Liouville-von-Neumann-Gleichung
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ρ
˙
=
−
i
ℏ
[
H
,
ρ
]
mit
ρ
Dichteoperator
H
Hamiltonoperator
[
_
,
_
]
Kommutator
[
1
]
[
2
]
Einzelnachweise
↑
QM 2.5 Teil 1 Seite 77
↑
Schöll, QM 2.5 Teil 1 Seite 77,
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