Schrödinger-Gleichung

$𝔦 \partial_{t} Ψ = \hat{H} Ψ, \hat{H} = - \frac{Δ}{2 m}$

𝔦 ℏ \frac{\partial}{\partial t} | ψ (t) ⟩ = \hat{H} | ψ (t) ⟩

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