<?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 in Physics on Haifei's Home</title><link>https://haifei-home.pages.dev/en/tags/mathematical-methods-in-physics/</link><description>Recent content in Mathematical Methods in 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, 01 May 2024 03:04:30 +0800</lastBuildDate><atom:link href="https://haifei-home.pages.dev/en/tags/mathematical-methods-in-physics/index.xml" rel="self" type="application/rss+xml"/><item><title>How are creation and annihilation operators derived?</title><link>https://haifei-home.pages.dev/en/post_20240501_%E4%BA%A7%E7%94%9F%E6%B9%AE%E7%81%AD%E7%AE%97%E7%AC%A6%E6%98%AF%E6%80%8E%E4%B9%88%E5%BE%97%E5%88%B0%E7%9A%84/</link><pubDate>Wed, 01 May 2024 03:04:30 +0800</pubDate><author>hfwang132@gmail.com (hfwang132)</author><guid>https://haifei-home.pages.dev/en/post_20240501_%E4%BA%A7%E7%94%9F%E6%B9%AE%E7%81%AD%E7%AE%97%E7%AC%A6%E6%98%AF%E6%80%8E%E4%B9%88%E5%BE%97%E5%88%B0%E7%9A%84/</guid><description>&lt;p&gt;The motivation for defining creation and annihilation operators is simple and can be entirely derived from classical mechanics.&lt;/p&gt;
&lt;p&gt;Think about how we solve the classical harmonic oscillator. Since position and momentum are coupled:&lt;/p&gt;
&lt;p&gt;$\begin{cases} \frac{\mathrm{d}x}{\mathrm{d}t} = \omega p \\ \frac{\mathrm{d}p}{\mathrm{d}t} = -\omega x \end{cases}$&lt;/p&gt;
&lt;p&gt;That is,&lt;/p&gt;
&lt;p&gt;$\frac{\mathrm{d}}{\mathrm{d}t} \begin{bmatrix} x \\ p \end{bmatrix} = \begin{bmatrix} 0 &amp;amp; \omega \\ -\omega &amp;amp; 0 \end{bmatrix} \begin{bmatrix} x \\ p \end{bmatrix}$&lt;/p&gt;
&lt;p&gt;So, we just need to decouple them. By diagonalizing, we obtain the eigenvectors $a^{\pm} = x \pm \mathrm{i} p$, and the derivatives of $a^{\pm}$ only depend on themselves:&lt;/p&gt;</description></item></channel></rss>