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Update Sphinx documentation, commit c65f760 [skip ci].
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2 changes: 1 addition & 1 deletion _sources/changelog.rst
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Changelog
=========

2.0.0 (unreleased)
2.0.0 (2023-09-22)
------------------

New
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488 changes: 244 additions & 244 deletions changelog.html

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46 changes: 23 additions & 23 deletions index.html
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Expand Up @@ -501,29 +501,29 @@ <h1>heyoka.py<a class="headerlink" href="#heyoka-py" title="Permalink to this he
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<li class="toctree-l1"><a class="reference internal" href="breaking_changes.html">Breaking changes</a><ul>
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2 changes: 1 addition & 1 deletion notebooks/Batch mode overview.html
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8 changes: 4 additions & 4 deletions notebooks/Customising the adaptive integrator.html
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<div class="output stderr highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>/tmp/ipykernel_13118/2332358995.py:11: DeprecationWarning: Conversion of an array with ndim &gt; 0 to a scalar is deprecated, and will error in future. Ensure you extract a single element from your array before performing this operation. (Deprecated NumPy 1.25.)
<div class="output stderr highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>/tmp/ipykernel_13138/2332358995.py:11: DeprecationWarning: Conversion of an array with ndim &gt; 0 to a scalar is deprecated, and will error in future. Ensure you extract a single element from your array before performing this operation. (Deprecated NumPy 1.25.)
ta.pars[6] = np.heaviside(switching_function(x_0,y_0,lx_0,ly_0, ps), 1.)
/tmp/ipykernel_13118/2332358995.py:14: DeprecationWarning: Conversion of an array with ndim &gt; 0 to a scalar is deprecated, and will error in future. Ensure you extract a single element from your array before performing this operation. (Deprecated NumPy 1.25.)
/tmp/ipykernel_13138/2332358995.py:14: DeprecationWarning: Conversion of an array with ndim &gt; 0 to a scalar is deprecated, and will error in future. Ensure you extract a single element from your array before performing this operation. (Deprecated NumPy 1.25.)
ta.state[0] = x_0; ta.state[1] = y_0; ta.state[2] = lx_0; ta.state[3] = ly_0
</pre></div>
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<div class="output stderr highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>/tmp/ipykernel_13118/685660463.py:12: DeprecationWarning: Conversion of an array with ndim &gt; 0 to a scalar is deprecated, and will error in future. Ensure you extract a single element from your array before performing this operation. (Deprecated NumPy 1.25.)
<div class="output stderr highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>/tmp/ipykernel_13138/685660463.py:12: DeprecationWarning: Conversion of an array with ndim &gt; 0 to a scalar is deprecated, and will error in future. Ensure you extract a single element from your array before performing this operation. (Deprecated NumPy 1.25.)
ta.pars[6] = np.heaviside(switching_function(x_0,y_0,lx_0,ly_0, ps), 1.)
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<div class="output stream highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>--- 10.38841199874878 seconds --- to build the Taylor integrator
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<div class="output stream highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>--- 0.052178144454956055 seconds --- to propagate
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<div class="output text_plain highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>&lt;matplotlib.collections.PathCollection at 0x7f62a96b69b0&gt;
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Taylor order : 20
Dimension : 2
Time : 20
State : [0.05099169342796565, 0.07278139612705842],
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None)
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Expand All @@ -470,8 +470,8 @@ <h1>JIT compilation and caching<a class="headerlink" href="#jit-compilation-and-
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Wall time: 15.6 ms
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<div class="output text_plain highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>(&lt;taylor_outcome.time_limit: -4294967299&gt;,
Expand All @@ -498,8 +498,8 @@ <h1>JIT compilation and caching<a class="headerlink" href="#jit-compilation-and-
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Wall time: 994 µs
</pre></div>
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<div class="output text_plain highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>(&lt;taylor_outcome.time_limit: -4294967299&gt;,
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Expand Up @@ -609,7 +609,7 @@ <h2>Running the experiments<a class="headerlink" href="#running-the-experiments"
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<p>This Poincare’ section is suggesting that the integral of motion <span class="math notranslate nohighlight">\(\mathcal{C}\)</span> does indeed exist, because the intersections of all random orbits are clearly tracing curves on the <span class="math notranslate nohighlight">\(x=0\)</span> plane.</p>
Expand All @@ -624,7 +624,7 @@ <h2>Running the experiments<a class="headerlink" href="#running-the-experiments"
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<p>The qualitative picture is now radically different. Although islands of stable motion persist, now most trajectories seem to be densely filling the plane, rather than tracing curves on it. Let us further increase the energy level:</p>
Expand All @@ -635,7 +635,7 @@ <h2>Running the experiments<a class="headerlink" href="#running-the-experiments"
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<p>At higher energies, the densely-filling behaviour (which Henon and Heiles call <em>ergodic</em>) is even more prevalent than before.</p>
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Expand Up @@ -598,8 +598,8 @@ <h1>Interoperability with SymPy<a class="headerlink" href="#interoperability-wit
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<div class="output text_plain highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>(&lt;taylor_outcome.time_limit: -4294967299&gt;,
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<div class="output text_plain highlight-myst-ansi notranslate"><div class="highlight"><pre><span></span>(&lt;taylor_outcome.time_limit: -4294967299&gt;,
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2 changes: 1 addition & 1 deletion searchindex.js

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