Definition

A MM is finite if its identity 1M1_M is a in MM. Explicitly, whenever vMv\in M satisfies vv=1Mv^*v=1_M, one must also have vv=1Mvv^*=1_M; thus every isometry belonging to MM is unitary. Equivalently, no proper subprojection of 1M1_M is to 1M1_M. Finiteness is an internal comparison property of projections. It does not require MM to be finite-dimensional, a factor, or represented on a finite-dimensional .

Equivalent formulations and structure

Finiteness of the identity forces every projection in MM to be finite. Conversely, that condition plainly includes the identity. A major structure theorem supplies every finite von Neumann algebra with a unique faithful normal center-valued trace normalized at 1M1_M; its scalar specializations organize the ordinary finite traces. See Kadison–Ringrose, §6.5 for the projection-comparison and trace formulations.

Finite factors split into two classes. A is a matrix algebra, whereas a finite factor without nonzero is of type II1\mathrm{II}_1. A finite von Neumann algebra with nontrivial center can have both sorts of central summands.

Examples and non-examples

Every matrix algebra Mn(C)M_n(\mathbb C) is finite. An infinite-dimensional is also finite: a in an abelian algebra has equal initial and final projections.

By contrast, B(H)B(H) for an infinite-dimensional Hilbert space HH is not finite. A unilateral shift is an isometry whose range projection is strictly smaller than the identity.

Conventions and scope
References
  1. R. V. Kadison and J. R. Ringrose, Fundamentals of the Theory of Operator Algebras, vol. II, American Mathematical Society, 1997. DOI record. Relevant: §6.5 on finite von Neumann algebras, comparison, and center-valued traces.
  2. M. Takesaki, Theory of Operator Algebras I, Springer, 1979. DOI record. Relevant: Chapter V, §2 on finite von Neumann algebras.