Functional analysis von Neumann algebras Concept
Commutant
Summary
Let be a set of operators on a Hilbert space. Its commutant is the set of all bounded operators that commute with every element of . It is the operator version of the centralizer in an algebra. The commutant of a self-adjoint set is always a von Neumann algebra. By the bicommutant theorem, the von Neumann algebras are the self-adjoint unital algebras equal to their double commutant.
Where this leads
4 pages build on this one.
Further reading
About this page
| Tag | 1VC7EJ1ZBZ |
|---|---|
| URI | m2://1VC7EJ1ZBZ |
| Kind | concept |
| Writing | W0 stub |
| MSC | 46L10, 47L05 |
| Changed | 2 November 2026 |
Markdown · JSON · Edit on GitHub
What this page needs for W1
- an inventory row: the row of the inventory that the node accounts for (0 of 1)
- a source with a locator (0 of 1)
The writing levels say how complete the text of a page is. They do not measure its truth.
What links here
Results about this
Used by
- Von Neumann bicommutant theorem
- Murray–von Neumann classification of factors
- Tomita–Takesaki theory
- Subfactor