<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Neural ODE on Chen Kai Blog</title><link>https://www.chenk.top/en/tags/neural-ode/</link><description>Recent content in Neural ODE on Chen Kai Blog</description><generator>Hugo</generator><language>en</language><lastBuildDate>Mon, 15 Jul 2024 09:00:00 +0000</lastBuildDate><atom:link href="https://www.chenk.top/en/tags/neural-ode/index.xml" rel="self" type="application/rss+xml"/><item><title>PDE and ML (6): Continuous Normalizing Flows and Neural ODE</title><link>https://www.chenk.top/en/pde-ml/06-continuous-normalizing-flows/</link><pubDate>Mon, 15 Jul 2024 09:00:00 +0000</pubDate><guid>https://www.chenk.top/en/pde-ml/06-continuous-normalizing-flows/</guid><description>&lt;p>&lt;figure class="article-figure">
 &lt;img src="https://blog-pic-ck.oss-cn-beijing.aliyuncs.com/posts/en/pde-ml/06-Continuous-Normalizing-Flows/illustration_1.png" alt="PDE and ML (6): Continuous Normalizing Flows and Neural ODE — Chapter overview" loading="lazy" decoding="async" class="content-image">
 
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&lt;p>How do you turn an isotropic Gaussian into a photograph of a cat?&lt;/p>
&lt;p>Normalizing flows give the most direct answer: stack a sequence of invertible transformations and let them push the simple distribution into the complex one. This article&amp;rsquo;s continuous version (CNF) takes that idea to the limit — let the step size go to zero and the discrete chain becomes an ODE. Invertibility is automatic, and the change of density is governed by the instantaneous change of variables formula.&lt;/p></description></item><item><title>PDE and ML (5): Symplectic Geometry and Structure-Preserving Networks</title><link>https://www.chenk.top/en/pde-ml/05-symplectic-geometry/</link><pubDate>Sun, 30 Jun 2024 09:00:00 +0000</pubDate><guid>https://www.chenk.top/en/pde-ml/05-symplectic-geometry/</guid><description>&lt;p>&lt;figure class="article-figure">
 &lt;img src="https://blog-pic-ck.oss-cn-beijing.aliyuncs.com/posts/en/pde-ml/05-Symplectic-Geometry/illustration_1.png" alt="PDE and ML (5): Symplectic Geometry and Structure-Preserving Networks — Chapter overview" loading="lazy" decoding="async" class="content-image">
 
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&lt;p>A pendulum keeps swinging for a very long time without slowly winding down — energy is conserved. The Earth orbits the Sun for billions of years without flying off — angular momentum is conserved. Behind every &amp;ldquo;this quantity stays constant&amp;rdquo; lurks a piece of geometry called &lt;strong>symplectic structure&lt;/strong>.&lt;/p>
&lt;p>Train a vanilla Neural ODE on pendulum data: after a few hundred steps the energy drifts. The network can fit the short-term trajectory just fine; what it can&amp;rsquo;t fit is the long-time conservation law. &lt;strong>Structure-preserving networks&lt;/strong> (HNN, LNN, SympNet) take a different approach: bake the conservation law into the architecture so the network &lt;em>cannot&lt;/em> violate it.&lt;/p></description></item></channel></rss>