build based on 8d63119

Author: Documenter.jl

dev/.documenter-siteinfo.json

@@ -1 +1 @@
-{"documenter":{"julia_version":"1.12.3","generation_timestamp":"2025-12-18T01:28:38","documenter_version":"1.16.1"}}
+{"documenter":{"julia_version":"1.12.3","generation_timestamp":"2025-12-23T10:29:47","documenter_version":"1.16.1"}}

dev/Changelog/index.html

@@ -6,4 +6,4 @@
         Springer Science &amp; Business Media.</code></pre></li><li class="footnote" id="footnote-kitaev"><a class="tag is-link" href="#citeref-kitaev">kitaev</a><pre><code class="nohighlight hljs">  Kitaev, A. (2006). Anyons in an exactly solved model and beyond.
         Annals of Physics, 321(1), 2-111.</code></pre></li><li class="footnote" id="footnote-beer"><a class="tag is-link" href="#citeref-beer">beer</a><pre><code class="nohighlight hljs">    From categories to anyons: a travelogue
         Kerstin Beer, Dmytro Bondarenko, Alexander Hahn, Maria Kalabakov, Nicole Knust, Laura Niermann, Tobias J. Osborne, Christin Schridde, Stefan Seckmeyer, Deniz E. Stiegemann, and Ramona Wolf
-        [https://arxiv.org/abs/1811.06670](https://arxiv.org/abs/1811.06670)</code></pre></li></ul></section></article><nav class="docs-footer"><a class="docs-footer-prevpage" href="../symmetric_tutorial/">« A symmetric tensor deep dive: constructing your first tensor map</a><a class="docs-footer-nextpage" href="../../Changelog/">Changelog »</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 1.16.1 on <span class="colophon-date" title="Thursday 18 December 2025 01:28">Thursday 18 December 2025</span>. Using Julia version 1.12.3.</p></section><footer class="modal-card-foot"></footer></div></div></div></body></html>
+        [https://arxiv.org/abs/1811.06670](https://arxiv.org/abs/1811.06670)</code></pre></li></ul></section></article><nav class="docs-footer"><a class="docs-footer-prevpage" href="../symmetric_tutorial/">« A symmetric tensor deep dive: constructing your first tensor map</a><a class="docs-footer-nextpage" href="../../Changelog/">Changelog »</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 1.16.1 on <span class="colophon-date" title="Tuesday 23 December 2025 10:29">Tuesday 23 December 2025</span>. Using Julia version 1.12.3.</p></section><footer class="modal-card-foot"></footer></div></div></div></body></html>

dev/appendix/categories/index.html

@@ -669,4 +669,4 @@
 
  * (FusionTree{FibonacciAnyon}((:τ, :τ), :τ, (false, false), ()), FusionTree{FibonacciAnyon}((:τ, :τ), :τ, (false, false), ())) => 1×1×1×1 StridedViews.StridedView{Float64, 4, Memory{Float64}, typeof(identity)}:
 [:, :, 1, 1] =
- 0.0</code></pre><div class="admonition is-info" id="Note-527fead9933cbe71"><header class="admonition-header">Note<a class="admonition-anchor" href="#Note-527fead9933cbe71" title="Permalink"></a></header><div class="admonition-body"><p>In the previous section we have stressed the role of Clebsch-Gordan coefficients in the structure of symmetric tensors, and how they can be used to map between the representation of an operator in the irrep basis and its symmetric tensor representation. However, for categorical symmetries such as the Fibonacci anyons, there are no Clebsch-Gordan coefficients. Therefore, the &#39;matrix elements of the operator in the irrep basis&#39; are not well-defined, meaning that a Fibonacci-symmetric tensor cannot actually be converted to a plain array in a straightforward way.</p></div></div></article><nav class="docs-footer"><a class="docs-footer-prevpage" href="../../index/">« Index</a><a class="docs-footer-nextpage" href="../categories/">Optional introduction to category theory »</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 1.16.1 on <span class="colophon-date" title="Thursday 18 December 2025 01:28">Thursday 18 December 2025</span>. Using Julia version 1.12.3.</p></section><footer class="modal-card-foot"></footer></div></div></div></body></html>
+ 0.0</code></pre><div class="admonition is-info" id="Note-527fead9933cbe71"><header class="admonition-header">Note<a class="admonition-anchor" href="#Note-527fead9933cbe71" title="Permalink"></a></header><div class="admonition-body"><p>In the previous section we have stressed the role of Clebsch-Gordan coefficients in the structure of symmetric tensors, and how they can be used to map between the representation of an operator in the irrep basis and its symmetric tensor representation. However, for categorical symmetries such as the Fibonacci anyons, there are no Clebsch-Gordan coefficients. Therefore, the &#39;matrix elements of the operator in the irrep basis&#39; are not well-defined, meaning that a Fibonacci-symmetric tensor cannot actually be converted to a plain array in a straightforward way.</p></div></div></article><nav class="docs-footer"><a class="docs-footer-prevpage" href="../../index/">« Index</a><a class="docs-footer-nextpage" href="../categories/">Optional introduction to category theory »</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 1.16.1 on <span class="colophon-date" title="Tuesday 23 December 2025 10:29">Tuesday 23 December 2025</span>. Using Julia version 1.12.3.</p></section><footer class="modal-card-foot"></footer></div></div></div></body></html>