<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Topology on Haifei's Home</title><link>https://haifei-home.pages.dev/en/tags/topology/</link><description>Recent content in Topology on Haifei's Home</description><generator>Hugo</generator><language>en</language><managingEditor>hfwang132@gmail.com (hfwang132)</managingEditor><webMaster>hfwang132@gmail.com (hfwang132)</webMaster><copyright>This work is licensed under a Creative Commons Attribution-NonCommercial 4.0 International License.</copyright><lastBuildDate>Sun, 30 Mar 2025 01:13:18 +0800</lastBuildDate><atom:link href="https://haifei-home.pages.dev/en/tags/topology/index.xml" rel="self" type="application/rss+xml"/><item><title>Dirac Magnetic Monopoles—Chern Classes and Chern Numbers [Higher and More Wonderful Electrodynamics · 4]</title><link>https://haifei-home.pages.dev/en/post_20250330_%E7%8B%84%E6%8B%89%E5%85%8B%E7%A3%81%E5%8D%95%E6%9E%81%E5%AD%90-%E9%99%88%E7%B1%BB%E4%B8%8E%E9%99%88%E6%95%B0-%E6%9B%B4%E9%AB%98%E6%9B%B4%E5%A6%99%E7%9A%84%E7%94%B5%E5%8A%A8%E5%8A%9B%E5%AD%A6-4/</link><pubDate>Sun, 30 Mar 2025 01:13:18 +0800</pubDate><author>hfwang132@gmail.com (hfwang132)</author><guid>https://haifei-home.pages.dev/en/post_20250330_%E7%8B%84%E6%8B%89%E5%85%8B%E7%A3%81%E5%8D%95%E6%9E%81%E5%AD%90-%E9%99%88%E7%B1%BB%E4%B8%8E%E9%99%88%E6%95%B0-%E6%9B%B4%E9%AB%98%E6%9B%B4%E5%A6%99%E7%9A%84%E7%94%B5%E5%8A%A8%E5%8A%9B%E5%AD%A6-4/</guid><description>&lt;p&gt;Previous article in this series:&lt;/p&gt;
&lt;p&gt;&lt;a href="https://zhuanlan.zhihu.com/p/32173040413" target="_blank" rel="noopener noreffer "&gt;Godfly: The electromagnetic field is more than just electric and magnetic fields—The AB effect and Berry connection [Higher and More Wonderful Electrodynamics · 3]&lt;/a&gt;&lt;/p&gt;
&lt;hr&gt;
&lt;p&gt;In the &lt;a href="https://zhuanlan.zhihu.com/p/32173040413" target="_blank" rel="noopener noreffer "&gt;previous article&lt;/a&gt;, we mentioned that if a manifold is topologically trivial, then integrating the Berry curvature over a closed surface \(\Sigma\) should yield zero. This is because, according to Stokes&amp;rsquo; theorem:&lt;/p&gt;
\[\int_\Sigma F = \int_{\partial \Sigma } A = 0\]&lt;p&gt;However, on a topologically nontrivial manifold, the integral \(\int_\Sigma F\) need not be zero. This is because a globally single-valued connection \(A\) cannot be defined in this case, so Stokes&amp;rsquo; theorem no longer applies. What does this mean?&lt;/p&gt;</description></item></channel></rss>