build based on ad8bdd2

Author: Documenter.jl

previews/PR106/.documenter-siteinfo.json

@@ -1 +1 @@
-{"documenter":{"documenter_version":"1.17.0","generation_timestamp":"2026-04-15T13:27:51","julia_version":"1.12.6"}}
+{"documenter":{"documenter_version":"1.17.0","generation_timestamp":"2026-04-17T09:49:51","julia_version":"1.12.6"}}

previews/PR106/api/index.html

@@ -60,4 +60,4 @@
 <span class="sgr32"><span class="sgr1">             </span></span>└ <span class="sgr90">--manifest-path /home/runner/work/SymmetricTightBinding.jl/SymmetricTightBinding.jl/docs/.CondaPkg/pixi.toml</span>
 ✔ The default environment has been installed.</code><br/><code class="language-julia-repl hljs" style="display:block;">julia&gt; calc_detailed_topology.(ns, Ref(brs))</code><code class="nohighlight hljs ansi" style="display:block;">2-element Vector{Crystalline.TopologyKind}:
  TRIVIAL::TopologyKind = 0
- FRAGILE::TopologyKind = 2</code></pre></article><nav class="docs-footer"><a class="docs-footer-prevpage" href="../tutorial/">« Tutorial</a><a class="docs-footer-nextpage" href="../berry/">Berry curvature &amp; Chern numbers »</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 1.17.0 on <span class="colophon-date" title="Wednesday 15 April 2026 13:27">Wednesday 15 April 2026</span>. Using Julia version 1.12.6.</p></section><footer class="modal-card-foot"></footer></div></div></div></body></html>
+ FRAGILE::TopologyKind = 2</code></pre></article><nav class="docs-footer"><a class="docs-footer-prevpage" href="../tutorial/">« Tutorial</a><a class="docs-footer-nextpage" href="../berry/">Berry curvature &amp; Chern numbers »</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 1.17.0 on <span class="colophon-date" title="Friday 17 April 2026 09:49">Friday 17 April 2026</span>. Using Julia version 1.12.6.</p></section><footer class="modal-card-foot"></footer></div></div></div></body></html>

previews/PR106/band-symmetry/index.html

@@ -142,4 +142,4 @@
 Φ = sum(berrycurvature(ptbm, [k1, k2, k3], 1)[3] for k1 in k12s, k2 in k12s; init=0.0) / Nk^2
 
 # normalize by 2π to obtain associated Chern number
-C₃ = Φ / (2π)</code></pre></div></div><section class="footnotes is-size-7"><ul><li class="footnote" id="footnote-1"><a class="tag is-link" href="#citeref-1">1</a>F.D.M. Haldane, <em>Model for a Quantum Hall Effect without Landau Levels: Condensed-Matter Realization of the &quot;Parity Anomaly&quot;</em>, <a href="https://doi.org/10.1103/PhysRevLett.61.2015">Phys. Rev. Lett. <strong>61</strong>, 2015 (1988)</a>.</li><li class="footnote" id="footnote-2"><a class="tag is-link" href="#citeref-2">2</a>While it is natural to think of the Haldane model as associated with 6-fold symmetry and a graphene-like model, and hence with plane groups <em>p</em>6 or <em>p</em>6mm, the presence of the staggered mass term reduces the model&#39;s symmetry to <em>p</em>3. Thus, the orbitals do not associate with the 2b Wyckoff position of <em>p</em>6(mm), as is usually the case for graphene-like models, but with the two distinct Wyckoff positions that the <em>p</em>6(mm) 2b Wyckoff position subduces to when inversion symmetry is broken: this is precisely the 2b and 2c positions in <em>p</em>3.</li><li class="footnote" id="footnote-3"><a class="tag is-link" href="#citeref-3">3</a>Fukui, Hatsugai, &amp; Suzuki, <em>Chern Numbers in Discretized Brillouin Zone: Efficient Method of Computing (Spin) Hall Conductances</em>, <a href="https://doi.org/10.1143/JPSJ.74.1674">J. Phys. Soc. Jpn. <strong>74</strong>, 1674 (2005)</a>.</li></ul></section></article><nav class="docs-footer"><a class="docs-footer-prevpage" href="../band-symmetry/">« Band symmetry</a><a class="docs-footer-nextpage" href="../symmetry-breaking/">Symmetry breaking »</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 1.17.0 on <span class="colophon-date" title="Wednesday 15 April 2026 13:27">Wednesday 15 April 2026</span>. Using Julia version 1.12.6.</p></section><footer class="modal-card-foot"></footer></div></div></div></body></html>
+C₃ = Φ / (2π)</code></pre></div></div><section class="footnotes is-size-7"><ul><li class="footnote" id="footnote-1"><a class="tag is-link" href="#citeref-1">1</a>F.D.M. Haldane, <em>Model for a Quantum Hall Effect without Landau Levels: Condensed-Matter Realization of the &quot;Parity Anomaly&quot;</em>, <a href="https://doi.org/10.1103/PhysRevLett.61.2015">Phys. Rev. Lett. <strong>61</strong>, 2015 (1988)</a>.</li><li class="footnote" id="footnote-2"><a class="tag is-link" href="#citeref-2">2</a>While it is natural to think of the Haldane model as associated with 6-fold symmetry and a graphene-like model, and hence with plane groups <em>p</em>6 or <em>p</em>6mm, the presence of the staggered mass term reduces the model&#39;s symmetry to <em>p</em>3. Thus, the orbitals do not associate with the 2b Wyckoff position of <em>p</em>6(mm), as is usually the case for graphene-like models, but with the two distinct Wyckoff positions that the <em>p</em>6(mm) 2b Wyckoff position subduces to when inversion symmetry is broken: this is precisely the 2b and 2c positions in <em>p</em>3.</li><li class="footnote" id="footnote-3"><a class="tag is-link" href="#citeref-3">3</a>Fukui, Hatsugai, &amp; Suzuki, <em>Chern Numbers in Discretized Brillouin Zone: Efficient Method of Computing (Spin) Hall Conductances</em>, <a href="https://doi.org/10.1143/JPSJ.74.1674">J. Phys. Soc. Jpn. <strong>74</strong>, 1674 (2005)</a>.</li></ul></section></article><nav class="docs-footer"><a class="docs-footer-prevpage" href="../band-symmetry/">« Band symmetry</a><a class="docs-footer-nextpage" href="../symmetry-breaking/">Symmetry breaking »</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 1.17.0 on <span class="colophon-date" title="Friday 17 April 2026 09:49">Friday 17 April 2026</span>. Using Julia version 1.12.6.</p></section><footer class="modal-card-foot"></footer></div></div></div></body></html>