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Von Neumann bicommutant theorem : ウィキペディア英語版
Von Neumann bicommutant theorem
In mathematics, specifically closure of a set of bounded operators on a Hilbert space in certain operator topologyn Neumann algebra]] generated by .
There are several other topologies on the space of bounded operators, and one can ask what are the
*-algebras closed in these topologies. If is closed in the norm topology then it is a C
*-algebra
, but not necessarily a von Neumann algebra. One such example is the C
*-algebra of compact operators (on an infinite dimensional Hilbert space). For most other common topologies the closed
*-algebras containing 1 are still von Neumann algebras; this applies in particular to the weak operator, strong operator,
*-strong operator, ultraweak, ultrastrong, and
*-ultrastrong topologies.

It is related to the Jacobson density theorem.
== Proof ==
Let be a Hilbert space and the bounded operators on . Consider a self-adjoint unital subalgebra of . (this means that contains the adjoints of its members, and the identity operator on )
The theorem is equivalent to the combination of the following three statements:
:(i)
:(ii)
:(iii)
where the and subscripts stand for closures in the weak and strong operator topologies, respectively.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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