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SunnySuite · Sep 20, 2024 · d5dede3 · d5dede3
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diff --git a/dev/.documenter-siteinfo.json b/dev/.documenter-siteinfo.json
@@ -1 +1 @@
-{"documenter":{"julia_version":"1.10.5","generation_timestamp":"2024-09-20T17:22:00","documenter_version":"1.7.0"}}
+{"documenter":{"julia_version":"1.10.5","generation_timestamp":"2024-09-20T19:53:17","documenter_version":"1.7.0"}}
diff --git a/dev/assets/notebooks/05_MC_Ising.ipynb b/dev/assets/notebooks/05_MC_Ising.ipynb
@@ -42,7 +42,7 @@
     "Create a `System` of spin dipoles. Following the Ising convention, we\n",
     "will restrict the dipoles to $±1$ along the global $\\hat{z}$-axis. Select\n",
     "$g=-1$ so that the Zeeman coupling between external field $𝐁$ and spin\n",
-    "dipole $𝐬$ is $-𝐁⋅𝐬$. The system size is 128×128."
+    "dipole $𝐒$ is $-𝐁⋅𝐒$. The system size is 128×128."
    ],
    "metadata": {}
   },
@@ -117,7 +117,7 @@
     "consists of, on average, one trial update per spin in the system. Each\n",
     "proposed update is accepted or rejected according to the Metropolis acceptance\n",
     "probability. As its name suggests, the `propose_flip` function will\n",
-    "only propose pure spin flips, $𝐬 \\rightarrow -𝐬$."
+    "only propose pure spin flips, $𝐒 \\rightarrow -𝐒$."
    ],
    "metadata": {}
   },

diff --git a/dev/assets/notebooks/06_CP2_Skyrmions.ipynb b/dev/assets/notebooks/06_CP2_Skyrmions.ipynb
@@ -52,7 +52,7 @@
    "cell_type": "markdown",
    "source": [
     "Create a spin `System` containing $L×L$ cells. Following previous\n",
-    "worse, select $g=-1$ so that the Zeeman coupling has the form $-𝐁⋅𝐬$."
+    "worse, select $g=-1$ so that the Zeeman coupling has the form $-𝐁⋅𝐒$."
    ],
    "metadata": {}
   },

diff --git a/dev/assets/notebooks/SW13_LiNiPO4.ipynb b/dev/assets/notebooks/SW13_LiNiPO4.ipynb
@@ -68,7 +68,6 @@
    "outputs": [],
    "cell_type": "code",
    "source": [
-    "S = 3/2\n",
     "sys = System(cryst, [1 => Moment(s=1, g=2)], :dipole_large_s)\n",
     "Jbc =  1.036\n",
     "Jb  =  0.6701\n",

diff --git a/dev/assets/scripts/SW13_LiNiPO4.jl b/dev/assets/scripts/SW13_LiNiPO4.jl
@@ -10,7 +10,6 @@ types = ["Ni"]
 cryst = Crystal(latvecs, positions, 62, setting=""; types)
 view_crystal(cryst)
 
-S = 3/2
 sys = System(cryst, [1 => Moment(s=1, g=2)], :dipole_large_s)
 Jbc =  1.036
 Jb  =  0.6701

diff --git a/dev/examples/01_LSWT_CoRh2O4-3703d499.png b/dev/examples/01_LSWT_CoRh2O4-3703d499.png
diff --git a/dev/examples/01_LSWT_CoRh2O4-4e7ea387.png b/dev/examples/01_LSWT_CoRh2O4-4e7ea387.png
diff --git a/dev/examples/01_LSWT_CoRh2O4-f235b95e.png → dev/examples/01_LSWT_CoRh2O4-9fc04702.png b/dev/examples/01_LSWT_CoRh2O4-f235b95e.png → dev/examples/01_LSWT_CoRh2O4-9fc04702.png
diff --git a/dev/examples/01_LSWT_CoRh2O4-a02a5316.png b/dev/examples/01_LSWT_CoRh2O4-a02a5316.png
diff --git a/dev/examples/01_LSWT_CoRh2O4-a5e6eb9b.png b/dev/examples/01_LSWT_CoRh2O4-a5e6eb9b.png
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diff --git a/dev/examples/01_LSWT_CoRh2O4-f5fbbf16.png b/dev/examples/01_LSWT_CoRh2O4-f5fbbf16.png
diff --git a/dev/examples/01_LSWT_CoRh2O4-f725892f.png b/dev/examples/01_LSWT_CoRh2O4-f725892f.png
diff --git a/dev/examples/01_LSWT_CoRh2O4.html b/dev/examples/01_LSWT_CoRh2O4.html
diff --git a/dev/examples/02_LLD_CoRh2O4-00e5c6e3.png b/dev/examples/02_LLD_CoRh2O4-00e5c6e3.png
diff --git a/dev/examples/02_LLD_CoRh2O4-0731477b.png b/dev/examples/02_LLD_CoRh2O4-0731477b.png
diff --git a/dev/examples/02_LLD_CoRh2O4-089799fa.png b/dev/examples/02_LLD_CoRh2O4-089799fa.png
diff --git a/dev/examples/02_LLD_CoRh2O4-16dfa128.png b/dev/examples/02_LLD_CoRh2O4-16dfa128.png
diff --git a/dev/examples/02_LLD_CoRh2O4-2683b131.png b/dev/examples/02_LLD_CoRh2O4-2683b131.png
diff --git a/dev/examples/02_LLD_CoRh2O4-3db81b04.png b/dev/examples/02_LLD_CoRh2O4-3db81b04.png
diff --git a/dev/examples/02_LLD_CoRh2O4-5b947802.png b/dev/examples/02_LLD_CoRh2O4-5b947802.png
diff --git a/dev/examples/02_LLD_CoRh2O4-760c5fea.png b/dev/examples/02_LLD_CoRh2O4-760c5fea.png
diff --git a/dev/examples/02_LLD_CoRh2O4-8629401a.png b/dev/examples/02_LLD_CoRh2O4-8629401a.png
diff --git a/dev/examples/02_LLD_CoRh2O4-898ef19e.png b/dev/examples/02_LLD_CoRh2O4-898ef19e.png
diff --git a/dev/examples/02_LLD_CoRh2O4-b28b116b.png b/dev/examples/02_LLD_CoRh2O4-b28b116b.png
diff --git a/dev/examples/02_LLD_CoRh2O4-b69b161a.png b/dev/examples/02_LLD_CoRh2O4-b69b161a.png
diff --git a/dev/examples/02_LLD_CoRh2O4-c0cffd59.png b/dev/examples/02_LLD_CoRh2O4-c0cffd59.png
diff --git a/dev/examples/02_LLD_CoRh2O4-f71b044c.png b/dev/examples/02_LLD_CoRh2O4-f71b044c.png
diff --git a/dev/examples/02_LLD_CoRh2O4.html b/dev/examples/02_LLD_CoRh2O4.html
diff --git a/dev/examples/03_LSWT_SU3_FeI2.html b/dev/examples/03_LSWT_SU3_FeI2.html
@@ -127,4 +127,4 @@
 res = domain_average(cryst, path; rotations, weights) do path_rotated
     intensities(swt, path_rotated; energies, kernel)
 end
-plot_intensities(res; units, colormap=:viridis, title=&quot;Domain Averaged Intensities&quot;)</code></pre><img src="03_LSWT_SU3_FeI2-d3f7d87e.png" alt="Example block output"/><p>This result can be directly compared to experimental neutron scattering data from <a href="https://doi.org/10.1038/s41567-020-01110-1">Bai et al.</a></p><img src="https://raw.githubusercontent.com/SunnySuite/Sunny.jl/main/docs/src/assets/FeI2_intensity.jpg"><p>(The publication figure used a non-standard coordinate system to label the wave vectors.)</p><p>To get this agreement, the theory of SU(3) coherent states is essential. The lower band has large quadrupolar character, and arises from the strong easy-axis anisotropy of FeI₂.</p><p>An interesting exercise is to repeat the same study, but using <code>:dipole</code> mode instead of <code>:SUN</code>. That alternative choice would constrain the coherent state dynamics to the space of dipoles only, and the flat band of single-ion bound states would be missing.</p></article><nav class="docs-footer"><a class="docs-footer-prevpage" href="02_LLD_CoRh2O4.html">« 2. Landau-Lifshitz dynamics of CoRh₂O₄ at finite <em>T</em></a><a class="docs-footer-nextpage" href="04_GSD_FeI2.html">4. Generalized spin dynamics of FeI₂ at finite <em>T</em> »</a><div class="flexbox-break"></div><p class="footer-message">Powered by <a href="https://github.com/JuliaDocs/Documenter.jl">Documenter.jl</a> and the <a href="https://julialang.org/">Julia Programming Language</a>.</p></nav></div><div class="modal" id="documenter-settings"><div class="modal-background"></div><div class="modal-card"><header class="modal-card-head"><p class="modal-card-title">Settings</p><button class="delete"></button></header><section class="modal-card-body"><p><label class="label">Theme</label><div class="select"><select id="documenter-themepicker"><option value="auto">Automatic (OS)</option><option value="documenter-light">documenter-light</option><option value="documenter-dark">documenter-dark</option><option value="catppuccin-latte">catppuccin-latte</option><option value="catppuccin-frappe">catppuccin-frappe</option><option value="catppuccin-macchiato">catppuccin-macchiato</option><option value="catppuccin-mocha">catppuccin-mocha</option></select></div></p><hr/><p>This document was generated with <a href="https://github.com/JuliaDocs/Documenter.jl">Documenter.jl</a> version 1.7.0 on <span class="colophon-date" title="Friday 20 September 2024 17:21">Friday 20 September 2024</span>. Using Julia version 1.10.5.</p></section><footer class="modal-card-foot"></footer></div></div></div></body></html>
+plot_intensities(res; units, colormap=:viridis, title=&quot;Domain Averaged Intensities&quot;)</code></pre><img src="03_LSWT_SU3_FeI2-d3f7d87e.png" alt="Example block output"/><p>This result can be directly compared to experimental neutron scattering data from <a href="https://doi.org/10.1038/s41567-020-01110-1">Bai et al.</a></p><img src="https://raw.githubusercontent.com/SunnySuite/Sunny.jl/main/docs/src/assets/FeI2_intensity.jpg"><p>(The publication figure used a non-standard coordinate system to label the wave vectors.)</p><p>To get this agreement, the theory of SU(3) coherent states is essential. The lower band has large quadrupolar character, and arises from the strong easy-axis anisotropy of FeI₂.</p><p>An interesting exercise is to repeat the same study, but using <code>:dipole</code> mode instead of <code>:SUN</code>. That alternative choice would constrain the coherent state dynamics to the space of dipoles only, and the flat band of single-ion bound states would be missing.</p></article><nav class="docs-footer"><a class="docs-footer-prevpage" href="02_LLD_CoRh2O4.html">« 2. Landau-Lifshitz dynamics of CoRh₂O₄ at finite <em>T</em></a><a class="docs-footer-nextpage" href="04_GSD_FeI2.html">4. Generalized spin dynamics of FeI₂ at finite <em>T</em> »</a><div class="flexbox-break"></div><p class="footer-message">Powered by <a href="https://github.com/JuliaDocs/Documenter.jl">Documenter.jl</a> and the <a href="https://julialang.org/">Julia Programming Language</a>.</p></nav></div><div class="modal" id="documenter-settings"><div class="modal-background"></div><div class="modal-card"><header class="modal-card-head"><p class="modal-card-title">Settings</p><button class="delete"></button></header><section class="modal-card-body"><p><label class="label">Theme</label><div class="select"><select id="documenter-themepicker"><option value="auto">Automatic (OS)</option><option value="documenter-light">documenter-light</option><option value="documenter-dark">documenter-dark</option><option value="catppuccin-latte">catppuccin-latte</option><option value="catppuccin-frappe">catppuccin-frappe</option><option value="catppuccin-macchiato">catppuccin-macchiato</option><option value="catppuccin-mocha">catppuccin-mocha</option></select></div></p><hr/><p>This document was generated with <a href="https://github.com/JuliaDocs/Documenter.jl">Documenter.jl</a> version 1.7.0 on <span class="colophon-date" title="Friday 20 September 2024 19:53">Friday 20 September 2024</span>. Using Julia version 1.10.5.</p></section><footer class="modal-card-foot"></footer></div></div></div></body></html>
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