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  <div class="section" id="todo-list">
<h1>Todo list<a class="headerlink" href="#todo-list" title="Permalink to this headline"></a></h1>
<div class="admonition-todo admonition " id="index-6">
<p class="first admonition-title">Todo</p>
<p class="last">生成的分割が Rényi エントロピー の上限を与えることに
ついての説明を加える</p>
</div>
<p class="todo-source">(The <a class="reference internal" href="dynamical-renyi-entropies.html#index-6"><em>original entry</em></a> is located in  dynamical-renyi-entropies.rst, line 204.)</p>
<div class="admonition-todo admonition " id="index-1">
<p class="first admonition-title">Todo</p>
<p class="last">Gibbs 測度が不変測度の中で位相圧力最大を与える解であることを示す.
<a class="reference internal" href="refs.html#beck1993">[Beck1993]</a> には詳しい説明が無い.
<a class="reference internal" href="refs.html#bowen2008">[Bowen2008]</a> に証明がまとまっているのを見つけたが,関数解析
の知識が必要.</p>
</div>
<p class="todo-source">(The <a class="reference internal" href="gibbs-measures-and-srb-measures.html#index-1"><em>original entry</em></a> is located in  gibbs-measures-and-srb-measures.rst, line 64.)</p>
<div class="admonition-todo admonition " id="index-2">
<p class="first admonition-title">Todo</p>
<p class="last">「拡大的 (expanding) 力学系 ならば,マルコフ分割が存在する」
について,補足する.</p>
</div>
<p class="todo-source">(The <a class="reference internal" href="gibbs-measures-and-srb-measures.html#index-2"><em>original entry</em></a> is located in  gibbs-measures-and-srb-measures.rst, line 209.)</p>
<div class="admonition-todo admonition " id="index-0">
<p class="first admonition-title">Todo</p>
<p class="last">Perron-Frobenius 演算子の導出</p>
</div>
<p class="todo-source">(The <a class="reference internal" href="perron-frobenius-operator.html#index-0"><em>original entry</em></a> is located in  perron-frobenius-operator.rst, line 4.)</p>
<div class="admonition-todo admonition " id="index-3">
<p class="first admonition-title">Todo</p>
<p class="last">なぜ (あるいはどのような条件で) Perron-Frobenius 演算子の
最大固有値 <img class="math" src="_images/math/67a66635f0821bb52d4d2301841f796ccf8bb2ad.png" alt="\eta_0"/> は 1 なのか?
固有関数 <img class="math" src="_images/math/254c8ed9835a01428975acb16206391263c66bdf.png" alt="\phi_0 (x)"/> が重解 (縮退している) 場合は無いのか?
あるとしたらどういう場合か?
などについてまとめる.</p>
</div>
<p class="todo-source">(The <a class="reference internal" href="perron-frobenius-operator.html#index-3"><em>original entry</em></a> is located in  perron-frobenius-operator.rst, line 29.)</p>
<div class="admonition-todo admonition " id="index-1">
<p class="first admonition-title">Todo</p>
<p class="last">アンサンブル <img class="math" src="_images/math/45725367611a5e4e87fe0b5a740ff6d6373b5d99.png" alt="\{\xk\}"/> のとり方は色々あって,
双曲型力学系ならそれらのとり方に依存しないなどの
話題にも触れる.</p>
</div>
<p class="todo-source">(The <a class="reference internal" href="topological-pressure.html#index-1"><em>original entry</em></a> is located in  topological-pressure.rst, line 44.)</p>
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