LagrangeEuler
- 711
- 22
Why you can do separation of variables in time-dependent
with
\psi(\vec{r},t)=\varphi(\vec{r})T(t)
and when in general is that possible?
Schrödinger equation
i \hbar \frac{\partial \psi(\vec{r},t)}{\partial t}=-\frac{\hbar^2}{2m}\Delta \psi(\vec{r},t)+V(\vec{r})\psi(\vec{r},t)with
\psi(\vec{r},t)=\varphi(\vec{r})T(t)
and when in general is that possible?