RCWA calculations on Binder

binder/apt.txt

@@ -0,0 +1,8 @@
+make
+git
+gcc
+g++
+libopenblas-dev
+libfftw3-dev
+libsuitesparse-dev
+libboost-all-dev

binder/postBuild

@@ -0,0 +1,7 @@
+set -ex
+
+git clone https://github.com/phoebe-p/S4
+cd S4
+make S4_pyext
+cd ..
+rm -rf S4

docs/solcore-workshop/notebooks/2-Efficiency_limits.html

@@ -307,7 +307,7 @@ <h3 class="anchored" data-anchor-id="solar-spectrum">Solar Spectrum</h3>
 <span id="cb1-6"><a href="#cb1-6" aria-hidden="true" tabindex="-1"></a><span class="co"># Setup the AM1.5G solar spectrum</span></span>
 <span id="cb1-7"><a href="#cb1-7" aria-hidden="true" tabindex="-1"></a>wl <span class="op">=</span> np.linspace(<span class="dv">300</span>, <span class="dv">4000</span>, <span class="dv">4000</span>) <span class="op">*</span> <span class="fl">1e-9</span>    <span class="co"># wl contains the x-coordinate in wavelength</span></span>
 <span id="cb1-8"><a href="#cb1-8" aria-hidden="true" tabindex="-1"></a>am15g <span class="op">=</span> LightSource(source_type<span class="op">=</span><span class="st">'standard'</span>, x<span class="op">=</span>wl<span class="op">*</span><span class="fl">1e9</span>, version<span class="op">=</span><span class="st">'AM1.5g'</span>,</span>
-<span id="cb1-9"><a href="#cb1-9" aria-hidden="true" tabindex="-1"></a>                    outputs<span class="op">=</span><span class="st">"power_density_per_nm"</span>)</span>
+<span id="cb1-9"><a href="#cb1-9" aria-hidden="true" tabindex="-1"></a>                    output_units<span class="op">=</span><span class="st">"power_density_per_nm"</span>)</span>
 <span id="cb1-10"><a href="#cb1-10" aria-hidden="true" tabindex="-1"></a></span>
 <span id="cb1-11"><a href="#cb1-11" aria-hidden="true" tabindex="-1"></a>plt.figure()</span>
 <span id="cb1-12"><a href="#cb1-12" aria-hidden="true" tabindex="-1"></a>plt.title(<span class="st">'Spectral Irradiance'</span>)</span>
@@ -439,7 +439,7 @@ <h3 class="anchored" data-anchor-id="calculating-the-trivich-flinn-efficiency-li
 <div class="cell" data-executetime="{&quot;end_time&quot;:&quot;2023-07-31T07:51:28.702500Z&quot;,&quot;start_time&quot;:&quot;2023-07-31T07:51:28.515220Z&quot;}" data-execution_count="35">
 <div class="sourceCode cell-code" id="cb17"><pre class="sourceCode python code-with-copy"><code class="sourceCode python"><span id="cb17-1"><a href="#cb17-1" aria-hidden="true" tabindex="-1"></a>plt.figure()</span>
 <span id="cb17-2"><a href="#cb17-2" aria-hidden="true" tabindex="-1"></a>plt.title(<span class="st">'Trivich-Flinn Single Junction Efficiency Limit'</span>)</span>
-<span id="cb17-3"><a href="#cb17-3" aria-hidden="true" tabindex="-1"></a>plt.plot(eg, <span class="dv">100</span><span class="op">*</span>eg<span class="op">*</span>jsc<span class="op">/</span>b,label<span class="op">=</span><span class="st">'AM1.5G'</span>)  <span class="co"># Divide by 10 to convert from A.m^-2 to mA.cm^-2</span></span>
+<span id="cb17-3"><a href="#cb17-3" aria-hidden="true" tabindex="-1"></a>plt.plot(eg, <span class="dv">100</span><span class="op">*</span>eg<span class="op">*</span>jsc<span class="op">/</span>b,label<span class="op">=</span><span class="st">'AM1.5G'</span>)</span>
 <span id="cb17-4"><a href="#cb17-4" aria-hidden="true" tabindex="-1"></a>plt.xlim(<span class="fl">0.5</span>, <span class="fl">2.5</span>)</span>
 <span id="cb17-5"><a href="#cb17-5" aria-hidden="true" tabindex="-1"></a>plt.xlabel(<span class="st">'Band Gap energy (eV)'</span>)</span>
 <span id="cb17-6"><a href="#cb17-6" aria-hidden="true" tabindex="-1"></a>plt.ylabel(<span class="st">'Efficiency (%)'</span>)</span>

docs/solcore-workshop/notebooks/7-InGaP_Si_planar.html

@@ -281,7 +281,7 @@ <h2 class="anchored" data-anchor-id="defining-materials-layers-and-junctions">De
 <p>The paper referenced above uses a double-layer anti-reflection coating (ARC) made of MgF<span class="math inline">\(_2\)</span> and ZnS. As in the previous example, we use the interface to the refractiveindex.info database to select optical constant data from specific sources, and define Solcore materials using this data. The III-V materials are taken from Solcore’s own material database.</p>
 <p>Note that for the epoxy/glass layer, we use only a single material (BK7 glass). The epoxy and glass used in the paper have the same refractive index (n = 1.56), so we can use a single material with an appropriate refractive index to represent them.</p>
 <div class="cell" data-execution_count="66">
-<div class="sourceCode cell-code" id="cb2"><pre class="sourceCode python code-with-copy"><code class="sourceCode python"><span id="cb2-1"><a href="#cb2-1" aria-hidden="true" tabindex="-1"></a><span class="co"># download_db() # uncomment to download database</span></span>
+<div class="sourceCode cell-code" id="cb2"><pre class="sourceCode python code-with-copy"><code class="sourceCode python"><span id="cb2-1"><a href="#cb2-1" aria-hidden="true" tabindex="-1"></a>download_db() <span class="co"># uncomment to download database</span></span>
 <span id="cb2-2"><a href="#cb2-2" aria-hidden="true" tabindex="-1"></a></span>
 <span id="cb2-3"><a href="#cb2-3" aria-hidden="true" tabindex="-1"></a>MgF2_pageid <span class="op">=</span> search_db(os.path.join(<span class="st">"MgF2"</span>, <span class="st">"Rodriguez-de Marcos"</span>))[<span class="dv">0</span>][<span class="dv">0</span>]<span class="op">;</span></span>
 <span id="cb2-4"><a href="#cb2-4" aria-hidden="true" tabindex="-1"></a>ZnS_pageid <span class="op">=</span> search_db(os.path.join(<span class="st">"ZnS"</span>, <span class="st">"Querry"</span>))[<span class="dv">0</span>][<span class="dv">0</span>]<span class="op">;</span></span>