Heisenberg evolution and conserved observables
The Heisenberg observable A_H=U†A_SU obeys dA_H/dt=(i/ħ)[H_H,A_H]+(∂A_S/∂t)_H.
Key knowledge
The Heisenberg observable A_H=U†A_SU obeys dA_H/dt=(i/ħ)[H_H,A_H]+(∂A_S/∂t)_H. A time-independent observable commuting with H is conserved by this evolution.
Values and equations
dA_H/dt=(i/ħ)[H_H,A_H]+(∂A_S/∂t)_H
- A_H,A_S
- Heisenberg/Schrödinger observable; own physical unit
- H_H
- Hamiltonian J
- ħ
- Reduced Planck constant J s
- t
- Time s
- i
- Imaginary unit
Conditions and scope
- Closed-system unitary dynamics and products/derivatives on a suitable common operator domain.
- Explicit operator time dependence must be retained; commutation alone is insufficient when A explicitly changes.
Sources · 1
References
Sources retain their recorded scope. A source link alone does not establish verification of every statement.
Evidence and review
Quantum Mechanics (2016): Heisenberg equation of motion: Equations 3.19–3.25 and final conserved-observable paragraph; explicit time derivative restored for an explicitly time-dependent observable.
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Entry details
Permanent link to this entry ↗- Record identity
- physics-heisenberg-dynamics
- Revision
- university-core.1
- Structured reference record
- University core expansion