Definition

Let AA be a . A projection in AA is an element pAp\in A satisfying

p=p=p2.p=p^*=p^2.

Thus a projection is a self-adjoint . The definition makes sense whether or not AA is unital; the zero element is always a projection, while a multiplicative identity is a projection when it exists. If AA is represented faithfully on a , pp acts as the orthogonal projection onto its closed range. This abstract definition does not require a particular representation or a subspace chosen in advance.

Spectral and geometric properties

The spectrum of a projection lies in {0,1}\{0,1\}. Every nonzero projection has norm one, and 1p1-p is a projection when AA is unital. In a concrete operator algebra, self-adjointness distinguishes from general idempotent operators, whose range and kernel need not be orthogonal. These facts follow directly from the Murphy, §2.2.

Equivalence and stabilization

Projections pp and qq are Murray–von Neumann equivalent when there is a vv with vv=pv^*v=p and vv=qvv^*=q. This records isomorphism of the corresponding and is weaker than equality. One also studies projections in matrix algebras Mn(A)M_n(A); block sum provides the stabilization operation used in operator KK-theory.

Role in K-theory

For a unital CC^*-algebra, the group is built from stable of projections in the matrix algebras over AA. For a nonunital algebra, one passes to a unitization and retains the kernel of the map induced by the scalar quotient. Consequently, “a projection defining a K0K_0-class” may live in a matrix algebra or a unitization rather than in AA itself.

References
  1. Bruce Blackadar, K-Theory for Operator Algebras, 2nd ed., Cambridge University Press, 1998. Publisher record. Relevant: Chapter III, especially §5, on projections and K0K_0.
  2. Gerard J. Murphy, CC^*-Algebras and Operator Theory, Academic Press, 1990. DOI record. Relevant: §§2.2–2.3 on projections and functional calculus.