<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Mathematical Methods of Physics on Haifei's Home</title><link>https://haifei.pro/en/categories/mathematical-methods-of-physics/</link><description>Recent content in Mathematical Methods of Physics 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>Wed, 09 Jul 2025 19:23:54 +0800</lastBuildDate><atom:link href="https://haifei.pro/en/categories/mathematical-methods-of-physics/index.xml" rel="self" type="application/rss+xml"/><item><title>Why Spin Is Not a Relativistic Effect</title><link>https://haifei.pro/en/post_20250709_%E8%87%AA%E6%97%8B%E4%B8%BA%E4%BB%80%E4%B9%88%E4%B8%8D%E6%98%AF%E7%9B%B8%E5%AF%B9%E8%AE%BA%E6%95%88%E5%BA%94/</link><pubDate>Wed, 09 Jul 2025 19:23:54 +0800</pubDate><author>hfwang132@gmail.com (hfwang132)</author><guid>https://haifei.pro/en/post_20250709_%E8%87%AA%E6%97%8B%E4%B8%BA%E4%BB%80%E4%B9%88%E4%B8%8D%E6%98%AF%E7%9B%B8%E5%AF%B9%E8%AE%BA%E6%95%88%E5%BA%94/</guid><description>&lt;p&gt;Conclusion: integer spin is a classical effect, whereas half-integer spin is a quantum effect and has little to do with relativity.&lt;/p&gt;
&lt;p&gt;The reason is simple: spin-1 is the smallest faithful representation of SO(3), while spin-1/2 is the smallest faithful representation of SU(2).&lt;/p&gt;
&lt;p&gt;So why can quantum mechanics lift SO(3) to SU(2)? Because quantum states are rays and are equivalent up to a global phase. In other words, quantum mechanics requires projective representations of SO(3). And projective representations of SO(3) are in one-to-one correspondence with representations of SU(2) (Bargmann&amp;rsquo;s theorem). This is why quantum mechanics considers SU(2) rather than SO(3).&lt;/p&gt;</description></item><item><title>What Is Curl in Higher-Dimensional Spaces?</title><link>https://haifei.pro/en/post_20230526_%E9%AB%98%E7%BB%B4%E7%A9%BA%E9%97%B4%E4%B8%AD%E7%9A%84%E6%97%8B%E5%BA%A6/</link><pubDate>Fri, 26 May 2023 21:00:37 +0800</pubDate><author>hfwang132@gmail.com (hfwang132)</author><guid>https://haifei.pro/en/post_20230526_%E9%AB%98%E7%BB%B4%E7%A9%BA%E9%97%B4%E4%B8%AD%E7%9A%84%E6%97%8B%E5%BA%A6/</guid><description>&lt;h3 id="differential-forms"&gt;Differential Forms&lt;/h3&gt;
&lt;p&gt;Before introducing curl, we must first introduce differential forms and the exterior derivative operator.&lt;/p&gt;
&lt;p&gt;An n-form can be defined as an alternating multilinear map \(\omega:(T_pM)^n\rightarrow \mathbb{R}\) . It maps multiple vectors to a real number. Moreover, it satisfies alternation: exchanging two input vectors introduces an additional minus sign in the output.&lt;/p&gt;
&lt;p&gt;Thus, an n-form can be explicitly defined as follows:&lt;br&gt;
&lt;/p&gt;
\[\omega^1\wedge \omega^2\wedge\cdots\wedge \omega^n(v_1,v_2,\cdots,v_n)= \begin{vmatrix} \omega^1(v_1) &amp; \cdots &amp; \omega^{1}(v_n) \\ \vdots &amp; \ddots &amp; \vdots \\ \omega^n(v_1) &amp; \cdots &amp; \omega^n(v_n) \end{vmatrix}\in\mathbb{R}\]&lt;p&gt;The set of all n-forms on \(T_pM\) can be written as \(\bigwedge^n(T^*_pM)\) .&lt;/p&gt;</description></item></channel></rss>