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Heisenberg picture

In physics, the Heisenberg picture or Heisenberg representation[1] 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 and the states evolve in time.

It further serves to define a third, hybrid, picture, the interaction picture.

  1. ^ "Heisenberg representation". Encyclopedia of Mathematics. Retrieved 3 September 2013.

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