Klein–Gordon hong-têng-sek
Klein–Gordon
描述[修改]
Klein–Gordon方程式是
- 解析失敗 (Chīn-liōng iōng MathML (chhì-giām-sèng--ê)：從伺服器 "https://wikimedia.org/api/rest_v1/" 收到無效的回應 ("Math extension cannot connect to Restbase.")。): {\displaystyle \frac {1}{c^2} \frac{\partial^2}{\partial t^2} \psi - \nabla^2 \psi + \frac {m^2 c^2}{\hbar^2} \psi = 0} 。
- 解析失敗 (Chīn-liōng iōng MathML (chhì-giām-sèng--ê)：從伺服器 "https://wikimedia.org/api/rest_v1/" 收到無效的回應 ("Math extension cannot connect to Restbase.")。): {\displaystyle - \partial_t^2 \psi + \nabla^2 \psi = m^2 \psi}
共變 形式[修改]
- 解析失敗 (Chīn-liōng iōng MathML (chhì-giām-sèng--ê)：從伺服器 "https://wikimedia.org/api/rest_v1/" 收到無效的回應 ("Math extension cannot connect to Restbase.")。): {\displaystyle \frac{\mathbf{p}^2}{2m} \psi = i \hbar \frac{\partial}{\partial t}\psi }
Schrödinger方程式
- 解析失敗 (Chīn-liōng iōng MathML (chhì-giām-sèng--ê)：從伺服器 "https://wikimedia.org/api/rest_v1/" 收到無效的回應 ("Math extension cannot connect to Restbase.")。): {\displaystyle E = \sqrt{\mathbf{p}^2 c^2 + m^2 c^4}}
共Schrödinger方程式
- 解析失敗 (語法錯誤): {\displaystyle (\Box^2 + \mu^2) \psi = 0， }
其中 解析失敗 (Chīn-liōng iōng MathML (chhì-giām-sèng--ê)：從伺服器 "https://wikimedia.org/api/rest_v1/" 收到無效的回應 ("Math extension cannot connect to Restbase.")。): {\displaystyle \mu = \frac{mc}{\hbar} \,}
D'Alembertian是 解析失敗 (Chīn-liōng iōng MathML (chhì-giām-sèng--ê)：從伺服器 "https://wikimedia.org/api/rest_v1/" 收到無效的回應 ("Math extension cannot connect to Restbase.")。): {\displaystyle \Box^2 = \frac{1}{c^2}\frac{\partial^2}{\partial t^2} - \nabla^2\,}
