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 .

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.