Finite von Neumann algebra

In mathematics, a finite von Neumann algebra is a von Neumann algebra in which every isometry is a unitary. In other words, for an operator V in a finite von Neumann algebra if $V^*V = I$ , then $VV^* = I$ . In terms of the comparison theory of projections, the identity operator is not (Murray-von Neumann) equivalent to any proper subprojection in the von Neumann algebra.

Properties

Let $\mathcal{M}$ denote a finite von Neumann algebra with center $\mathcal{Z}$ . One of the fundamental characterizing properties of finite von Neumann algebras is the existence of a center-valued trace. A von Neumann algebra $\mathcal{M}$ is finite if and only if there exists a normal positive bounded map $\tau : \mathcal{M} \to \mathcal{Z}$ with the properties:

$\tau(AB) = \tau(BA), A, B \in \mathcal{M}$ ,
if $A \ge 0$ and $\tau(A) = 0$ then $A = 0$ ,
$\tau(C) = C$ for $C \in \mathcal{Z}$ ,
$\tau(CA) = C\tau(A)$ for $A \in \mathcal{M}$ and $C \in \mathcal{Z}$ .

Examples

=Finite-dimensional von Neumann algebras=

The finite-dimensional von Neumann algebras can be characterized using Wedderburn's theory of semisimple algebras.

Let C^{n × n} be the n × n matrices with complex entries. A von Neumann algebra M is a self adjoint subalgebra in C^{n × n} such that M contains the identity operator I in C^{n × n}.

Every such M as defined above is a semisimple algebra, i.e. it contains no nilpotent ideals. Suppose M ≠ 0 lies in a nilpotent ideal of M. Since M* ∈ M by assumption, we have M*M, a positive semidefinite matrix, lies in that nilpotent ideal. This implies (M*M)^k = 0 for some k. So M*M = 0, i.e. M = 0.

The center of a von Neumann algebra M will be denoted by Z(M). Since M is self-adjoint, Z(M) is itself a (commutative) von Neumann algebra. A von Neumann algebra N is called a factor if Z(N) is one-dimensional, that is, Z(N) consists of multiples of the identity I.

Theorem Every finite-dimensional von Neumann algebra M is a direct sum of m factors, where m is the dimension of Z(M).

Proof: By Wedderburn's theory of semisimple algebras, Z(M) contains a finite orthogonal set of idempotents (projections) {P_i} such that P_iP_j = 0 for i ≠ j, Σ P_i = I, and

: $Z(\mathbf M) = \bigoplus _i Z(\mathbf M) P_i$

where each Z(M)P_i is a commutative simple algebra. Every complex simple algebras is isomorphic to

the full matrix algebra C^{k × k} for some k. But Z(M)P_i is commutative, therefore one-dimensional.

The projections P_i "diagonalizes" M in a natural way. For M ∈ M, M can be uniquely decomposed into M = Σ MP_i. Therefore,

: ${\mathbf M} = \bigoplus_i {\mathbf M} P_i .$

One can see that Z(MP_i) = Z(M)P_i. So Z(MP_i) is one-dimensional and each MP_i is a factor. This proves the claim.

For general von Neumann algebras, the direct sum is replaced by the direct integral. The above is a special case of the central decomposition of von Neumann algebras.

=Abelian von Neumann algebras=

=Type <math>II_1</math> factors=

References

{{cite book |title=Fundamentals of the Theory of Operator Algebras, Vol. II : Advanced Theory

|first1=R. V.|last1=Kadison|first2=J. R.|last2=Ringrose

|publisher=AMS|year=1997|isbn=978-0821808207|pages=676}}

{{cite book |title=Finite von Neumann Algebras and Masas

|first1=A. M.|last1=Sinclair|first2=R. R.|last2=Smith

|publisher=Cambridge University Press|year=2008|isbn=978-0521719193|pages=410}}

Category:Linear algebra