Liouville-von-Neumann-Gleichung

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$\dot{ρ} = - \frac{i}{ℏ} [H, ρ]$ mit

$ρ$	Dichteoperator
H	Hamiltonoperator
$[_,_]$	Kommutator

Einzelnachweise

↑ QM 2.5 Teil 1 Seite 77

Wikipedia-Eintrag

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