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The Stone–von Neumann theorem (due to Marshall Stone and John von Neumann) says that there is – up to isomorphism – a unique irreducible unitary representation of the Heisenberg group on finitely many generators (equivalently: of the Weyl algebra, Weyl relations, canonical commutation relations).
The analogous statement does not hold for infinitely many generators (as they appear in quantum field theory); this is Haag's theorem.
Explicitly, the canonical commutation relations on two generators (canonical coordinate and canonical momentum ) in the form
may be represented as unbounded operators on the Hilbert space of square integrable functions on the real line by defining them on the dense subspace of smooth functions as
where on the right we have the derivative along the canonical coordinate function on .
This is often called the Schrödinger representation, after Erwin Schrödinger, cf. eg. Redei (to be distinguished from “Schrödinger picture” which is a related but different concept).
For the Schrödinger representation obtained via geometric quantization see there.
The original articles:
John von Neumann, Die Eindeutigkeit der Schrödingerschen Operatoren, Mathematische Annalen 104 (1931) 570–578 [doi:10.1007/BF01457956]
John von Neumann, Über Einen Satz Von Herrn M. H. Stone, Annals of Mathematics, Second Series 33 3 (1932) 567-573 [doi:10.2307/1968535, jstor:1968535]
Review:
Further discussion:
See also
Last revised on December 2, 2023 at 17:58:56. See the history of this page for a list of all contributions to it.