [possible values: x, z] --ngrid Grid size for realspace wavefunction, 3 numbers are required, i.e. NGXF NGYF and NGZF. If this argument is left empty, NG_F will be set as NG_F=2*NG_. Be aware that NG_F must be greater than or at least equal to corresponding NG_. -o, --output-parts [...] Specify output part of the wavefunction. Detailed message: - normsquared/ns: Perform `ρ(r) = |ѱ(r)|^2` action to get the spatial distribution of selected band. - real/re: Real part of the wavefunction, suffix '_re.vasp' is added to the output filename. - imag/im: Imaginary part of the wavefunction, suffix '_im.vasp' is added to the output filename. - reim: Output both real part and imaginary parts of the wavefunction. - uns/dns: Perform `ρ(r) = |ѱ(r)|^2` for spinor up/down only. **Note: this option works for `ncl` WAVECAR only.** [possible values: normsquared, ns, uns, dns, real, re, imag, im, reim] --prefix Prefix of output filename [default: wav] -e, --show-eigs-suffix Add eigen value suffix to the filename --sum-chgs Perform sum-up of the charge densities for selected bands. With this flag open, only `normsquared` or `ns` or `uns` or `dns` are allowed for the `-o`/`--output-parts` option. IMPORTANT NOTES: - The prefix for output filename `sum-prefix` is also required and has no default prefix. - The individual charge densities will not be saved to corresponding '.vasp' files if this flag is on. --sum-prefix Specify the output file for the summed charge densities. This argument is required if `sum_chgs` is on. -h, --help Print help (see a summary with '-h')","breadcrumbs":"Wavefunction 3D » Help Message","id":"29","title":"Help Message"},"3":{"body":"The build requires Internet accessibility. If you haven't installed Rust toolchain, run curl --proto '=https' --tlsv1.2 -sSf https://sh.rustup.rs | sh and follow the instructions to configure it. When you finished the toolchain installation, you should be able to run cargo in command-line. Detailed instructions can be found here . If you have installed Rust toolchain already, just run cargo install --git https://github.com/Ionizing/rsgrad. Several minutes later, the rsgrad should be installed to ~/.cargo/bin, no need to modify the $PATH (or %PATH% on Windows).","breadcrumbs":"Installation » Build from Scratch","id":"3","title":"Build from Scratch"},"30":{"body":"List the brief information of WAVECAR $ rsgrad wav3d -l [2022-07-14T09:19:51Z INFO rsgrad::commands::wav3d] Reading WAVECAR: \"./WAVECAR\"\nLENGTH = 54145104\nRECLEN = 1388336\nTYPE = Standard\nNSPIN = 1\nNKPTS = 1\nNBANDS = 36\nENCUT = 450.000\nEFERMI = -5.368\nVOLUME = 8000.000\nNGRID = [ 71, 71, 71]\nNPLWS = [173541]\nACELL = [[ 20.000, 0.000, 0.000], [ 0.000, 20.000, 0.000], [ 0.000, 0.000, 20.000]]\nBCELL = [[ 0.050, 0.000, 0.000], [ 0.000, 0.050, 0.000], [ 0.000, 0.000, 0.050]] [2022-07-14T09:19:51Z INFO rsgrad] Time used: 160.337862ms if you want the band eigen values information $ rsgrad wav3d -ld ...\n\n... ISPIN: 1 IKPOINT: 1 IBAND: 1 E-Efermi: -19.991 Occupation: 1.000\nISPIN: 1 IKPOINT: 1 IBAND: 2 E-Efermi: -18.141 Occupation: 1.000\nISPIN: 1 IKPOINT: 1 IBAND: 3 E-Efermi: -18.141 Occupation: 1.000\nISPIN: 1 IKPOINT: 1 IBAND: 4 E-Efermi: -16.418 Occupation: 1.000\nISPIN: 1 IKPOINT: 1 IBAND: 5 E-Efermi: -15.534 Occupation: 1.000\nISPIN: 1 IKPOINT: 1 IBAND: 6 E-Efermi: -15.532 Occupation: 1.000\nISPIN: 1 IKPOINT: 1 IBAND: 7 E-Efermi: -10.662 Occupation: 1.000\nISPIN: 1 IKPOINT: 1 IBAND: 8 E-Efermi: -10.661 Occupation: 1.000\n... Save the selected wavefunction to .vasp file $ rsgrad wav3d -b {10..20} -o ns -e [2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Reading WAVECAR: \"./WAVECAR\"\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Reading POSCAR: \"./POSCAR\"\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 10 ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 13 ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 11 ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 14 ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 12 ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 15 ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-13_-5.740eV.vasp\" ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-15_-5.601eV.vasp\" ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-14_-5.728eV.vasp\" ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-10_-8.376eV.vasp\" ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-11_-7.385eV.vasp\" ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-12_-7.380eV.vasp\" ...\n[2022-07-14T09:23:08Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 18 ...\n[2022-07-14T09:23:08Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 19 ...\n[2022-07-14T09:23:09Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-18_-3.514eV.vasp\" ...\n[2022-07-14T09:23:09Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 16 ...\n[2022-07-14T09:23:09Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 20 ...\n[2022-07-14T09:23:09Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-19_-3.265eV.vasp\" ...\n[2022-07-14T09:23:09Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 17 ...\n[2022-07-14T09:23:10Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-16_-5.477eV.vasp\" ...\n[2022-07-14T09:23:10Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-17_-3.546eV.vasp\" ...\n[2022-07-14T09:23:10Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-20_-0.701eV.vasp\" ...\n[2022-07-14T09:23:11Z INFO rsgrad] Time used: 5.484733549s Open the .vasp in VESTA rsgrad wav3d supports extracting multiple bands at the same time, and the processes executed in parallel, which can save a lot of time.","breadcrumbs":"Wavefunction 3D » Example","id":"30","title":"Example"},"31":{"body":"This command is similar to rsgrad wav3d. The only difference is that wav1d integrates the wavefunction over specified plane, and produces the averaged one dimensional wavefunction. This command is useful when you are looking for image potential states.","breadcrumbs":"Wavefunction 1D » Wavefunction 1D","id":"31","title":"Wavefunction 1D"},"32":{"body":"$ rsgrad wav1d --help\nrsgrad-wav1d Plot wavefunction in realspace, then integrate over some plane, and save it as '.txt' file USAGE: rsgrad wav1d [OPTIONS] OPTIONS: --axis Integration direction. e.g. if 'z' is provided, the XoY plane is integrated [default: z] [possible values: X, Y, Z] -b, --ibands ... Select band index, starting from 1 -d, --detail Show the eigen values and band occupations of current WAVECAR. This flag should be used with `--list` --gamma-half Gamma Half direction of WAVECAR. You need to set this to 'x' or 'z' when processing WAVECAR produced by `vasp_gam` [possible values: x, z] -h, --help Print help information --htmlout Specify the file name to be written with html wav1d data [default: wav1d.html] -k, --ikpoints ... Select kpoint index, starting from 1 [default: 1] -l, --list List the brief info of current WAVECAR -s, --ispins ... Select spin index, starting from 1 [default: 1] --scale Scale the wavefunction [default: 10] --show Open the browser and show the plot immediately --to-inline-html Render the plot and print thw rendered code to stdout --txtout Specify the file name to be written with raw wav1d data [default: wav1d.txt] -w, --wavecar WAVECAR file name [default: ./WAVECAR]","breadcrumbs":"Wavefunction 1D » Help Message","id":"32","title":"Help Message"},"33":{"body":"The usage is similar to rsgrad wav3d, too. $ rsgrad wav1d -b {20..27}\n[2022-07-14T12:54:35Z INFO rsgrad::commands::wav1d] Reading WAVECAR: \"./WAVECAR\"\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Processing spin 1, k-point 1, band 20 ...\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Processing spin 1, k-point 1, band 24 ...\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Processing spin 1, k-point 1, band 22 ...\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Processing spin 1, k-point 1, band 23 ...\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Processing spin 1, k-point 1, band 21 ...\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Processing spin 1, k-point 1, band 26 ...\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Processing spin 1, k-point 1, band 27 ...\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Processing spin 1, k-point 1, band 25 ...\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Writing to \"wav1d.html\"\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Writing to \"wav1d.txt\"\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Printing inline html to stdout ...\n[2022-07-14T12:54:36Z INFO rsgrad] Time used: 864.911523ms Then produces Note: The Fermi level is shiftted to 0.0 eV","breadcrumbs":"Wavefunction 1D » Example","id":"33","title":"Example"},"34":{"body":"rsgrad workfunc reads LOCPOT to calculate the work function. For further discussion about work function, please read this blog . Note: rsgrad workfunc does not show the vacuum level directly, hence you need to find it by hovering on the step of the work function. Take the work function above as an example, the vacuum level should be about 4.048eV around 40Å.","breadcrumbs":"Workfunction » Workfunction","id":"34","title":"Workfunction"},"35":{"body":"$ rsgrad workfunc --help\nrsgrad-workfunc\nCalculate work-function from LOCPOT file, OUTCAR is also needed to get the Fermi level. The work function is calculated by plannar integration of the data cube in LOCPOT. The selected axis\nshould be perpendicular to the other two axises. USAGE: rsgrad workfunc [OPTIONS] [LOCPOT] ARGS: LOCPOT file path. Turn on 'LVHAR' in INCAR to get the electro-static potential saved it [default: ./LOCPOT] OPTIONS: --axis Integration direction. e.g. if 'z' is provided, the XoY plane is integrated [default: z] [possible values: X, Y, Z] -h, --help Print help information -o, --htmlout Write the plot to html and view it in the web browser [default: ./workfunction.html] --outcar OUTCAR file path. This file is needed to get the E-fermi level and lattice properties [default: ./OUTCAR] --show Open default browser to see the plot immediately --to-inline-html Render the plot and print the rendered code to stdout --txtout Write the raw plot data as txt file in order to replot it with more advanced tools [default: locpot.txt]","breadcrumbs":"Workfunction » Help Message","id":"35","title":"Help Message"},"36":{"body":"In general, you don't need t provide additional arguments. $ rsgrad workfunc\n[2022-07-14T14:41:38Z INFO rsgrad::commands::workfunc] Reading \"./OUTCAR\"\n[2022-07-14T14:41:38Z INFO rsgrad::commands::workfunc] Reading electro-static potential data from \"./LOCPOT\"\n[2022-07-14T14:41:39Z INFO rsgrad::commands::workfunc] Writing raw plot data to \"locpot.txt\"\n[2022-07-14T14:41:39Z INFO rsgrad::commands::workfunc] Writing to \"./workfunction.html\"\n[2022-07-14T14:41:39Z INFO rsgrad] Time used: 1.352347116s","breadcrumbs":"Workfunction » Example","id":"36","title":"Example"},"37":{"body":"There are several operations that rsgrad pos can do Convert the fractional coordinates to Cartesian coordinates or convert reversely; Split the POSCAR and save the two parts; This command is useful when you want to calculate charge density difference and adsorption energy . Format the POSCAR and add element symbol tags to each atom.","breadcrumbs":"POSCAR » POSCAR","id":"37","title":"POSCAR"},"38":{"body":"$ rsgrad pos --help\nrsgrad-pos Operation(s) about POSCAR, including split it into two POSCARs USAGE: rsgrad pos [OPTIONS] [--] [POSCAR] ARGS: Specify the input POSCAR file [default: ./POSCAR] OPTIONS: -a, --a-name Splitted POSCAR path with selected atoms [default: POSCAR_A] -b, --b-name Splitted POSCAR path with complement of `a_name` [default: POSCAR_B] -c, --cartesian Cartesian coordinates is used in writting POSCAR --convert Convert POSCAR to cartesian coordinates or fractional coordinates --converted The target path of converted POSCAR [default: POSCAR_new] -h, --help Print help information -i, --select-indices ... Selects the indices to operate. Step indices start from '1', if '0' is given, all the structures will be selected. Step indices can be negative, where negative index means counting reversely. E.g. \"-i -2 -1 1 2 3\" means selecting the last two and the first three atom. --no-add-symbols-tags The symbols of each atom will not be written as comment in POSCAR --no-preserve-constraints Atom constraints will be dropped when writting POSCAR -s, --split Split POSCAR according to selected_indices","breadcrumbs":"POSCAR » Help Message","id":"38","title":"Help Message"},"39":{"body":"Format the POSCAR to add element symbol tags The original POSCAR of CO2: C O 1.0000000000000000 20.0000000000000000 0.0000000000000000 0.0000000000000000 0.0000000000000000 20.0000000000000000 0.0000000000000000 0.0000000000000000 0.0000000000000000 20.0000000000000000 C O 1 2\nDirect 0.5000000000000000 0.5000000000000000 -0.5000000000000000 0.5754584707965210 0.4974961803083730 0.5000000000000000 0.4249089651951450 0.5078477015701101 0.5000000000000000 Then run rsgrad pos POSCAR --convert $ rsgrad pos POSCAR --convert\n[2022-07-14T15:38:47Z INFO rsgrad::commands::pos] Reading POSCAR file \"POSCAR\" ...\n[2022-07-14T15:38:47Z INFO rsgrad::commands::pos] Converting it to \"POSCAR_new\"\n[2022-07-14T15:38:47Z INFO rsgrad::commands::pos] Done\n[2022-07-14T15:38:47Z INFO rsgrad] Time used: 1.96796ms The formatted file should be POSCAR_new C O 1.0000000 20.000000000 0.000000000 0.000000000 0.000000000 20.000000000 0.000000000 0.000000000 0.000000000 20.000000000 C O 1 2\nDirect 0.5000000000 0.5000000000 -0.5000000000 ! C-001 1 0.5754584708 0.4974961803 0.5000000000 ! O-001 2 0.4249089652 0.5078477016 0.5000000000 ! O-002 3 Convert POSCAR to Cartesian coordinates Just run rsgrad pos POSCAR --convert --cartesian $ rsgrad pos POSCAR --convert --cartesian\n[2022-07-14T15:40:33Z INFO rsgrad::commands::pos] Reading POSCAR file \"POSCAR\" ...\n[2022-07-14T15:40:33Z INFO rsgrad::commands::pos] Converting it to \"POSCAR_new\"\n[2022-07-14T15:40:33Z INFO rsgrad::commands::pos] Done\n[2022-07-14T15:40:33Z INFO rsgrad] Time used: 1.57861ms The converted file POSCAR_new should be like C O 1.0000000 20.000000000 0.000000000 0.000000000 0.000000000 20.000000000 0.000000000 0.000000000 0.000000000 20.000000000 C O 1 2\nCartesian 10.0000000000 10.0000000000 -10.0000000000 ! C-001 1 11.5091694159 9.9499236062 10.0000000000 ! O-001 2 8.4981793039 10.1569540314 10.0000000000 ! O-002 3 Split the POSCAR Let take the CO2 structure as the example again. Here we will take the C atom out to see what the operation does. The C atom index is 1, so we should run rsgrad pos POSCAR -s -i 1 $ rsgrad pos POSCAR -s -i 1\n[2022-07-14T15:49:32Z INFO rsgrad::commands::pos] Reading POSCAR file \"POSCAR\" ...\n[2022-07-14T15:49:32Z INFO rsgrad::commands::pos] Splitting it to \"POSCAR_A\" and \"POSCAR_B\" ...\n[2022-07-14T15:49:32Z INFO rsgrad::commands::pos] \"POSCAR_A\" contains\n[2022-07-14T15:49:32Z INFO rsgrad::commands::pos] C 1\n[2022-07-14T15:49:32Z INFO rsgrad::commands::pos] \"POSCAR_B\" contains\n[2022-07-14T15:49:32Z INFO rsgrad::commands::pos] O 2\n[2022-07-14T15:49:32Z INFO rsgrad::commands::pos] \"POSCAR_A\" written\n[2022-07-14T15:49:32Z INFO rsgrad::commands::pos] \"POSCAR_B\" written\n[2022-07-14T15:49:32Z INFO rsgrad] Time used: 2.11275ms The separated files should be like $ bat POSCAR_A POSCAR_B\n───────┬────────────────────────────────────────────────────────────────────────── │ File: POSCAR_A\n───────┼────────────────────────────────────────────────────────────────────────── 1 │ Generated by rsgrad, POSCAR with selected atoms 2 │ 1.0000000 3 │ 20.000000000 0.000000000 0.000000000 4 │ 0.000000000 20.000000000 0.000000000 5 │ 0.000000000 0.000000000 20.000000000 6 │ C 7 │ 1 8 │ Direct 9 │ 0.5000000000 0.5000000000 -0.5000000000 ! C-001 1\n───────┴──────────────────────────────────────────────────────────────────────────\n───────┬────────────────────────────────────────────────────────────────────────── │ File: POSCAR_B\n───────┼────────────────────────────────────────────────────────────────────────── 1 │ Generated by rsgrad, POSCAR complement 2 │ 1.0000000 3 │ 20.000000000 0.000000000 0.000000000 4 │ 0.000000000 20.000000000 0.000000000 5 │ 0.000000000 0.000000000 20.000000000 6 │ O 7 │ 2 8 │ Direct 9 │ 0.5754584708 0.4974961803 0.5000000000 ! O-001 1 10 │ 0.4249089652 0.5078477016 0.5000000000 ! O-002 2\n───────┴────────────────────────────────────────────────────────────────────────── The process schema:","breadcrumbs":"POSCAR » Examples","id":"39","title":"Examples"},"4":{"body":"To track the relaxation or MD process, use rsgrad rlx. This command is useful if you want to know the progress of geometry optimization (aka relaxation ) or molecular dynamics. This commands extract the following tags from OUTCAR: TOTEN TOTEN without entropy TOTEN difference between two ionic steps Maximum of atom forces (The negative EDIFFG is the threshold of this tag) The index of the atom with the maximum of force Number of SCF steps of each ionic step Time usage of each ionic step Volume of the cell Total magnetic moment","breadcrumbs":"Relaxation » Relaxation","id":"4","title":"Relaxation"},"40":{"body":"This command generates POTCAR according to POSCAR . The usage is simple: rsgrad pot in the directory with POSCAR presents. To use this command, a configuration file is required like: [functional-path]\nPAW_PBE = \"\"\nPAW_LDA = \"\" and you need to put it at ~/.rsgrad for Linux/macOS, and C:\\Users\\\\.rsgrad.toml for Windows. Note : rsgrad pot will give some hint if you have no idea on how to write the file. Then you can specify the element type in POSCAR , for example: Cd2 S2 HSE optimized 1.00000000000000 4.1704589747753724 0.0000000049514629 0.0000000000000000 -2.0852299788115007 3.6117232476351271 -0.0000000000000000 0.0000000000000000 -0.0000000000000000 6.7822968954189937 Cd S 2 2\nDirect 0.6666669999999968 0.3333330000000032 0.5001535716160643 0.3333330000000032 0.6666669999999968 0.0001535716160644 0.6666669999999968 0.3333330000000032 0.8768464283839381 0.3333330000000032 0.6666669999999968 0.3768464283839381 Finally rsgrad-pot will read the line \" Cd S \", and find the corresponding POTCAR and merge them. In some cases, several elements does not have \"standard\" POTCAR that without suffix. E.g. the K/POTCAR is not available for PBE functional. We provide two solutions for it: Write K_sv or other available K-related functionals in POSCAR Cd2 S2 HSE optimized 1.00000000000000 4.1704589747753724 0.0000000049514629 0.0000000000000000 -2.0852299788115007 3.6117232476351271 -0.0000000000000000 0.0000000000000000 -0.0000000000000000 6.7822968954189937 Cd K_sv 2 2\nDirect 0.6666669999999968 0.3333330000000032 0.5001535716160643 ... Use aliases field in .rsgrad.toml [functional-path]\n...\naliases = { K = \"K_sv\" } or [functional-path]\n...\n[functional-path.aliases]\nK = \"K_sv\"","breadcrumbs":"POTCAR » Pseudo Potential","id":"40","title":"Pseudo Potential"},"41":{"body":"rsgrad-pot\nGenerate the POTCAR according to POSCAR USAGE: rsgrad pot [OPTIONS] [FUNCTIONAL] ARGS: Specify the functional type, now only \"PAW_PBE\"(or \"paw_pbe\") and \"PAW_LDA\"(or \"paw_lda\") are available [default: PAW_PBE] OPTIONS: -c, --config Specify the configuration file, if left blank, rsgrad will read `.rsgrad.toml` at your home dir -h, --help Print help information -p, --poscar Specify the POSCAR file Note: the elements symbols' line should involve the specified valence configuration if you need. For example, if you need a `K_sv` POTCAR for `K`, just write `K_sv` in the POSCAR [default: ./POSCAR] -s, --save-in Specify where the `POTCAR` would be written [default: ./]","breadcrumbs":"POTCAR » Help Message","id":"41","title":"Help Message"},"42":{"body":"$ rsgrad pot\n[2023-10-20T16:19:48Z INFO rsgrad::settings] Reading rsgrad settings from \"/Users/ionizing/.rsgrad.toml\" ...\n[2023-10-20T16:19:48Z INFO rsgrad::settings] Checking rsgrad setting availability ...\n[2023-10-20T16:19:48Z INFO rsgrad::commands::pot] Reading POSCAR file \"../tests/POSCAR.CdS_HSE\" ...\n[2023-10-20T16:19:48Z INFO rsgrad::vasp_parsers::potcar] Reading POTCAR from \"/Users/ionizing/apps/vasp/pp/potpaw_PBE.54/Cd/POTCAR\"\n[2023-10-20T16:19:48Z INFO rsgrad::vasp_parsers::potcar] Reading POTCAR from \"/Users/ionizing/apps/vasp/pp/potpaw_PBE.54/S/POTCAR\"\n[2023-10-20T16:19:48Z INFO rsgrad::commands::pot] Writing POTCAR to \"./POTCAR\" ...\n[2023-10-20T16:19:48Z INFO rsgrad] Time used: 5.524643ms","breadcrumbs":"POTCAR » Example","id":"42","title":"Example"},"43":{"body":"This command (rsgrad tdm) calculates the transition dipole moment(tdm) between given bands, and then plot the peaks with plotly. Note: This command can only calculate the TDM between bands in same k-point. The inter-kpoint transition is not supported yet. Also, this commands calculates the TDM in reciprocal space by \\[ TDM_{i\\to j} = \\langle \\phi_j | e\\cdot\\vec{r} | \\phi_i \\rangle = e\\cdot\\frac{i\\hbar}{m_e\\Delta E_{ij}} \\langle \\phi_j | \\vec{p} | \\phi_i \\rangle \\] Also, this command only calculates the TDM if \\(j > i\\), otherwise it will ignore the invalid \\(i\\to j\\) pairs.","breadcrumbs":"Transition Dipole Moment » Transition Dipole Moment","id":"43","title":"Transition Dipole Moment"},"44":{"body":"$ rsgrad tdm --help\nrsgrad-tdm\nCalculate Transition Dipole Moment (TDM) between given bands. Note: This command can only calculate the TDM between bands in same k-point. The inter-kpoint\ntransition is not supported yet. Also, this commands calculates the TDM in reciprocal space by tdm_{i->j} = = i*ħ/(ΔE*m)* USAGE: rsgrad tdm [OPTIONS] --ibands ... --jbands ... OPTIONS: --barwidth Specify the width of bars in the center of peaks. (eV) [default: 0.1] --gamma-half Gamma Half direction of WAVECAR. You need to set this to 'x' or 'z' when processing WAVECAR produced by `vasp_gam` [possible values: x, z] -h, --help Print help information --htmlout Write the plot of TDM to html file [default: tdm_smeared.html] -i, --ibands ... Initial band indices, start from 1 -j, --jbands ... Final band indices, starts from 1 -k, --ikpoint K-point index, starts from 1 [default: 1] --npoints How many points in the x axis PER eV [default: 500] --peakout Write the TDM peaks to raw txt file [default: tdm_peaks.txt] -s, --ispin Spin index, 1 for up, 2 for down [default: 1] [possible values: 1, 2] --show Open the default browser to show the plot --sigma Smearing width, in eV [default: 0.05] --to-inline-html Print the inline HTML to stdout --txtout Write the summed and smeared TDM to raw txt file [default: tdm_smeared.txt] -v, --verbose Print the calculated TDM to screen -w, --wavecar WAVECAR file path [default: ./WAVECAR] --xmax Highest energy scale for tdm_smeared.txt, default for max(dE) + 2.0 --xmin Lowest energy scale for tdm_smeared.txt, default for min(dE) - 2.0","breadcrumbs":"Transition Dipole Moment » Help Message","id":"44","title":"Help Message"},"45":{"body":"The -i and -j arguments are required, or it will complain with error. $ rsgrad tdm -i 2 -j {3..5}\n[2022-08-10T07:26:46Z INFO rsgrad::commands::tdm] Reading \"./WAVECAR\"\n[2022-08-10T07:26:46Z INFO rsgrad::commands::tdm] Writing peaks info to \"tdm_peaks.txt\" ...\n[2022-08-10T07:26:46Z INFO rsgrad::commands::tdm] Writing smeared TDM data to \"tdm_smeared.txt\"\n[2022-08-10T07:26:46Z INFO rsgrad::commands::tdm] Writing plot to \"tdm_smeared.html\"\n[2022-08-10T07:26:46Z INFO rsgrad] Time used: 56.655387ms It produces the HTML like: You can view the \\(x\\), \\(y\\) and \\(z\\) components of each peak by hovering on the thin bars at the center of peaks. Note: If two peaks are in the same x position, one of them will be covered. Then the tdm_peaks.txt should be like: # iband jband E_i E_j ΔE Tx Ty Tz 2 3 -5.974 -3.675 2.298 1.311 2.556 0.000 2 4 -5.974 -3.675 2.298 2.556 1.311 0.000 2 5 -5.974 -0.975 4.999 0.000 0.000 5.309 And the tdm_smeared.txt should be like: # E(eV) Tx(Debye) Ty(Debye) Tz(Debye) 0.298325 0.007692 0.007692 0.001912 0.017295 0.300240 0.007706 0.007706 0.001914 0.017326 0.302155 0.007721 0.007721 0.001915 0.017357 0.304070 0.007736 0.007736 0.001917 0.017389 0.305985 0.007751 0.007751 0.001918 0.017420 0.307900 0.007766 0.007766 0.001920 0.017451\n...\n... Then you can plot the TDM peaks with other tools like OriginPro. If your WAVECAR is produced by vasp_gam, you'd better specify the gamma half direction by --gamma-half x or --gamma-half z, or rsgrad tdm will produce wrong results.","breadcrumbs":"Transition Dipole Moment » Example","id":"45","title":"Example"},"46":{"body":"This command (rsgrad gap) calculates the band gap and prints positions of VBM and CBM. There are two ways to run this command: Use WAVECAR only. All required information can be extracted from WAVECAR. Or use PROCAR and OUTCAR instead. PROCAR is read for the band energies, band occupations and k-point coordinates; OUTCAR is read for the Fermi level only. Note: Usually it's faster to parse results from WAVECAR. If your system is a non-SCF calculation for band structure, you may need to specify the correct Fermi level by rsgrad gap -e , the correct Fermi level can be obtained from the OUTCAR of SCF calculation.","breadcrumbs":"Gap » Gap","id":"46","title":"Gap"},"47":{"body":"$ rsgrad gap --help\nrsgrad-gap\nFind band gap and print positions of VBM and CBM USAGE: rsgrad gap [OPTIONS] OPTIONS: -e, --efermi Specify Fermi level, if left empty, this value would be read from WAVECAR or OUTCAR -h, --help Print help information -o, --outcar OUTCAR file name, this file is parsed to get Fermi level only [default: OUTCAR] -p, --procar PROCAR file name, OUTCAR is also needed to get Fermi level [default: PROCAR] -w, --wavecar WAVECAR file name, no more files needed [default: WAVECAR]","breadcrumbs":"Gap » Help Message","id":"47","title":"Help Message"},"48":{"body":"For metal system: [2022-12-01T11:30:49Z INFO rsgrad::commands::gap] Trying to parse \"WAVECAR\" ...\n---------------------------------------- Current system is Metal\n----------------------------------------\n[2022-12-01T11:30:49Z INFO rsgrad] Time used: 166.251241ms For non-spin-polarized direct gap system: [2022-12-01T11:37:15Z INFO rsgrad::commands::gap] Trying to parse \"WAVECAR\" ...\n-------------------------------------------------------------------------------- Current system has Direct Gap of 0.328 eV CBM @ k-point 1 of ( 0.000, 0.000, 0.000) , band 819 of 0.322 eV VBM @ k-point 1 of ( 0.000, 0.000, 0.000) , band 818 of -0.006 eV\n--------------------------------------------------------------------------------\n[2022-12-01T11:37:15Z INFO rsgrad] Time used: 253.556682ms For spin-polarized direct gap system: $ rsgrad gap\n[2022-12-01T11:38:16Z INFO rsgrad::commands::gap] Trying to parse \"WAVECAR\" ...\n-------------------------------------------------------------------------------- ==================== Gap Info For SPIN UP ==================== Current system has Direct Gap of 0.976 eV CBM @ k-point 1 of ( 0.000, 0.000, 0.000) , band 129 of 0.498 eV VBM @ k-point 1 of ( 0.000, 0.000, 0.000) , band 128 of -0.478 eV ==================== Gap Info For SPIN DOWN ==================== Current system has Direct Gap of 0.980 eV CBM @ k-point 1 of ( 0.000, 0.000, 0.000) , band 129 of 0.499 eV VBM @ k-point 1 of ( 0.000, 0.000, 0.000) , band 128 of -0.481 eV\n--------------------------------------------------------------------------------\n[2022-12-01T11:38:16Z INFO rsgrad] Time used: 31.744371ms For non-spin-polarized indirect gap system: $ rsgrad gap\n[2022-12-01T11:40:52Z INFO rsgrad::commands::gap] Trying to parse \"WAVECAR\" ...\n-------------------------------------------------------------------------------- Current system has Indirect Gap of 1.160 eV CBM @ k-point 25 of ( 0.000, 0.444, 0.444) , band 5 of 1.097 eV VBM @ k-point 17 of ( 0.000, 0.000, 0.000) , band 4 of -0.062 eV\n--------------------------------------------------------------------------------\n[2022-12-01T11:40:52Z INFO rsgrad] Time used: 22.565948ms","breadcrumbs":"Gap » Example","id":"48","title":"Example"},"49":{"body":"This command (rsgrad uc) converts input quantity to units representing same energy. Metric prefixes are supported, from Atto (a, 10-18) to Exa (E, 1018). Here are supported prefixes and corresponding acronyms: Metric prefix Acronym Base 10 atto a 10-18 femto f 10-15 pico p 10-12 nano n 10-9 micro μ 10-6 milli m 10-3 -- -- 100 Kilo K 103 Mega M 106 Giga G 109 Tera T 1012 Peta P 1015 exa E 1018 If you use acronyms, note that prefixes smaller than 1 (from a , atto to m , micro) must be lowercased whereas the prefixes lager than 1 (from K , Kilo to E , Exa) must be uppercased. Supported units: Unit Symbol Hartree Ha Wavenumber cm-1 Temperature(Kelvin) K Calorie per mole Cal/mol Joule per mole J/mol Wavelength m Period s Electron volt eV Frequency Hz","breadcrumbs":"UnitConversion » UnitConversion","id":"49","title":"UnitConversion"},"5":{"body":"$ rsgrad rlx -h\nrsgrad-rlx\nTracking relaxation or MD progress USAGE: rsgrad rlx [OPTIONS] [OUTCAR] ARGS: Specify the input OUTCAR file [default: ./OUTCAR] OPTIONS: -a, --favg Prints averaged total force in eV/A -e, --toten Prints TOTEN in eV -h, --help Print help information -i, --fmidx Prints the index of ion with maximum total force load. Starts from 1 --no-fmax Don't print maximum total force in A^3 --no-lgde Don't print Log10(delta(TOTEN without entropy)) --no-magmom Don't print total magnetic moment in muB --no-nscf Don't print number of SCF iteration for each ionic step --no-time Don't print time elapsed for each ionic step in minutes --no-totenz Don't print TOTEN without entropy in eV -p, --poscar Specify the input POSCAR file [default: ./POSCAR] -v, --volume Prints lattice volume in A^3 -x, --fmaxis Prints the axis where the strongest total force component lies on. [XYZ]","breadcrumbs":"Relaxation » Help Message","id":"5","title":"Help Message"},"50":{"body":"$ rsgrad uc\nConversion between various energy units Usage: rsgrad uc [INPUT]... Arguments: [INPUT]... Input energy quantity to be converted. Multiple input are supported Options: -h, --help Print help Try `rsgrad uc 298K` to see what happens.","breadcrumbs":"UnitConversion » Help Message","id":"50","title":"Help Message"},"51":{"body":"$ rsgrad uc 298K\n==================== Processing input \"298K\" ==================== 298.000000 K == 943.709369 μHa 298.000000 K == 207.125149 cm-1 298.000000 K == 298.000000 K 298.000000 K == 592.202785 Cal/mol 298.000000 K == 2.477776 KJ/mol 298.000000 K == 48.281101 μm 298.000000 K == 161.048425 fs 298.000000 K == 25.679653 meV 298.000000 K == 6.209312 THz\n================================================================================ [2024-09-11T07:21:07Z INFO rsgrad] Time used: 470.398µs You can also input multiple quantities at a time $ rsgrad uc 298K 25meV 300THz\n==================== Processing input \"298K\" ==================== 298.000000 K == 161.048425 fs 298.000000 K == 207.125149 cm-1 298.000000 K == 2.477776 KJ/mol 298.000000 K == 25.679653 meV 298.000000 K == 48.281101 μm 298.000000 K == 943.709369 μHa 298.000000 K == 592.202785 Cal/mol 298.000000 K == 6.209312 THz 298.000000 K == 298.000000 K\n================================================================================ ==================== Processing input \"25meV\" ==================== 25.000000 meV == 165.426708 fs 25.000000 meV == 201.643250 cm-1 25.000000 meV == 2.412198 KJ/mol 25.000000 meV == 25.000000 meV 25.000000 meV == 49.593677 μm 25.000000 meV == 918.732590 μHa 25.000000 meV == 576.529191 Cal/mol 25.000000 meV == 6.044973 THz 25.000000 meV == 290.112953 K\n================================================================================ ==================== Processing input \"300THz\" ==================== 300.000000 THz == 3.333333 fs 300.000000 THz == 10.007154 Kcm-1 300.000000 THz == 119.712599 KJ/mol 300.000000 THz == 1.240700 eV 300.000000 THz == 999.308150 nm 300.000000 THz == 45.594872 mHa 300.000000 THz == 28.611998 KCal/mol 300.000000 THz == 300.000000 THz 300.000000 THz == 14.397729 KK\n================================================================================ [2024-09-11T07:27:53Z INFO rsgrad] Time used: 544.171µs","breadcrumbs":"UnitConversion » Examples","id":"51","title":"Examples"},"52":{"body":"We are happy that you reach here. As an open-source project, rsgrad welcomes feedback. If you have want to add features to rsgrad, just open an issue at GitHub Issues . We also created a feature-requests list, you can follow it at this page . If rsgrad complains something or produces wrong result, just open an issue at GitHub Issues . We are grateful if you can provide the input files in order that we can reproduce the issue conveniently, thus solve the issue as soon as possible. If you are interested in rsgrad and want to contribute to the source code, just fork rsgrad and create pull requests at Pull Requests . We are super grateful if you can contribute to rsgrad.","breadcrumbs":"Feedback » Feedback","id":"52","title":"Feedback"},"53":{"body":"Qijing Zheng : The WAVECAR related function are written with the help of this code. pymatgen and ASE : Some test files are copied from these two repositories. RustFFT and ndrustfft : These two crates make wav3d and wav1d become possible. plotly.rs : This crate makes the visualization possible.","breadcrumbs":"Acknowledgements » Acknowledgements","id":"53","title":"Acknowledgements"},"6":{"body":"","breadcrumbs":"Relaxation » Example","id":"6","title":"Example"},"7":{"body":"The rsgrad dos command calculates the Density of States (DOS) of current system. rsgrad DOES NOT read the DOSCAR , but calculates the DOS from PROCAR instead by $$ D(E) = \\frac{1}{V} \\sum_{i=1}^{N} \\delta(E-E(\\mathbf{k}_i)) $$ Because rsgrad uses arbitrary unit, the factor \\(\\frac{1}{V}\\) is omitted. The \\(\\delta(x)\\) is replaced by Gaussian function or Lorentzian function: $$ g(x) = \\frac{1}{\\sigma\\sqrt{2\\pi}} \\exp \\left( -\\frac{1}{2} \\frac{(x-\\mu)^2}{\\sigma^2} \\right) \\\\ l(x) = \\frac{1}{\\pi} \\frac{\\sigma}{(x-\\mu)^2 + \\sigma^2} $$ where \\(\\mu\\) is \\(E(\\mathbf{k}_i)\\) and \\(\\sigma\\) is sigma of configuration in the implementation. This method makes it easier to calculate projected DOS with projection of specific atoms, angular moments and k-points. However, this method sometimes differs from DOSCAR with ISMEAR = -5. For detailed explaination, see the document here . The OUTCAR is also needed to get the Fermi level.","breadcrumbs":"Density of States » Density of States","id":"7","title":"Density of States"},"8":{"body":"$ rsgrad dos -h\nrsgrad-dos\nCalculate density of states from PROCAR and OUTCAR USAGE: rsgrad dos [OPTIONS] OPTIONS: -c, --config Projected DOS configuration file path --gen-template Generate projected DOS configuration template -h, --help Print help information --htmlout Save the projected DOS plot as HTML. Then you can view it in the browser [default: dos.html] --outcar OUTCAR path [default: ./OUTCAR] --procar PROCAR path [default: ./PROCAR] --show Open the browser and show the plot immediately --show-brief Print brief info of PROCAR, this may be helpful when you write the configuration --to-inline-html Render the plot and print the rendered code to stdout --txtout Save the raw data of projected DOS. Then you can replot it with more advanced tools [default: dos_raw.txt] --xlim Set the x-range of the plot [default: -1 6]","breadcrumbs":"Density of States » Help Message","id":"8","title":"Help Message"},"9":{"body":"The configuration template can be generated by running rsgrad dos --gen-template. The following configuration is written to pband.toml by default: # rsgrad DOS configuration in toml format.\n# multiple tokens inside string are seperated by whitespace\nmethod = \"Gaussian\" # smearing method\nsigma = 0.05 # smearing width, (eV)\nprocar = \"PROCAR\" # PROCAR path\noutcar = \"OUTCAR\" # OUTCAR path\ntxtout = \"dos_raw.txt\" # save the raw data as \"dos_raw.txt\"\nhtmlout = \"dos.html\" # save the pdos plot as \"dos.html\"\ntotdos = true # plot the total dos\nfill = true # fill the plot to x axis or not\nxlim = [-1, 6] # x-range of plot [pdos.plot1] # One label produces one plot, the labels CANNOT be repetitive. # This label is 'plot1', to add more pdos, write '[pdos.plot2]' and so on.\nkpoints = \"1 3..7 -1\" # selects 1 3 4 5 6 7 and the last kpoint for pdos plot.\natoms = \"1 3..7 -1\" # selects 1 3 4 5 6 7 and the last atoms' projection for pdos plot.\norbits = \"s px dxy\" # selects the s px and dx orbits' projection for pdos plot.\nfactor = 1.01 # the factor multiplied to this pdos [pdos.plot2] # One label produces one plot, the labels CANNOT be repetitive. # This label is 'plot2', to add more pdos, write '[pdos.plot2]' and so on.\nkpoints = \"1 3..7 -1\" # selects 1 3 4 5 6 7 and the last kpoint for pdos plot.\natoms = \"1 3..7 -1\" # selects 1 3 4 5 6 7 and the last atoms' projection for pdos plot.\norbits = \"s px dxy\" # selects the s px and dx orbits' projection for pdos plot.\nfactor = 1.01 # the factor multiplied to this pdos # The fields can be left blank, if you want select all the components for some fields,\n# just comment them. 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is an open-source command-line tool to help VASP players play better with VASP. rsgrad is written proudly in pure Rust . Now rsgrad provides several features: Track the relaxation and MD (molecular dynamics) progress; Calculate and visualize the DOS (density of states) and pDOS (projected DOS); Plot and visualize the band structure and fat band structure; Save the frames with given MD or relaxation trajectory; Calculate charge density difference; Analyze the vibration eigen values and eigen vectors; Plot the wave function at given bands in real-space; Plot the wave function at given bands in real-space then integrate it over specified plane; Plot and visualize the work function; Split POSCAR ; Convert between fractional coordinates and Cartesian coordinates; Format POSCAR ; Generate POTCAR according to POSCAR ; Calculate Transition Dipole Moment from WAVECAR ; Calculate band gap and print locations of CBM and VBM. Convert one quantity to other units that representing same energy. Wish you have a good time with rsgrad ^_^","breadcrumbs":"Introduction » Introduction","id":"0","title":"Introduction"},"1":{"body":"There are two ways to install rsgrad, downloading the pre-built binaries and building from scratch.","breadcrumbs":"Installation » Installation","id":"1","title":"Installation"},"10":{"body":"This command can calculate total DOS only. To calculate projected DOS, use configuration instead (see next section). $ rsgrad dos\n[2022-07-14T18:42:55Z INFO rsgrad::commands::dos] Parsing PROCAR file \"./PROCAR\"\n[2022-07-14T18:42:55Z INFO rsgrad::commands::dos] Parsing OUTCAR file \"./OUTCAR\" for Fermi level\n[2022-07-14T18:42:55Z INFO rsgrad::commands::dos] Found Fermi level = -1.9018, eigenvalues will be shifted.\n[2022-07-14T18:42:55Z INFO rsgrad::commands::dos] Plotting Total DOS ...\n[2022-07-14T18:42:55Z INFO rsgrad::commands::dos] Total DOS plot time usage: 29.055µs\n[2022-07-14T18:42:55Z INFO rsgrad::commands::dos] Writing DOS plot to \"dos.html\"\n[2022-07-14T18:42:55Z INFO rsgrad::commands::dos] Writing raw DOS data to \"dos_raw.txt\"\n[2022-07-14T18:42:55Z INFO rsgrad] Time used: 124.426652ms The output html should be like something in the following","breadcrumbs":"Density of States » Example (without configuration file)","id":"10","title":"Example (without configuration file)"},"11":{"body":"To plot multiple PDOS, using configuration file is suggested. With the configuration (pdos.toml) in the following method = \"Gaussian\"\nsigma = 0.05\nprocar = \"PROCAR\"\noutcar = \"OUTCAR\"\ntxtout = \"dos_raw.txt\"\nhtmlout = \"dos.html\"\ntotdos = true\nfill = true\nxlim = [-1, 6] [pdos.Benzene]\natoms = \"37..48\" [pdos.AgSurf]\natoms = \"3 6 10 14 21 23 25 33 36\" then rsgrad dos -c pdos.toml $ rsgrad dos -c pdos.toml\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Reading PDOS configuration from Some(\"pdos.toml\")\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Parsing PROCAR file \"PROCAR\"\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Parsing OUTCAR file \"OUTCAR\" for Fermi level\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Found Fermi level = -1.9018, eigenvalues will be shifted.\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Plotting Total DOS ...\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Total DOS plot time usage: 42.878µs\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Plotting PDOS ...\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] PDOS plot time usage: 6.223076ms\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Writing DOS plot to \"dos.html\"\n[2022-07-14T18:43:34Z INFO rsgrad::commands::dos] Writing raw DOS data to \"dos_raw.txt\"\n[2022-07-14T18:43:34Z INFO rsgrad] Time used: 61.982958ms you will get something in the following","breadcrumbs":"Density of States » Example (with configuration file)","id":"11","title":"Example (with configuration file)"},"12":{"body":"rsgrad can write the raw data of plot by setting txtout (dos_raw.txt by default). The organization of it shows the energy, total DOS and projected dos respectively: # E-Ef TotDOS Benzene AgSurf\n... -7.921938 0.002969 0.002158 0.000004 -7.899296 0.016032 0.011655 0.000019 -7.876654 0.070713 0.051408 0.000085 -7.854012 0.254749 0.185212 0.000307 -7.831371 0.749573 0.544998 0.000910 -7.808729 1.801235 1.309709 0.002202 -7.786087 3.534640 2.570233 0.004349 -7.763446 5.663677 4.118580 0.007011 -7.740804 7.409459 5.388357 0.009226 -7.718162 7.913407 5.755104 0.009908 -7.695520 6.898991 5.017578 0.008683 -7.672879 4.909619 3.570876 0.006208 -7.650237 2.854880 2.076535 0.003622 -7.627595 1.373037 0.998928 0.001724 -7.604953 0.617183 0.449840 0.000672 -7.582312 0.494734 0.362904 0.000231 -7.559670 0.977346 0.718873 0.000173 -7.537028 2.169137 1.593003 0.000599 -7.514387 4.077126 2.981347 0.002383 -7.491745 6.295459 4.560748 0.007858 -7.469103 8.005154 5.685401 0.021128\n... The first line shows the labels of each series and have a hastag # in the beginning in order to let numpy.loadtxt can read it directly. Then you can throw it into other plotters like Excel, Matplotlib, OriginPro GnuPlot etc. and do whatever fancy things you prefer.","breadcrumbs":"Density of States » Usage of txtout","id":"12","title":"Usage of txtout"},"13":{"body":"rsgrad band can plot the band structure from PROCAR and OUTCAR .","breadcrumbs":"Band Structure » Band Structure","id":"13","title":"Band Structure"},"14":{"body":"$ rsgrad band -h\nrsgrad-band\nPlot bandstructure and projected bandstructure USAGE: rsgrad band [OPTIONS] OPTIONS: -c, --config Band structure plot configuration file path --colormap [default: jet] --efermi Set the E-fermi given from SCF's OUTCAR and it will be the reference energy level --gen-template Generate band structure plot configuration template -h, --help Print help information --htmlout Save the band structure plot as HTML [default: band.html] -k, --kpoint-labels Symbols for high symmetry points on the kpoint path --ncl-spinor [possible values: X, Y, Z] --outcar OUTCAR path [default: ./OUTCAR] --procar PROCAR path [default: ./PROCAR] --show Open the browser and show the plot immediately --to-inline-html Render the plot and print the rendered code to stdout --txtout-prefix Save the raw data of band structure [default: band_raw] --ylim Set the y-range of the plot [default: \"-1 6\"]","breadcrumbs":"Band Structure » Help Message","id":"14","title":"Help Message"},"15":{"body":"# rsgrad Band plot configuration in toml format.\n# multiple tokens inside string are seperated by whitespace, if you # kpoint-labels = [\"G\", \"K\", \"M\", \"G\"] # should be consistant with the boundaries in KPOINTS\nprocar = \"PROCAR\"\noutcar = \"OUTCAR\"\ntxtout-prefix = \"band_raw\"\nhtmlout = \"band.html\"\n# segment-ranges = [[1, 40], [41, 80], [81, 120]] # if commented, rsgrad will find the boundaries by judging if k[i] == k[i+1]\n# ncl-spinor = \"Z\" # for vasp_ncl calculation\n# colormap = \"jet\" # the colormap specified to plot ncl-band\n# efermi = 0.0 # if commented, rsgrad will read the efermi from OUTCAR, but if may be slightly different from scf's\n# ylim = [-1, 6] # [pband.plot1]\n# spins = \"up down\" # \"u d\" are also ok, for ncl system, \"tot x y z\" are available\n# atoms = \"1 3..7 -1\" # which atoms to project on, if commented, all atoms are selected\n# orbits = \"s px dxy\" # which orbits to project on, if commented, all orbits are selected\n# color = \"red\" # the color of marker","breadcrumbs":"Band Structure » Configuration Template","id":"15","title":"Configuration Template"},"16":{"body":"Simply run rsgrad band can plot the band structure. $ rsgrad band\n[2022-07-14T18:40:18Z INFO rsgrad::commands::band] Reading fermi level and lattice data from \"./OUTCAR\"\n[2022-07-14T18:40:18Z INFO rsgrad::commands::band] Reading band data from \"./PROCAR\"\n[2022-07-14T18:40:18Z INFO rsgrad::commands::band] Found Fermi level: 12.7626, shifting eigenvalues ...\n[2022-07-14T18:40:18Z WARN rsgrad::commands::band] No k-point labels found, use empty labels instead\n[2022-07-14T18:40:18Z INFO rsgrad::commands::band] Plotting raw bands ...\n[2022-07-14T18:40:18Z INFO rsgrad::commands::band] Writing Bandstructure to \"band.html\"\n[2022-07-14T18:40:18Z INFO rsgrad::commands::band] Writing raw band data to \"band_raw.txt\"\n[2022-07-14T18:40:18Z INFO rsgrad] Time used: 79.644034ms There may be a warning reminds you provide the labels of each high-symmetry point. rsgrad identifies high-symmetry points by calculate the difference of consecutive k-points. If the difference equals zero, these two points are labelled as one high-symmetry point. For example: ...\nk-point 38 : 0.0000 0.0256 0.0000\nk-point 39 : 0.0000 0.0128 0.0000\nk-point 40 : 0.0000 0.0000 0.0000\nk-point 41 : 0.0000 0.0000 0.0000\nk-point 42 : -0.0085 0.0171 0.0000\nk-point 43 : -0.0171 0.0342 0.0000\n... k-point 40 and k-point 41 are same, thus be identified as one high-symmetry point. Each of the high-symmetry points need a label. You may either left the --kpoint-labels empty or provide the correct labels seperated by white spaces. Sometimes it may produce wrong band structure due to the special k-point path like kpoints for bandstructure L-G-X-U K-G 10\nline\nreciprocal 0.50000 0.50000 0.50000 1 0.00000 0.00000 0.00000 1 0.00000 0.00000 0.00000 1 0.00000 0.50000 0.50000 1 0.00000 0.50000 0.50000 1 0.25000 0.62500 0.62500 1 0.37500 0.7500 0.37500 1 0.00000 0.00000 0.00000 1 The end of third segment (0.25000, 0.62500, 0.62500) and the beginning of fourth segment (0.37500, 0.7500, 0.37500) are not consistent, which produces wrong k-path, leading to wrong band structure: To solve this issue, you need to try the configuration file.","breadcrumbs":"Band Structure » Example (without configuration file)","id":"16","title":"Example (without configuration file)"},"17":{"body":"With the configuration in the following kpoint-labels = [\"L\", \"Γ\", \"X\", \"U|K\", \"Γ\"]\nprocar = \"PROCAR\"\noutcar = \"OUTCAR\"\ntxtout-prefix = \"pband_raw\"\nhtmlout = \"pband.html\"\nsegment-ranges = [[1, 10], [11, 20], [21, 30], [31, 40]] [pband.Si-p-orbit]\norbits = \"px py pz\"\ncolor = \"red\" and run rsgrad -c pband.toml $ rsgrad band -c pband.toml\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Reading porjected band configuration fomr Some(\"pband.toml\")\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Reading fermi level and lattice data from \"OUTCAR\"\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Reading band data from \"PROCAR\"\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Found Fermi level: 12.7626, shifting eigenvalues ...\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Plotting raw bands ...\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Plotting projected bands ...\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Writting projected band Si-p-orbit to \"pband_raw_Si-p-orbit.txt\" ...\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Projected band plot time usage: 1.220401ms\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Writing Bandstructure to \"band.html\"\n[2022-07-14T18:41:02Z INFO rsgrad::commands::band] Writing raw band data to \"pband_raw.txt\"\n[2022-07-14T18:41:02Z INFO rsgrad] Time used: 77.804627ms then it produces","breadcrumbs":"Band Structure » Example (with configuration file)","id":"17","title":"Example (with configuration file)"},"18":{"body":"For the results produced by vasp_ncl, rsgrad supports plotting the \\(z\\) (\\(x\\) and \\(y\\) are also OK) projection to analyze the spin angular moments. kpoint-labels = [\"M\", \"Γ\", \"K\", \"M\"]\nprocar = \"PROCAR\"\noutcar = \"OUTCAR\"\ntxtout-prefix = \"band_ncl_raw\"\nhtmlout = \"band_ncl.html\"\nsegment-ranges = [[81, 120], [1, 40], [41, 80]]\nncl-spinor = \"Z\"\ncolormap = \"jet\" then it produces","breadcrumbs":"Band Structure » Example (for non-collinear system)","id":"18","title":"Example (for non-collinear system)"},"19":{"body":"rsgrad reads OUTCAR then provide some operations in the following. Save selected steps as XDATCAR . Save selected steps as POSCAR files. Save selected steps as XSF files. With XSF , VESTA can show the force vectors on every atom.","breadcrumbs":"Trajectory » Trajectory","id":"19","title":"Trajectory"},"2":{"body":"We provide the pre-built binaries at GitHub Release . There are four platforms we support with pre-built binaries rsgrad--linux-x86_64-musl.tar.gz: Statically linked binary. Can run on almost all Linux distros. However, the musl libc may have performance issues in some scenes like wave1d, wav3d etc. rsgrad--linux-x86_64.tar.gz: Dynamically linked against glibc and other fundamental system libraries. For the binaries with 0.3.6_ci-test or upper version, they can run on most Linux distros (e.g. CentOS 7, Ubuntu 18.04). If it still complains with message like /lib64/libc.so.6: version 'GLIBC_2.18' not found, just switch to -musl binary or build from scratch. rsgrad--macos-x86_64.tar.gz: Binary for macOS (Intel). rsgrad is developed on macOS 13, which means you are don't need to worry about the availability if you are using macOS. rsgrad--macos-aarch64.tar.gz: Binary for macOS (Apple Silicon). rsgrad--windows-x86_64.zip: Binary for Windows system. We have no plan to support 32-bit systems. Download the corresponding binary and put it in $PATH (or %PATH% on Windows), and have fun!","breadcrumbs":"Installation » Download the Binary from GitHub Release","id":"2","title":"Download the Binary from GitHub Release"},"20":{"body":"$ rsgrad traj --help\nrsgrad-traj\nOperations about relaxation/MD trajectory. POSCAR is needed if you want to preserve the constraints when saving frames to POSCAR. USAGE: rsgrad traj [OPTIONS] [--] [OUTCAR] ARGS: Specify the input OUTCAR file [default: ./OUTCAR] OPTIONS: --cartesian Save to POSCAR in cartesian coordinates, the coordinates written is direct/fractional by default -d, --save-as-xdatcar Save whole trajectory in XDATCAR format -h, --help Print help information -i, --select-indices ... Selects the indices to operate. Step indices start from '1', if '0' is given, all the structures will be selected. Step indices can be negative, where negative index means counting reversely. E.g. \"-i -2 -1 1 2 3\" means selecting the last two and first three steps. --no-add-symbol-tags Don't add chemical symbol to each line of coordinates --no-preserve-constraints Don't preverse constraints when saving trajectory to POSCAR -p, --poscar Specify the input POSCAR file [default: ./POSCAR] -s, --save-as-poscar Save selected steps as POSCARs --save-in Define where the files would be saved [default: .] -x, --save-as-xsfs Saves each selected modes to XSF file, this file includes each atom's force information","breadcrumbs":"Trajectory » Help Message","id":"20","title":"Help Message"},"21":{"body":"Take the last step and save as XSF file rsgrad traj -i -1 -x $ rsgrad traj -i -1 -x\n[2022-07-14T18:37:35Z INFO rsgrad::commands::traj] Parsing file \"./OUTCAR\" and \"./POSCAR\"\n[2022-07-14T18:37:35Z INFO rsgrad::vasp_parsers::outcar] Saving ionic step to \"./step_0003.xsf\" ...\n[2022-07-14T18:37:35Z INFO rsgrad] Time used: 11.223561ms Take the first step and save as POSCAR file rsgrad traj -i 1 -s $ rsgrad traj -i 1 -s\n[2022-07-14T18:38:51Z INFO rsgrad::commands::traj] Parsing file \"./OUTCAR\" and \"./POSCAR\"\n[2022-07-14T18:38:51Z INFO rsgrad::vasp_parsers::outcar] Saving trajectory step # 1 to \"./POSCAR_00001.vasp\" ...\n[2022-07-14T18:38:51Z INFO rsgrad] Time used: 8.64197ms","breadcrumbs":"Trajectory » Examples","id":"21","title":"Examples"},"22":{"body":"rsgrad chgdiff can calculate the charge density difference from CHGCAR files: $$ \\Delta \\rho = \\rho_{A+B} - (\\rho_A + \\rho_B) $$ Where \\(\\rho_{A+B}\\), \\(\\rho_A\\) and \\(\\rho_B\\) are the charge densities of total structure, A structure and B structure, respectively. You may also need rsgrad poscar --split ... to generate the structure of A and B from A+B.","breadcrumbs":"Charge Density Difference » Charge Density Difference","id":"22","title":"Charge Density Difference"},"23":{"body":"$ rsgrad chgdiff --help\nrsgrad-chgdiff\nCalculate charge density difference. The operation is performed by `chgdiff = chgcar_ab - (chgcar_a + chgcar_b)`. USAGE: rsgrad chgdiff [OPTIONS] ARGS: The CHGCAR of A+B system The CHGCAR of A system The CHGCAR of B system OPTIONS: -h, --help Print help information -o, --output The output charge density difference file path [default: CHGDIFF.vasp]","breadcrumbs":"Charge Density Difference » Help message","id":"23","title":"Help message"},"24":{"body":"You need to calculate the electronic structure of the three structures (A+B, A and B) first, then rsgrad chgdiff CHGCAR_A+B CHGCAR_A CHGCAR_B like $ rsgrad chgdiff ../scf/CHGCAR Ag/CHGCAR noAg/CHGCAR\n[2022-07-14T18:34:59Z INFO rsgrad::commands::chgdiff] Reading charge density from \"Ag/CHGCAR\"\n[2022-07-14T18:34:59Z INFO rsgrad::commands::chgdiff] Reading charge density from \"noAg/CHGCAR\"\n[2022-07-14T18:34:59Z INFO rsgrad::commands::chgdiff] Reading charge density from \"../scf/CHGCAR\"\n[2022-07-14T18:35:06Z INFO rsgrad::commands::chgdiff] Calculating charge density difference by `CHGDIFF = \"../scf/CHGCAR\" - (\"Ag/CHGCAR\" + \"noAg/CHGCAR\")`\n[2022-07-14T18:35:06Z INFO rsgrad::commands::chgdiff] Writing charge difference to \"CHGDIFF.vasp\"\n[2022-07-14T18:35:10Z INFO rsgrad] Time used: 11.189259653s finally use VESTA to visualize the data","breadcrumbs":"Charge Density Difference » Example","id":"24","title":"Example"},"25":{"body":"For systems enabled vibration calculation (phonon at Γ point only), rsgrad vib can Print the phonon eigenvalues; Save the phonon eigenvectors; Modulate the ground-state according to specified modes.","breadcrumbs":"Vibration » Vibration","id":"25","title":"Vibration"},"26":{"body":"$ rsgrad vib --help\nrsgrad-vib\nTracking vibration information. For systems enabled vibration mode calculation, this command can extract phonon eigenvalues and\nphonon eigenvectors at Gamma point. USAGE: rsgrad vib [OPTIONS] [--] [OUTCAR] ARGS: Specify the input OUTCAR file [default: ./OUTCAR] OPTIONS: -a, --amplitude Modulation amplitude coefficient, to avoid precision issue, abs(amplitude) >= 0.01 should be satisfied [default: 0.1] -c, --cartesian Catesian coordinate is used when writting POSCAR. Fractional coordinate is used by default -h, --help Print help information -i, --select-indices ... Selects the mode indices to operate. Step indices start from '1', if '0' is given, all the structures will be selected. Step indices can be negative, where negative index means counting reversely. E.g. \"-i -2 -1 1 2 3\" means selecting the last two and first three steps. -l, --list Shows vibration modes in brief -m, --modulate Modulate the ground-state POSCAR with respect to a certern vibration frequencies -p, --poscar Specify the input POSCAR file, the consntraints info is needed [default: ./POSCAR] --save-in Define where the files would be saved [default: .] -x, --save-as-xsfs Saves each selected modes to XSF file","breadcrumbs":"Vibration » Help Message","id":"26","title":"Help Message"},"27":{"body":"Print the phonon eigenvalues; Save the phonon eigenvectors; $ rsgrad vib -i {1..3} {-3..-1} -x\n[2022-07-14T18:32:49Z INFO rsgrad::commands::vib] Parsing file \"./OUTCAR\"\n[2022-07-14T18:32:49Z INFO rsgrad::vasp_parsers::outcar] Saving mode # 1 as \"./mode_0001_3682.13cm-1.xsf\" ...\n[2022-07-14T18:32:49Z INFO rsgrad::vasp_parsers::outcar] Saving mode # 3 as \"./mode_0003_3679.99cm-1.xsf\" ...\n[2022-07-14T18:32:49Z INFO rsgrad::vasp_parsers::outcar] Saving mode # 44 as \"./mode_0044_0010.79cm-1_imag.xsf\" ...\n[2022-07-14T18:32:49Z INFO rsgrad::vasp_parsers::outcar] Saving mode # 43 as \"./mode_0043_0007.12cm-1_imag.xsf\" ...\n[2022-07-14T18:32:49Z INFO rsgrad::vasp_parsers::outcar] Saving mode # 2 as \"./mode_0002_3680.83cm-1.xsf\" ...\n[2022-07-14T18:32:49Z INFO rsgrad::vasp_parsers::outcar] Saving mode # 45 as \"./mode_0045_0047.20cm-1_imag.xsf\" ...\n[2022-07-14T18:32:49Z INFO rsgrad] Time used: 109.566967ms Modulate the ground-state according to specified modes. $ rsgrad vib -i {-3..-1} --modulate --amplitude 0.1\n[2022-07-14T18:31:41Z INFO rsgrad::commands::vib] Parsing file \"./OUTCAR\"\n[2022-07-14T18:31:41Z INFO rsgrad::vasp_parsers::outcar] Saving modulated POSCAR of mode # 43 with amplitude coeff 0.100 as \"./mode_0043_0007.12cm-1_0.100_imag.vasp\" ...\n[2022-07-14T18:31:41Z INFO rsgrad::vasp_parsers::outcar] Saving modulated POSCAR of mode # 44 with amplitude coeff 0.100 as \"./mode_0044_0010.79cm-1_0.100_imag.vasp\" ...\n[2022-07-14T18:31:41Z INFO rsgrad::vasp_parsers::outcar] Saving modulated POSCAR of mode # 45 with amplitude coeff 0.100 as \"./mode_0045_0047.20cm-1_0.100_imag.vasp\" ...\n[2022-07-14T18:31:41Z INFO rsgrad] Time used: 202.629805ms","breadcrumbs":"Vibration » Example","id":"27","title":"Example"},"28":{"body":"Main functions of rsgrad wav3d List the brief information of WAVECAR ; Save the selected wavefunction to .vasp file.","breadcrumbs":"Wavefunction 3D » Wavefunction 3D","id":"28","title":"Wavefunction 3D"},"29":{"body":"$ rsgrad wav3d --help\nPlot wavefunction in realspace, and save it as '.vasp' file Usage: rsgrad wav3d [OPTIONS] Options: -w, --wavecar WAVECAR file name [default: ./WAVECAR] -p, --poscar POSCAR filename, POSCAR is needed to get the real-space wavefunction [default: ./POSCAR] -s, --ispins [...] Select spin index, starting from 1 [default: 1] -k, --ikpoints [...] Select kpoint index, starting from 1. You can input ranges directly: `-k 1..4 5..10` [default: 1] -b, --ibands [...] Select band index, starting from 1. You can input ranges directly: `-b 1..4 5..10` -l, --list List the brief info of current WAVECAR -d, --detail Show the eigen values and band occupations of current WAVECAR. This flag should be used with `--list` --gamma-half Gamma Half direction of WAVECAR. You need to set this to 'x' or 'z' when processing WAVECAR produced by `vasp_gam` [possible values: x, z] --ngrid Grid size for realspace wavefunction, 3 numbers are required, i.e. NGXF NGYF and NGZF. If this argument is left empty, NG_F will be set as NG_F=2*NG_. Be aware that NG_F must be greater than or at least equal to corresponding NG_. -o, --output-parts [...] Specify output part of the wavefunction. Detailed message: - normsquared/ns: Perform `ρ(r) = |ѱ(r)|^2` action to get the spatial distribution of selected band. - real/re: Real part of the wavefunction, suffix '_re.vasp' is added to the output filename. - imag/im: Imaginary part of the wavefunction, suffix '_im.vasp' is added to the output filename. - reim: Output both real part and imaginary parts of the wavefunction. - uns/dns: Perform `ρ(r) = |ѱ(r)|^2` for spinor up/down only. **Note: this option works for `ncl` WAVECAR only.** [possible values: normsquared, ns, uns, dns, real, re, imag, im, reim] --prefix Prefix of output filename [default: wav] -e, --show-eigs-suffix Add eigen value suffix to the filename --sum-chgs Perform sum-up of the charge densities for selected bands. With this flag open, only `normsquared` or `ns` or `uns` or `dns` are allowed for the `-o`/`--output-parts` option. IMPORTANT NOTES: - The prefix for output filename `sum-prefix` is also required and has no default prefix. - The individual charge densities will not be saved to corresponding '.vasp' files if this flag is on. --sum-prefix Specify the output file for the summed charge densities. This argument is required if `sum_chgs` is on. -h, --help Print help (see a summary with '-h')","breadcrumbs":"Wavefunction 3D » Help Message","id":"29","title":"Help Message"},"3":{"body":"The build requires Internet accessibility. If you haven't installed Rust toolchain, run curl --proto '=https' --tlsv1.2 -sSf https://sh.rustup.rs | sh and follow the instructions to configure it. When you finished the toolchain installation, you should be able to run cargo in command-line. Detailed instructions can be found here . If you have installed Rust toolchain already, just run cargo install --git https://github.com/Ionizing/rsgrad. Several minutes later, the rsgrad should be installed to ~/.cargo/bin, no need to modify the $PATH (or %PATH% on Windows).","breadcrumbs":"Installation » Build from Scratch","id":"3","title":"Build from Scratch"},"30":{"body":"List the brief information of WAVECAR $ rsgrad wav3d -l [2022-07-14T09:19:51Z INFO rsgrad::commands::wav3d] Reading WAVECAR: \"./WAVECAR\"\nLENGTH = 54145104\nRECLEN = 1388336\nTYPE = Standard\nNSPIN = 1\nNKPTS = 1\nNBANDS = 36\nENCUT = 450.000\nEFERMI = -5.368\nVOLUME = 8000.000\nNGRID = [ 71, 71, 71]\nNPLWS = [173541]\nACELL = [[ 20.000, 0.000, 0.000], [ 0.000, 20.000, 0.000], [ 0.000, 0.000, 20.000]]\nBCELL = [[ 0.050, 0.000, 0.000], [ 0.000, 0.050, 0.000], [ 0.000, 0.000, 0.050]] [2022-07-14T09:19:51Z INFO rsgrad] Time used: 160.337862ms if you want the band eigen values information $ rsgrad wav3d -ld ...\n\n... ISPIN: 1 IKPOINT: 1 IBAND: 1 E-Efermi: -19.991 Occupation: 1.000\nISPIN: 1 IKPOINT: 1 IBAND: 2 E-Efermi: -18.141 Occupation: 1.000\nISPIN: 1 IKPOINT: 1 IBAND: 3 E-Efermi: -18.141 Occupation: 1.000\nISPIN: 1 IKPOINT: 1 IBAND: 4 E-Efermi: -16.418 Occupation: 1.000\nISPIN: 1 IKPOINT: 1 IBAND: 5 E-Efermi: -15.534 Occupation: 1.000\nISPIN: 1 IKPOINT: 1 IBAND: 6 E-Efermi: -15.532 Occupation: 1.000\nISPIN: 1 IKPOINT: 1 IBAND: 7 E-Efermi: -10.662 Occupation: 1.000\nISPIN: 1 IKPOINT: 1 IBAND: 8 E-Efermi: -10.661 Occupation: 1.000\n... Save the selected wavefunction to .vasp file $ rsgrad wav3d -b {10..20} -o ns -e [2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Reading WAVECAR: \"./WAVECAR\"\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Reading POSCAR: \"./POSCAR\"\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 10 ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 13 ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 11 ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 14 ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 12 ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 15 ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-13_-5.740eV.vasp\" ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-15_-5.601eV.vasp\" ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-14_-5.728eV.vasp\" ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-10_-8.376eV.vasp\" ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-11_-7.385eV.vasp\" ...\n[2022-07-14T09:23:06Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-12_-7.380eV.vasp\" ...\n[2022-07-14T09:23:08Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 18 ...\n[2022-07-14T09:23:08Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 19 ...\n[2022-07-14T09:23:09Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-18_-3.514eV.vasp\" ...\n[2022-07-14T09:23:09Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 16 ...\n[2022-07-14T09:23:09Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 20 ...\n[2022-07-14T09:23:09Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-19_-3.265eV.vasp\" ...\n[2022-07-14T09:23:09Z INFO rsgrad::commands::wav3d] Processing spin 1, k-point 1, band 17 ...\n[2022-07-14T09:23:10Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-16_-5.477eV.vasp\" ...\n[2022-07-14T09:23:10Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-17_-3.546eV.vasp\" ...\n[2022-07-14T09:23:10Z INFO rsgrad::commands::wav3d] Writing \"wav_1-1-20_-0.701eV.vasp\" ...\n[2022-07-14T09:23:11Z INFO rsgrad] Time used: 5.484733549s Open the .vasp in VESTA rsgrad wav3d supports extracting multiple bands at the same time, and the processes executed in parallel, which can save a lot of time.","breadcrumbs":"Wavefunction 3D » Example","id":"30","title":"Example"},"31":{"body":"This command is similar to rsgrad wav3d. The only difference is that wav1d integrates the wavefunction over specified plane, and produces the averaged one dimensional wavefunction. This command is useful when you are looking for image potential states.","breadcrumbs":"Wavefunction 1D » Wavefunction 1D","id":"31","title":"Wavefunction 1D"},"32":{"body":"$ rsgrad wav1d --help\nrsgrad-wav1d Plot wavefunction in realspace, then integrate over some plane, and save it as '.txt' file USAGE: rsgrad wav1d [OPTIONS] OPTIONS: --axis Integration direction. e.g. if 'z' is provided, the XoY plane is integrated [default: z] [possible values: X, Y, Z] -b, --ibands ... Select band index, starting from 1 -d, --detail Show the eigen values and band occupations of current WAVECAR. This flag should be used with `--list` --gamma-half Gamma Half direction of WAVECAR. You need to set this to 'x' or 'z' when processing WAVECAR produced by `vasp_gam` [possible values: x, z] -h, --help Print help information --htmlout Specify the file name to be written with html wav1d data [default: wav1d.html] -k, --ikpoints ... Select kpoint index, starting from 1 [default: 1] -l, --list List the brief info of current WAVECAR -s, --ispins ... Select spin index, starting from 1 [default: 1] --scale Scale the wavefunction [default: 10] --show Open the browser and show the plot immediately --to-inline-html Render the plot and print thw rendered code to stdout --txtout Specify the file name to be written with raw wav1d data [default: wav1d.txt] -w, --wavecar WAVECAR file name [default: ./WAVECAR]","breadcrumbs":"Wavefunction 1D » Help Message","id":"32","title":"Help Message"},"33":{"body":"The usage is similar to rsgrad wav3d, too. $ rsgrad wav1d -b {20..27}\n[2022-07-14T12:54:35Z INFO rsgrad::commands::wav1d] Reading WAVECAR: \"./WAVECAR\"\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Processing spin 1, k-point 1, band 20 ...\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Processing spin 1, k-point 1, band 24 ...\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Processing spin 1, k-point 1, band 22 ...\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Processing spin 1, k-point 1, band 23 ...\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Processing spin 1, k-point 1, band 21 ...\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Processing spin 1, k-point 1, band 26 ...\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Processing spin 1, k-point 1, band 27 ...\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Processing spin 1, k-point 1, band 25 ...\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Writing to \"wav1d.html\"\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Writing to \"wav1d.txt\"\n[2022-07-14T12:54:36Z INFO rsgrad::commands::wav1d] Printing inline html to stdout ...\n[2022-07-14T12:54:36Z INFO rsgrad] Time used: 864.911523ms Then produces Note: The Fermi level is shiftted to 0.0 eV","breadcrumbs":"Wavefunction 1D » Example","id":"33","title":"Example"},"34":{"body":"rsgrad workfunc reads LOCPOT to calculate the work function. For further discussion about work function, please read this blog . Note: rsgrad workfunc does not show the vacuum level directly, hence you need to find it by hovering on the step of the work function. Take the work function above as an example, the vacuum level should be about 4.048eV around 40Å.","breadcrumbs":"Workfunction » Workfunction","id":"34","title":"Workfunction"},"35":{"body":"$ rsgrad workfunc --help\nrsgrad-workfunc\nCalculate work-function from LOCPOT file, OUTCAR is also needed to get the Fermi level. The work function is calculated by plannar integration of the data cube in LOCPOT. The selected axis\nshould be perpendicular to the other two axises. USAGE: rsgrad workfunc [OPTIONS] [LOCPOT] ARGS: LOCPOT file path. Turn on 'LVHAR' in INCAR to get the electro-static potential saved it [default: ./LOCPOT] OPTIONS: --axis Integration direction. e.g. if 'z' is provided, the XoY plane is integrated [default: z] [possible values: X, Y, Z] -h, --help Print help information -o, --htmlout Write the plot to html and view it in the web browser [default: ./workfunction.html] --outcar OUTCAR file path. This file is needed to get the E-fermi level and lattice properties [default: ./OUTCAR] --show Open default browser to see the plot immediately --to-inline-html Render the plot and print the rendered code to stdout --txtout Write the raw plot data as txt file in order to replot it with more advanced tools [default: locpot.txt]","breadcrumbs":"Workfunction » Help Message","id":"35","title":"Help Message"},"36":{"body":"In general, you don't need t provide additional arguments. $ rsgrad workfunc\n[2022-07-14T14:41:38Z INFO rsgrad::commands::workfunc] Reading \"./OUTCAR\"\n[2022-07-14T14:41:38Z INFO rsgrad::commands::workfunc] Reading electro-static potential data from \"./LOCPOT\"\n[2022-07-14T14:41:39Z INFO rsgrad::commands::workfunc] Writing raw plot data to \"locpot.txt\"\n[2022-07-14T14:41:39Z INFO rsgrad::commands::workfunc] Writing to \"./workfunction.html\"\n[2022-07-14T14:41:39Z INFO rsgrad] Time used: 1.352347116s","breadcrumbs":"Workfunction » Example","id":"36","title":"Example"},"37":{"body":"There are several operations that rsgrad pos can do Convert the fractional coordinates to Cartesian coordinates or convert reversely; Split the POSCAR and save the two parts; This command is useful when you want to calculate charge density difference and adsorption energy . Format the POSCAR and add element symbol tags to each atom.","breadcrumbs":"POSCAR » POSCAR","id":"37","title":"POSCAR"},"38":{"body":"$ rsgrad pos --help\nrsgrad-pos Operation(s) about POSCAR, including split it into two POSCARs USAGE: rsgrad pos [OPTIONS] [--] [POSCAR] ARGS: Specify the input POSCAR file [default: ./POSCAR] OPTIONS: -a, --a-name Splitted POSCAR path with selected atoms [default: POSCAR_A] -b, --b-name Splitted POSCAR path with complement of `a_name` [default: POSCAR_B] -c, --cartesian Cartesian coordinates is used in writting POSCAR --convert Convert POSCAR to cartesian coordinates or fractional coordinates --converted The target path of converted POSCAR [default: POSCAR_new] -h, --help Print help information -i, --select-indices ... Selects the indices to operate. Step indices start from '1', if '0' is given, all the structures will be selected. Step indices can be negative, where negative index means counting reversely. E.g. \"-i -2 -1 1 2 3\" means selecting the last two and the first three atom. --no-add-symbols-tags The symbols of each atom will not be written as comment in POSCAR --no-preserve-constraints Atom constraints will be dropped when writting POSCAR -s, --split Split POSCAR according to selected_indices","breadcrumbs":"POSCAR » Help Message","id":"38","title":"Help Message"},"39":{"body":"Format the POSCAR to add element symbol tags The original POSCAR of CO2: C O 1.0000000000000000 20.0000000000000000 0.0000000000000000 0.0000000000000000 0.0000000000000000 20.0000000000000000 0.0000000000000000 0.0000000000000000 0.0000000000000000 20.0000000000000000 C O 1 2\nDirect 0.5000000000000000 0.5000000000000000 -0.5000000000000000 0.5754584707965210 0.4974961803083730 0.5000000000000000 0.4249089651951450 0.5078477015701101 0.5000000000000000 Then run rsgrad pos POSCAR --convert $ rsgrad pos POSCAR --convert\n[2022-07-14T15:38:47Z INFO rsgrad::commands::pos] Reading POSCAR file \"POSCAR\" ...\n[2022-07-14T15:38:47Z INFO rsgrad::commands::pos] Converting it to \"POSCAR_new\"\n[2022-07-14T15:38:47Z INFO rsgrad::commands::pos] Done\n[2022-07-14T15:38:47Z INFO rsgrad] Time used: 1.96796ms The formatted file should be POSCAR_new C O 1.0000000 20.000000000 0.000000000 0.000000000 0.000000000 20.000000000 0.000000000 0.000000000 0.000000000 20.000000000 C O 1 2\nDirect 0.5000000000 0.5000000000 -0.5000000000 ! C-001 1 0.5754584708 0.4974961803 0.5000000000 ! O-001 2 0.4249089652 0.5078477016 0.5000000000 ! O-002 3 Convert POSCAR to Cartesian coordinates Just run rsgrad pos POSCAR --convert --cartesian $ rsgrad pos POSCAR --convert --cartesian\n[2022-07-14T15:40:33Z INFO rsgrad::commands::pos] Reading POSCAR file \"POSCAR\" ...\n[2022-07-14T15:40:33Z INFO rsgrad::commands::pos] Converting it to \"POSCAR_new\"\n[2022-07-14T15:40:33Z INFO rsgrad::commands::pos] Done\n[2022-07-14T15:40:33Z INFO rsgrad] Time used: 1.57861ms The converted file POSCAR_new should be like C O 1.0000000 20.000000000 0.000000000 0.000000000 0.000000000 20.000000000 0.000000000 0.000000000 0.000000000 20.000000000 C O 1 2\nCartesian 10.0000000000 10.0000000000 -10.0000000000 ! C-001 1 11.5091694159 9.9499236062 10.0000000000 ! O-001 2 8.4981793039 10.1569540314 10.0000000000 ! O-002 3 Split the POSCAR Let take the CO2 structure as the example again. Here we will take the C atom out to see what the operation does. The C atom index is 1, so we should run rsgrad pos POSCAR -s -i 1 $ rsgrad pos POSCAR -s -i 1\n[2022-07-14T15:49:32Z INFO rsgrad::commands::pos] Reading POSCAR file \"POSCAR\" ...\n[2022-07-14T15:49:32Z INFO rsgrad::commands::pos] Splitting it to \"POSCAR_A\" and \"POSCAR_B\" ...\n[2022-07-14T15:49:32Z INFO rsgrad::commands::pos] \"POSCAR_A\" contains\n[2022-07-14T15:49:32Z INFO rsgrad::commands::pos] C 1\n[2022-07-14T15:49:32Z INFO rsgrad::commands::pos] \"POSCAR_B\" contains\n[2022-07-14T15:49:32Z INFO rsgrad::commands::pos] O 2\n[2022-07-14T15:49:32Z INFO rsgrad::commands::pos] \"POSCAR_A\" written\n[2022-07-14T15:49:32Z INFO rsgrad::commands::pos] \"POSCAR_B\" written\n[2022-07-14T15:49:32Z INFO rsgrad] Time used: 2.11275ms The separated files should be like $ bat POSCAR_A POSCAR_B\n───────┬────────────────────────────────────────────────────────────────────────── │ File: POSCAR_A\n───────┼────────────────────────────────────────────────────────────────────────── 1 │ Generated by rsgrad, POSCAR with selected atoms 2 │ 1.0000000 3 │ 20.000000000 0.000000000 0.000000000 4 │ 0.000000000 20.000000000 0.000000000 5 │ 0.000000000 0.000000000 20.000000000 6 │ C 7 │ 1 8 │ Direct 9 │ 0.5000000000 0.5000000000 -0.5000000000 ! C-001 1\n───────┴──────────────────────────────────────────────────────────────────────────\n───────┬────────────────────────────────────────────────────────────────────────── │ File: POSCAR_B\n───────┼────────────────────────────────────────────────────────────────────────── 1 │ Generated by rsgrad, POSCAR complement 2 │ 1.0000000 3 │ 20.000000000 0.000000000 0.000000000 4 │ 0.000000000 20.000000000 0.000000000 5 │ 0.000000000 0.000000000 20.000000000 6 │ O 7 │ 2 8 │ Direct 9 │ 0.5754584708 0.4974961803 0.5000000000 ! O-001 1 10 │ 0.4249089652 0.5078477016 0.5000000000 ! O-002 2\n───────┴────────────────────────────────────────────────────────────────────────── The process schema:","breadcrumbs":"POSCAR » Examples","id":"39","title":"Examples"},"4":{"body":"To track the relaxation or MD process, use rsgrad rlx. This command is useful if you want to know the progress of geometry optimization (aka relaxation ) or molecular dynamics. This commands extract the following tags from OUTCAR: TOTEN TOTEN without entropy TOTEN difference between two ionic steps Maximum of atom forces (The negative EDIFFG is the threshold of this tag) The index of the atom with the maximum of force Number of SCF steps of each ionic step Time usage of each ionic step Volume of the cell Total magnetic moment","breadcrumbs":"Relaxation » Relaxation","id":"4","title":"Relaxation"},"40":{"body":"This command generates POTCAR according to POSCAR . The usage is simple: rsgrad pot in the directory with POSCAR presents. To use this command, a configuration file is required like: [functional-path]\nPAW_PBE = \"\"\nPAW_LDA = \"\" and you need to put it at ~/.rsgrad for Linux/macOS, and C:\\Users\\\\.rsgrad.toml for Windows. Note : rsgrad pot will give some hint if you have no idea on how to write the file. Then you can specify the element type in POSCAR , for example: Cd2 S2 HSE optimized 1.00000000000000 4.1704589747753724 0.0000000049514629 0.0000000000000000 -2.0852299788115007 3.6117232476351271 -0.0000000000000000 0.0000000000000000 -0.0000000000000000 6.7822968954189937 Cd S 2 2\nDirect 0.6666669999999968 0.3333330000000032 0.5001535716160643 0.3333330000000032 0.6666669999999968 0.0001535716160644 0.6666669999999968 0.3333330000000032 0.8768464283839381 0.3333330000000032 0.6666669999999968 0.3768464283839381 Finally rsgrad-pot will read the line \" Cd S \", and find the corresponding POTCAR and merge them. In some cases, several elements does not have \"standard\" POTCAR that without suffix. E.g. the K/POTCAR is not available for PBE functional. We provide two solutions for it: Write K_sv or other available K-related functionals in POSCAR Cd2 S2 HSE optimized 1.00000000000000 4.1704589747753724 0.0000000049514629 0.0000000000000000 -2.0852299788115007 3.6117232476351271 -0.0000000000000000 0.0000000000000000 -0.0000000000000000 6.7822968954189937 Cd K_sv 2 2\nDirect 0.6666669999999968 0.3333330000000032 0.5001535716160643 ... Use aliases field in .rsgrad.toml [functional-path]\n...\naliases = { K = \"K_sv\" } or [functional-path]\n...\n[functional-path.aliases]\nK = \"K_sv\"","breadcrumbs":"POTCAR » Pseudo Potential","id":"40","title":"Pseudo Potential"},"41":{"body":"rsgrad-pot\nGenerate the POTCAR according to POSCAR USAGE: rsgrad pot [OPTIONS] [FUNCTIONAL] ARGS: Specify the functional type, now only \"PAW_PBE\"(or \"paw_pbe\") and \"PAW_LDA\"(or \"paw_lda\") are available [default: PAW_PBE] OPTIONS: -c, --config Specify the configuration file, if left blank, rsgrad will read `.rsgrad.toml` at your home dir -h, --help Print help information -p, --poscar Specify the POSCAR file Note: the elements symbols' line should involve the specified valence configuration if you need. For example, if you need a `K_sv` POTCAR for `K`, just write `K_sv` in the POSCAR [default: ./POSCAR] -s, --save-in Specify where the `POTCAR` would be written [default: ./]","breadcrumbs":"POTCAR » Help Message","id":"41","title":"Help Message"},"42":{"body":"$ rsgrad pot\n[2023-10-20T16:19:48Z INFO rsgrad::settings] Reading rsgrad settings from \"/Users/ionizing/.rsgrad.toml\" ...\n[2023-10-20T16:19:48Z INFO rsgrad::settings] Checking rsgrad setting availability ...\n[2023-10-20T16:19:48Z INFO rsgrad::commands::pot] Reading POSCAR file \"../tests/POSCAR.CdS_HSE\" ...\n[2023-10-20T16:19:48Z INFO rsgrad::vasp_parsers::potcar] Reading POTCAR from \"/Users/ionizing/apps/vasp/pp/potpaw_PBE.54/Cd/POTCAR\"\n[2023-10-20T16:19:48Z INFO rsgrad::vasp_parsers::potcar] Reading POTCAR from \"/Users/ionizing/apps/vasp/pp/potpaw_PBE.54/S/POTCAR\"\n[2023-10-20T16:19:48Z INFO rsgrad::commands::pot] Writing POTCAR to \"./POTCAR\" ...\n[2023-10-20T16:19:48Z INFO rsgrad] Time used: 5.524643ms","breadcrumbs":"POTCAR » Example","id":"42","title":"Example"},"43":{"body":"This command (rsgrad tdm) calculates the transition dipole moment(tdm) between given bands, and then plot the peaks with plotly. Note: This command can only calculate the TDM between bands in same k-point. The inter-kpoint transition is not supported yet. Also, this commands calculates the TDM in reciprocal space by \\[ TDM_{i\\to j} = \\langle \\phi_j | e\\cdot\\vec{r} | \\phi_i \\rangle = e\\cdot\\frac{i\\hbar}{m_e\\Delta E_{ij}} \\langle \\phi_j | \\vec{p} | \\phi_i \\rangle \\] Also, this command only calculates the TDM if \\(j > i\\), otherwise it will ignore the invalid \\(i\\to j\\) pairs.","breadcrumbs":"Transition Dipole Moment » Transition Dipole Moment","id":"43","title":"Transition Dipole Moment"},"44":{"body":"$ rsgrad tdm --help\nrsgrad-tdm\nCalculate Transition Dipole Moment (TDM) between given bands. Note: This command can only calculate the TDM between bands in same k-point. The inter-kpoint\ntransition is not supported yet. Also, this commands calculates the TDM in reciprocal space by tdm_{i->j} = = i*ħ/(ΔE*m)* USAGE: rsgrad tdm [OPTIONS] --ibands ... --jbands ... OPTIONS: --barwidth Specify the width of bars in the center of peaks. (eV) [default: 0.1] --gamma-half Gamma Half direction of WAVECAR. You need to set this to 'x' or 'z' when processing WAVECAR produced by `vasp_gam` [possible values: x, z] -h, --help Print help information --htmlout Write the plot of TDM to html file [default: tdm_smeared.html] -i, --ibands ... Initial band indices, start from 1 -j, --jbands ... Final band indices, starts from 1 -k, --ikpoint K-point index, starts from 1 [default: 1] --npoints How many points in the x axis PER eV [default: 500] --peakout Write the TDM peaks to raw txt file [default: tdm_peaks.txt] -s, --ispin Spin index, 1 for up, 2 for down [default: 1] [possible values: 1, 2] --show Open the default browser to show the plot --sigma Smearing width, in eV [default: 0.05] --to-inline-html Print the inline HTML to stdout --txtout Write the summed and smeared TDM to raw txt file [default: tdm_smeared.txt] -v, --verbose Print the calculated TDM to screen -w, --wavecar WAVECAR file path [default: ./WAVECAR] --xmax Highest energy scale for tdm_smeared.txt, default for max(dE) + 2.0 --xmin Lowest energy scale for tdm_smeared.txt, default for min(dE) - 2.0","breadcrumbs":"Transition Dipole Moment » Help Message","id":"44","title":"Help Message"},"45":{"body":"The -i and -j arguments are required, or it will complain with error. $ rsgrad tdm -i 2 -j {3..5}\n[2022-08-10T07:26:46Z INFO rsgrad::commands::tdm] Reading \"./WAVECAR\"\n[2022-08-10T07:26:46Z INFO rsgrad::commands::tdm] Writing peaks info to \"tdm_peaks.txt\" ...\n[2022-08-10T07:26:46Z INFO rsgrad::commands::tdm] Writing smeared TDM data to \"tdm_smeared.txt\"\n[2022-08-10T07:26:46Z INFO rsgrad::commands::tdm] Writing plot to \"tdm_smeared.html\"\n[2022-08-10T07:26:46Z INFO rsgrad] Time used: 56.655387ms It produces the HTML like: You can view the \\(x\\), \\(y\\) and \\(z\\) components of each peak by hovering on the thin bars at the center of peaks. Note: If two peaks are in the same x position, one of them will be covered. Then the tdm_peaks.txt should be like: # iband jband E_i E_j ΔE Tx Ty Tz 2 3 -5.974 -3.675 2.298 1.311 2.556 0.000 2 4 -5.974 -3.675 2.298 2.556 1.311 0.000 2 5 -5.974 -0.975 4.999 0.000 0.000 5.309 And the tdm_smeared.txt should be like: # E(eV) Tx(Debye) Ty(Debye) Tz(Debye) 0.298325 0.007692 0.007692 0.001912 0.017295 0.300240 0.007706 0.007706 0.001914 0.017326 0.302155 0.007721 0.007721 0.001915 0.017357 0.304070 0.007736 0.007736 0.001917 0.017389 0.305985 0.007751 0.007751 0.001918 0.017420 0.307900 0.007766 0.007766 0.001920 0.017451\n...\n... Then you can plot the TDM peaks with other tools like OriginPro. If your WAVECAR is produced by vasp_gam, you'd better specify the gamma half direction by --gamma-half x or --gamma-half z, or rsgrad tdm will produce wrong results.","breadcrumbs":"Transition Dipole Moment » Example","id":"45","title":"Example"},"46":{"body":"This command (rsgrad gap) calculates the band gap and prints positions of VBM and CBM. There are two ways to run this command: Use WAVECAR only. All required information can be extracted from WAVECAR. Or use PROCAR and OUTCAR instead. PROCAR is read for the band energies, band occupations and k-point coordinates; OUTCAR is read for the Fermi level only. Note: Usually it's faster to parse results from WAVECAR. If your system is a non-SCF calculation for band structure, you may need to specify the correct Fermi level by rsgrad gap -e , the correct Fermi level can be obtained from the OUTCAR of SCF calculation.","breadcrumbs":"Gap » Gap","id":"46","title":"Gap"},"47":{"body":"$ rsgrad gap --help\nrsgrad-gap\nFind band gap and print positions of VBM and CBM USAGE: rsgrad gap [OPTIONS] OPTIONS: -e, --efermi Specify Fermi level, if left empty, this value would be read from WAVECAR or OUTCAR -h, --help Print help information -o, --outcar OUTCAR file name, this file is parsed to get Fermi level only [default: OUTCAR] -p, --procar PROCAR file name, OUTCAR is also needed to get Fermi level [default: PROCAR] -w, --wavecar WAVECAR file name, no more files needed [default: WAVECAR]","breadcrumbs":"Gap » Help Message","id":"47","title":"Help Message"},"48":{"body":"For metal system: [2022-12-01T11:30:49Z INFO rsgrad::commands::gap] Trying to parse \"WAVECAR\" ...\n---------------------------------------- Current system is Metal\n----------------------------------------\n[2022-12-01T11:30:49Z INFO rsgrad] Time used: 166.251241ms For non-spin-polarized direct gap system: [2022-12-01T11:37:15Z INFO rsgrad::commands::gap] Trying to parse \"WAVECAR\" ...\n-------------------------------------------------------------------------------- Current system has Direct Gap of 0.328 eV CBM @ k-point 1 of ( 0.000, 0.000, 0.000) , band 819 of 0.322 eV VBM @ k-point 1 of ( 0.000, 0.000, 0.000) , band 818 of -0.006 eV\n--------------------------------------------------------------------------------\n[2022-12-01T11:37:15Z INFO rsgrad] Time used: 253.556682ms For spin-polarized direct gap system: $ rsgrad gap\n[2022-12-01T11:38:16Z INFO rsgrad::commands::gap] Trying to parse \"WAVECAR\" ...\n-------------------------------------------------------------------------------- ==================== Gap Info For SPIN UP ==================== Current system has Direct Gap of 0.976 eV CBM @ k-point 1 of ( 0.000, 0.000, 0.000) , band 129 of 0.498 eV VBM @ k-point 1 of ( 0.000, 0.000, 0.000) , band 128 of -0.478 eV ==================== Gap Info For SPIN DOWN ==================== Current system has Direct Gap of 0.980 eV CBM @ k-point 1 of ( 0.000, 0.000, 0.000) , band 129 of 0.499 eV VBM @ k-point 1 of ( 0.000, 0.000, 0.000) , band 128 of -0.481 eV\n--------------------------------------------------------------------------------\n[2022-12-01T11:38:16Z INFO rsgrad] Time used: 31.744371ms For non-spin-polarized indirect gap system: $ rsgrad gap\n[2022-12-01T11:40:52Z INFO rsgrad::commands::gap] Trying to parse \"WAVECAR\" ...\n-------------------------------------------------------------------------------- Current system has Indirect Gap of 1.160 eV CBM @ k-point 25 of ( 0.000, 0.444, 0.444) , band 5 of 1.097 eV VBM @ k-point 17 of ( 0.000, 0.000, 0.000) , band 4 of -0.062 eV\n--------------------------------------------------------------------------------\n[2022-12-01T11:40:52Z INFO rsgrad] Time used: 22.565948ms","breadcrumbs":"Gap » Example","id":"48","title":"Example"},"49":{"body":"This command (rsgrad uc) converts input quantity to units representing same energy. Metric prefixes are supported, from Atto (a, 10-18) to Exa (E, 1018). Here are supported prefixes and corresponding acronyms: Metric prefix Acronym Base 10 atto a 10-18 femto f 10-15 pico p 10-12 nano n 10-9 micro μ 10-6 milli m 10-3 -- -- 100 Kilo K 103 Mega M 106 Giga G 109 Tera T 1012 Peta P 1015 exa E 1018 If you use acronyms, note that prefixes smaller than 1 (from a , atto to m , micro) must be lowercased whereas the prefixes lager than 1 (from K , Kilo to E , Exa) must be uppercased. Supported units: Unit Symbol Hartree Ha Wavenumber cm-1 Temperature(Kelvin) K Calorie per mole Cal/mol Joule per mole J/mol Wavelength m Period s Electron volt eV Frequency Hz","breadcrumbs":"UnitConversion » UnitConversion","id":"49","title":"UnitConversion"},"5":{"body":"$ rsgrad rlx -h\nrsgrad-rlx\nTracking relaxation or MD progress USAGE: rsgrad rlx [OPTIONS] [OUTCAR] ARGS: Specify the input OUTCAR file [default: ./OUTCAR] OPTIONS: -a, --favg Prints averaged total force in eV/A -e, --toten Prints TOTEN in eV -h, --help Print help information -i, --fmidx Prints the index of ion with maximum total force load. Starts from 1 --no-fmax Don't print maximum total force in A^3 --no-lgde Don't print Log10(delta(TOTEN without entropy)) --no-magmom Don't print total magnetic moment in muB --no-nscf Don't print number of SCF iteration for each ionic step --no-time Don't print time elapsed for each ionic step in minutes --no-totenz Don't print TOTEN without entropy in eV -p, --poscar Specify the input POSCAR file [default: ./POSCAR] -v, --volume Prints lattice volume in A^3 -x, --fmaxis Prints the axis where the strongest total force component lies on. [XYZ]","breadcrumbs":"Relaxation » Help Message","id":"5","title":"Help Message"},"50":{"body":"$ rsgrad uc\nConversion between various energy units Usage: rsgrad uc [INPUT]... Arguments: [INPUT]... Input energy quantity to be converted. Multiple input are supported Options: -h, --help Print help Try `rsgrad uc 298K` to see what happens.","breadcrumbs":"UnitConversion » Help Message","id":"50","title":"Help Message"},"51":{"body":"$ rsgrad uc 298K\n==================== Processing input \"298K\" ==================== 298.000000 K == 943.709369 μHa 298.000000 K == 207.125149 cm-1 298.000000 K == 298.000000 K 298.000000 K == 592.202785 Cal/mol 298.000000 K == 2.477776 KJ/mol 298.000000 K == 48.281101 μm 298.000000 K == 161.048425 fs 298.000000 K == 25.679653 meV 298.000000 K == 6.209312 THz\n================================================================================ [2024-09-11T07:21:07Z INFO rsgrad] Time used: 470.398µs You can also input multiple quantities at a time $ rsgrad uc 298K 25meV 300THz\n==================== Processing input \"298K\" ==================== 298.000000 K == 161.048425 fs 298.000000 K == 207.125149 cm-1 298.000000 K == 2.477776 KJ/mol 298.000000 K == 25.679653 meV 298.000000 K == 48.281101 μm 298.000000 K == 943.709369 μHa 298.000000 K == 592.202785 Cal/mol 298.000000 K == 6.209312 THz 298.000000 K == 298.000000 K\n================================================================================ ==================== Processing input \"25meV\" ==================== 25.000000 meV == 165.426708 fs 25.000000 meV == 201.643250 cm-1 25.000000 meV == 2.412198 KJ/mol 25.000000 meV == 25.000000 meV 25.000000 meV == 49.593677 μm 25.000000 meV == 918.732590 μHa 25.000000 meV == 576.529191 Cal/mol 25.000000 meV == 6.044973 THz 25.000000 meV == 290.112953 K\n================================================================================ ==================== Processing input \"300THz\" ==================== 300.000000 THz == 3.333333 fs 300.000000 THz == 10.007154 Kcm-1 300.000000 THz == 119.712599 KJ/mol 300.000000 THz == 1.240700 eV 300.000000 THz == 999.308150 nm 300.000000 THz == 45.594872 mHa 300.000000 THz == 28.611998 KCal/mol 300.000000 THz == 300.000000 THz 300.000000 THz == 14.397729 KK\n================================================================================ [2024-09-11T07:27:53Z INFO rsgrad] Time used: 544.171µs","breadcrumbs":"UnitConversion » Examples","id":"51","title":"Examples"},"52":{"body":"We are happy that you reach here. As an open-source project, rsgrad welcomes feedback. If you have want to add features to rsgrad, just open an issue at GitHub Issues . We also created a feature-requests list, you can follow it at this page . If rsgrad complains something or produces wrong result, just open an issue at GitHub Issues . We are grateful if you can provide the input files in order that we can reproduce the issue conveniently, thus solve the issue as soon as possible. If you are interested in rsgrad and want to contribute to the source code, just fork rsgrad and create pull requests at Pull Requests . We are super grateful if you can contribute to rsgrad.","breadcrumbs":"Feedback » Feedback","id":"52","title":"Feedback"},"53":{"body":"Qijing Zheng : The WAVECAR related function are written with the help of this code. pymatgen and ASE : Some test files are copied from these two repositories. RustFFT and ndrustfft : These two crates make wav3d and wav1d become possible. plotly.rs : This crate makes the visualization possible.","breadcrumbs":"Acknowledgements » Acknowledgements","id":"53","title":"Acknowledgements"},"6":{"body":"","breadcrumbs":"Relaxation » Example","id":"6","title":"Example"},"7":{"body":"The rsgrad dos command calculates the Density of States (DOS) of current system. rsgrad DOES NOT read the DOSCAR , but calculates the DOS from PROCAR instead by $$ D(E) = \\frac{1}{V} \\sum_{i=1}^{N} \\delta(E-E(\\mathbf{k}_i)) $$ Because rsgrad uses arbitrary unit, the factor \\(\\frac{1}{V}\\) is omitted. The \\(\\delta(x)\\) is replaced by Gaussian function or Lorentzian function: $$ g(x) = \\frac{1}{\\sigma\\sqrt{2\\pi}} \\exp \\left( -\\frac{1}{2} \\frac{(x-\\mu)^2}{\\sigma^2} \\right) \\\\ l(x) = \\frac{1}{\\pi} \\frac{\\sigma}{(x-\\mu)^2 + \\sigma^2} $$ where \\(\\mu\\) is \\(E(\\mathbf{k}_i)\\) and \\(\\sigma\\) is sigma of configuration in the implementation. This method makes it easier to calculate projected DOS with projection of specific atoms, angular moments and k-points. However, this method sometimes differs from DOSCAR with ISMEAR = -5. For detailed explaination, see the document here . The OUTCAR is also needed to get the Fermi level.","breadcrumbs":"Density of States » Density of States","id":"7","title":"Density of States"},"8":{"body":"$ rsgrad dos -h\nrsgrad-dos\nCalculate density of states from PROCAR and OUTCAR USAGE: rsgrad dos [OPTIONS] OPTIONS: -c, --config Projected DOS configuration file path --gen-template Generate projected DOS configuration template -h, --help Print help information --htmlout Save the projected DOS plot as HTML. Then you can view it in the browser [default: dos.html] --outcar OUTCAR path [default: ./OUTCAR] --procar PROCAR path [default: ./PROCAR] --show Open the browser and show the plot immediately --show-brief Print brief info of PROCAR, this may be helpful when you write the configuration --to-inline-html Render the plot and print the rendered code to stdout --txtout Save the raw data of projected DOS. Then you can replot it with more advanced tools [default: dos_raw.txt] --xlim Set the x-range of the plot [default: -1 6]","breadcrumbs":"Density of States » Help Message","id":"8","title":"Help Message"},"9":{"body":"The configuration template can be generated by running rsgrad dos --gen-template. The following configuration is written to pband.toml by default: # rsgrad DOS configuration in toml format.\n# multiple tokens inside string are seperated by whitespace\nmethod = \"Gaussian\" # smearing method\nsigma = 0.05 # smearing width, (eV)\nprocar = \"PROCAR\" # PROCAR path\noutcar = \"OUTCAR\" # OUTCAR path\ntxtout = \"dos_raw.txt\" # save the raw data as \"dos_raw.txt\"\nhtmlout = \"dos.html\" # save the pdos plot as \"dos.html\"\ntotdos = true # plot the total dos\nfill = true # fill the plot to x axis or not\nxlim = [-1, 6] # x-range of plot [pdos.plot1] # One label produces one plot, the labels CANNOT be repetitive. # This label is 'plot1', to add more pdos, write '[pdos.plot2]' and so on.\nkpoints = \"1 3..7 -1\" # selects 1 3 4 5 6 7 and the last kpoint for pdos plot.\natoms = \"1 3..7 -1\" # selects 1 3 4 5 6 7 and the last atoms' projection for pdos plot.\norbits = \"s px dxy\" # selects the s px and dx orbits' projection for pdos plot.\nfactor = 1.01 # the factor multiplied to this pdos [pdos.plot2] # One label produces one plot, the labels CANNOT be repetitive. # This label is 'plot2', to add more pdos, write '[pdos.plot2]' and so on.\nkpoints = \"1 3..7 -1\" # selects 1 3 4 5 6 7 and the last kpoint for pdos plot.\natoms = \"1 3..7 -1\" # selects 1 3 4 5 6 7 and the last atoms' projection for pdos plot.\norbits = \"s px dxy\" # selects the s px and dx orbits' projection for pdos plot.\nfactor = 1.01 # the factor multiplied to this pdos # The fields can be left blank, if you want select all the components for some fields,\n# just comment them. You can comment fields with '#'","breadcrumbs":"Density of States » Configuration Template","id":"9","title":"Configuration 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