Math 2.0

Functional analysis Definition

Murray–von Neumann equivalence

Builds on C*-algebraPartial isometry

Definition

Let AA be a C*-algebra. A projection in AA is an element pp with p=p∗=p2p = p^* = p^2. Two projections p,q∈Ap, q \in A are Murray–von Neumann equivalent, written p∼qp \sim q, if there is v∈Av \in A with v∗v=pandvv∗=q.v^* v = p \quad \text{and} \quad v v^* = q.

Remarks

Such a vv is a partial isometry with initial projection pp and final projection qq. The relation is reflexive (v=pv = p), symmetric (v∗v^* in place of vv), and transitive (if v∗v=pv^*v = p, vv∗=qvv^* = q, w∗w=qw^*w = q, ww∗=rww^* = r, then wvwv works for pp and rr). Example: in B(ℓ2(ℕ))B(\ell^2(\N)) let sek=e2ks e_k = e_{2k}; then s∗s=1s^* s = 1 and ss∗s s^* is the projection onto the span of the e2ke_{2k}, so this projection is equivalent to 11. Non-example: in M2(ℂ)M_2(\C), the projections diag⁡(1,0)\operatorname{diag}(1, 0) and 11 are not equivalent, since v∗vv^*v and vv∗vv^* always have the same rank. For K-theory one uses the same relation for projections in matrix algebras of different sizes, with vv a rectangular matrix over AA. Unitarily equivalent projections are Murray–von Neumann equivalent, but the converse fails in general, as the example above shows.

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  1. C*-algebra concept
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Further reading

  1. Web https://en.wikipedia.org/wiki/Operator_K-theory
About this page
TagTB7VCE0RS6
URIm2://TB7VCE0RS6
Kinddefinition
WritingW0 stub
MSC46L05, 46L80, 46L10
DefinesMurray–von Neumann equivalence
UsesC*-algebra, Partial isometry
Changed3 November 2026

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