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The quantum mechanical time evolution operator governs how observables and/or states evolve during finite time steps, and is always unitary. Use this tag for questions about the time evolution operator, or the different equations of motion in the Schrödinger/Heisenberg/Dirac pictures. For time-independent Hamiltonians, the time evolution operator is simply exp(-iHt).

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Notation in the Liouville-von Neumann equation $ i\hbar\frac{dI}{dt} = i\hbar\frac{\partial ... [duplicate]

The Liouville-von Neumannn equation is defined by $$ i\hbar\frac{dI}{dt} = i\hbar\frac{\partial I}{\partial t} + [I, H] $$ where $I$ is any operator and $H$ is the Hamiltonian. I assume that the left- …
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