Unify reference format

examples/01_LSWT_CoRh2O4.jl

@@ -2,8 +2,8 @@
 #
 # This tutorial introduces Sunny through its features for performing
 # conventional spin wave theory calculations. We consider the crystal CoRh₂O₄
-# and reproduce the calculations of [Ge et al., Phys. Rev. B 96,
-# 064413](https://doi.org/10.1103/PhysRevB.96.064413).
+# and reproduce the calculations of [Ge et al., Phys. Rev. B **96**,
+# 064413 (2017)](https://doi.org/10.1103/PhysRevB.96.064413).
 
 # ### Get Julia and Sunny
 # 

examples/03_LSWT_SU3_FeI2.jl

@@ -8,7 +8,7 @@
 # that is observable in neutron scattering, and cannot be described by a
 # dipole-only model. We will use the linear spin wave theory of SU(3) coherent
 # states (i.e. 2-flavor bosons) to model the magnetic spectrum of FeI₂. The
-# original study was performed in [Bai et al., Nature Physics 17, 467–472
+# original study was performed in [Bai et al., Nature Physics **17**, 467–472
 # (2021)](https://doi.org/10.1038/s41567-020-01110-1).
 #
 # ```@raw html

examples/spinw_tutorials/SW13_LiNiPO4.jl

@@ -21,8 +21,8 @@ types = ["Ni"]
 cryst = Crystal(latvecs, positions, 62; types)
 view_crystal(cryst)
 
-# Create a system with exchange parameters taken from [T. Jensen, et al., PRB
-# **79**, 092413 (2009)](https://doi.org/10.1103/PhysRevB.79.092413). The
+# Create a system with exchange parameters taken from [T. Jensen, et al., Phys.
+# Rev. B **79**, 092413 (2009)](https://doi.org/10.1103/PhysRevB.79.092413). The
 # corrected anisotropy values are taken from the thesis of T. Jensen. The mode
 # `:dipole_uncorrected` avoids a [classical-to-quantum rescaling factor](@ref
 # "Interaction Renormalization") of anisotropy strengths, as needed for

examples/spinw_tutorials/SW14_YVO3.jl

@@ -23,11 +23,11 @@ positions = [[0, 0, 0], [0, 0, 1/2]]
 types = ["V", "V"]
 cryst = Crystal(latvecs, positions, 1; types)
 
-# Create a system following the model of [C. Ulrich, et al. PRL **91**, 257202
-# (2003)](https://doi.org/10.1103/PhysRevLett.91.257202). The mode
-# `:dipole_uncorrected` avoids a [classical-to-quantum rescaling factor](@ref
-# "Interaction Renormalization") of anisotropy strengths, as needed for
-# consistency with the original fits.
+# Create a system following the model of [C. Ulrich, et al. Phys. Rev. Lett.
+# **91**, 257202 (2003)](https://doi.org/10.1103/PhysRevLett.91.257202). The
+# mode `:dipole_uncorrected` avoids a [classical-to-quantum rescaling
+# factor](@ref "Interaction Renormalization") of anisotropy strengths, as needed
+# for consistency with the original fits.
 
 moments = [1 => Moment(s=1/2, g=2), 2 => Moment(s=1/2, g=2)]
 sys = System(cryst, moments, :dipole_uncorrected; dims=(2,2,1))

src/FormFactor.jl

@@ -96,14 +96,15 @@ Two special, ``𝐪``-independent form factor values are available:
 as a perfect point particle, while the second zeros all contributions from the
 magnetic ion.
 
-## References:
+## References
 
-1. [P. J. Brown, The Neutron Data Booklet, 2nd ed., Sec. 2.5 Magnetic Form
-   Factors (2003)](https://www.ill.eu/sites/ccsl/ffacts/ffachtml.html)
+1. [P. J. Brown, The Neutron Data Booklet, 2nd ed., Sec. 2.5 _Magnetic Form
+   Factors_ (2003)](https://www.ill.eu/sites/ccsl/ffacts/ffachtml.html).
 2. Coefficient tables in [McPhase
-   documentation](https://www2.cpfs.mpg.de/~rotter/homepage_mcphase/manual/node137.html)
-3. [K. Kobayashi, T. Nagao, M. Ito, Acta Cryst. A, 67 pp 473–480
-   (2011)](https://doi.org/10.1107/S010876731102633X)
+   documentation](https://www2.cpfs.mpg.de/~rotter/homepage_mcphase/manual/node137.html).
+3. [K. Kobayashi, T. Nagao, M. Ito, _Radial integrals for the magnetic form
+   factor of 5d transition elements_, Acta Cryst. A, **67**, 473–480
+   (2011)](https://doi.org/10.1107/S010876731102633X).
 """
 function FormFactor(ion::String; g_lande=2)
     if !haskey(radial_integral_coefficients, ion)

src/Integrators.jl

@@ -45,10 +45,11 @@ the dipole in analogy to the vector cross product ``S × 𝐁``. The coupling to
 the thermal bath maps as ``λ̃ = |𝐒| λ``. Note, therefore, that the scaling of
 the `damping` parameter varies subtly between `:dipole` and `:SUN` modes.
 
-## References:
+## References
 
-1. [D. Dahlbom et al., Phys. Rev. B 106, 235154
-   (2022)](https://arxiv.org/abs/2209.01265).
+1. [D. Dahlbom et al., _Langevin dynamics of generalized spins as SU(N) coherent
+   states_, Phys. Rev. B **106**, 235154
+   (2022)](https://doi.org/10.1103/PhysRevB.106.235154).
 """
 mutable struct Langevin
     dt      :: Float64
@@ -99,10 +100,11 @@ or its generalization to SU(_N_) coherent states [1]. One call to the
 This integration scheme is exactly symplectic and eliminates energy drift over
 arbitrarily long simulation trajectories.
 
-## References:
+## References
 
-1. [H. Zhang and C. D. Batista, Phys. Rev. B 104, 104409
-   (2021)](https://arxiv.org/abs/2106.14125).
+1. [H. Zhang and C. D. Batista, _Classical spin dynamics based on SU(N) coherent
+   states_, Phys. Rev. B **104**, 104409
+   (2021)](https://doi.org/10.1103/PhysRevB.104.104409).
 """
 mutable struct ImplicitMidpoint
     dt      :: Float64

src/KPM/SpinWaveTheoryKPM.jl

@@ -21,9 +21,9 @@ Reasonable starting points are `1e-1` (more speed) or `1e-2` (more accuracy).
     particular, KPM may mask intensities that arise near the Goldstone modes of
     an ordered state with continuous symmetry.
 
-## References:
+## References
 
-1. H. Lane et al., Kernel Polynomial Method for Linear Spin Wave Theory (2023)
+1. H. Lane et al., _Kernel Polynomial Method for Linear Spin Wave Theory_ (2023)
    [[arXiv:2312.08349v3](https://arxiv.org/abs/2312.08349)].
 """
 struct SpinWaveTheoryKPM