Schrödinger-Gleichung

$\mathfrak{i}{\partial }_t\mathrm{\Psi }=\hat{H}\mathrm{\Psi },\hat{H}=-\frac{\mathrm{\Delta }}{2m}$

$\mathfrak{i}\hslash \frac{\partial }{\partial t}|\psi (t)⟩=\hat{H}|\psi (t)⟩$

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