定态薛定谔方程

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定义 · 1.2 正则量子化

而第二个方程是哈密顿算符的本征值问题，称为定态薛定谔方程(time-independent Schrödinger equation)、定态波薛定谔方程，或简称为薛定谔方程。对于三维空间，它写作

$$-\frac{1}{2m}{\nabla }^2\varphi (\mathbf{x})+V(\mathbf{x})\varphi (\mathbf{x})=E\varphi (\mathbf{x}).\text{\hspace{1em}(1.62)}$$

英文原文

while the second one is the eigenvalue problem of the Hamiltonian operator and called the time-independent Schrödinger equation, the stationary state Schrödinger equation or, simply, the Schrödinger equation. For three-dimensional space, it is written as

$$-\frac{1}{2m}{\nabla }^2\varphi (\mathbf{x})+V(\mathbf{x})\varphi (\mathbf{x})=E\varphi (\mathbf{x}).\text{\hspace{1em}(1.62)}$$

出处：1.2 正则量子化 · node a-3529d5c85ed38588ffccbf43 · 源节点 SHA-256 f21fa8c475dc40f9…