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Heisenberg picture
Formulation of quantum mechanics
Heisenberg picture
In physics, the Heisenberg picture or Heisenberg representation is a formulation (largely due to Werner Heisenberg in 1925) of quantum mechanics in which observables incorporate a dependency on time, but the states are time-independent. It stands in contrast to the Schrödinger picture in which observables are constant (as long as there is no external force) and the states evolve in time. It further serves to define a third, hybrid picture, the interaction picture.
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