Definition
Projection in a C*-algebra
A self-adjoint idempotent in a C*-algebra.
Definition
Let be a -algebra. A projection in is an element satisfying
Thus a projection is a self-adjoint idempotent. The definition makes sense whether or not is unital; the zero element is always a projection, while a multiplicative identity is a projection when it exists. If is represented faithfully on a Hilbert space, 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 . Every nonzero projection has norm one, and is a projection when is unital. In a concrete operator algebra, self-adjointness distinguishes orthogonal projections from general idempotent operators, whose range and kernel need not be orthogonal. These facts follow directly from the continuous functional calculus Murphy, §2.2.
Equivalence and stabilization
Projections and are Murray–von Neumann equivalent when there is a partial isometry with and . This records isomorphism of the corresponding projective modules and is weaker than equality. One also studies projections in matrix algebras ; block sum provides the stabilization operation used in operator -theory.
Role in K-theory
For a unital -algebra, the group is built from stable equivalence classes of projections in the matrix algebras over . 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 -class” may live in a matrix algebra or a unitization rather than in itself.
References
- Bruce Blackadar, K-Theory for Operator Algebras, 2nd ed., Cambridge University Press, 1998. Publisher record. Relevant: Chapter III, especially §5, on projections and .
- Gerard J. Murphy, -Algebras and Operator Theory, Academic Press, 1990. DOI record. Relevant: §§2.2–2.3 on projections and functional calculus.