# C*-algebra

In mathematics, specifically in functional analysis, a **C ^{∗}-algebra** (pronounced "C-star") is a Banach algebra together with an involution satisfying the properties of the adjoint. A particular case is that of a complex algebra

*A*of continuous linear operators on a complex Hilbert space with two additional properties:

C*-algebras were first considered primarily for their use in quantum mechanics to model algebras of physical observables. This line of research began with Werner Heisenberg's matrix mechanics and in a more mathematically developed form with Pascual Jordan around 1933. Subsequently, John von Neumann attempted to establish a general framework for these algebras, which culminated in a series of papers on rings of operators. These papers considered a special class of C*-algebras which are now known as von Neumann algebras.

Around 1943, the work of Israel Gelfand and Mark Naimark yielded an abstract characterisation of C*-algebras making no reference to operators on a Hilbert space.

C*-algebras are now an important tool in the theory of unitary representations of locally compact groups, and are also used in algebraic formulations of quantum mechanics. Another active area of research is the program to obtain classification, or to determine the extent of which classification is possible, for separable simple nuclear C*-algebras.

We begin with the abstract characterization of C*-algebras given in the 1943 paper by Gelfand and Naimark.

**Remark.** The first three identities say that *A* is a *-algebra. The last identity is called the **C* identity** and is equivalent to:

which is sometimes called the B*-identity. For history behind the names C*- and B*-algebras, see the history section below.

The C*-identity is a very strong requirement. For instance, together with the spectral radius formula, it implies that the C*-norm is uniquely determined by the algebraic structure:

A bounded linear map, *π* : *A* → *B*, between C*-algebras *A* and *B* is called a ***-homomorphism** if

In the case of C*-algebras, any *-homomorphism *π* between C*-algebras is contractive, i.e. bounded with norm ≤ 1. Furthermore, an injective *-homomorphism between C*-algebras is isometric. These are consequences of the C*-identity.

A bijective *-homomorphism *π* is called a **C*-isomorphism**, in which case *A* and *B* are said to be **isomorphic**.

The term B*-algebra was introduced by C. E. Rickart in 1946 to describe Banach *-algebras that satisfy the condition:

The term C*-algebra was introduced by I. E. Segal in 1947 to describe norm-closed subalgebras of *B*(*H*), namely, the space of bounded operators on some Hilbert space *H*. 'C' stood for 'closed'.^{[2]}^{[3]} In his paper Segal defines a C*-algebra as a "uniformly closed, self-adjoint algebra of bounded operators on a Hilbert space".^{[4]}

C*-algebras have a large number of properties that are technically convenient. Some of these properties can be established by using the continuous functional calculus or by reduction to commutative C*-algebras. In the latter case, we can use the fact that the structure of these is completely determined by the Gelfand isomorphism.

Self-adjoint elements are those of the form *x*=*x**. The set of elements of a C*-algebra *A* of the form *x*x* forms a closed convex cone. This cone is identical to the elements of the form *xx**. Elements of this cone are called *non-negative* (or sometimes *positive*, even though this terminology conflicts with its use for elements of **R**.)

The set of self-adjoint elements of a C*-algebra *A* naturally has the structure of a partially ordered vector space; the ordering is usually denoted ≥. In this ordering, a self-adjoint element *x* of *A* satisfies *x* ≥ 0 if and only if the spectrum of *x* is non-negative,^{[clarification needed]} if and only if *x* = *s*s* for some *s*. Two self-adjoint elements *x* and *y* of *A* satisfy *x* ≥ *y* if *x*−*y* ≥ 0.

This partially ordered subspace allows the definition of a positive linear functional on a C*-algebra, which in turn is used to define the states of a C*-algebra, which in turn can be used to construct the spectrum of a C*-algebra using the GNS construction.

Using approximate identities, one can show that the algebraic quotient of a C*-algebra by a closed proper two-sided ideal, with the natural norm, is a C*-algebra.

Similarly, a closed two-sided ideal of a C*-algebra is itself a C*-algebra.

The algebra M(*n*, **C**) of *n* × *n* matrices over **C** becomes a C*-algebra if we consider matrices as operators on the Euclidean space, **C**^{n}, and use the operator norm ||·|| on matrices. The involution is given by the conjugate transpose. More generally, one can consider finite direct sums of matrix algebras. In fact, all C*-algebras that are finite dimensional as vector spaces are of this form, up to isomorphism. The self-adjoint requirement means finite-dimensional C*-algebras are semisimple, from which fact one can deduce the following theorem of Artin–Wedderburn type:

**Theorem.** A finite-dimensional C*-algebra, *A*, is canonically isomorphic to a finite direct sum

where min *A* is the set of minimal nonzero self-adjoint central projections of *A*.

A **†-algebra** (or, more explicitly, a *†-closed algebra*) is the name occasionally used in physics^{[5]} for a finite-dimensional C*-algebra. The dagger, †, is used in the name because physicists typically use the symbol to denote a Hermitian adjoint, and are often not worried about the subtleties associated with an infinite number of dimensions. (Mathematicians usually use the asterisk, *, to denote the Hermitian adjoint.) †-algebras feature prominently in quantum mechanics, and especially quantum information science.

An immediate generalization of finite dimensional C*-algebras are the approximately finite dimensional C*-algebras.

The prototypical example of a C*-algebra is the algebra *B(H)* of bounded (equivalently continuous) linear operators defined on a complex Hilbert space *H*; here *x** denotes the adjoint operator of the operator *x* : *H* → *H*. In fact, every C*-algebra, *A*, is *-isomorphic to a norm-closed adjoint closed subalgebra of *B*(*H*) for a suitable Hilbert space, *H*; this is the content of the Gelfand–Naimark theorem.

Let *H* be a separable infinite-dimensional Hilbert space. The algebra *K*(*H*) of compact operators on *H* is a norm closed subalgebra of *B*(*H*). It is also closed under involution; hence it is a C*-algebra.

Concrete C*-algebras of compact operators admit a characterization similar to Wedderburn's theorem for finite dimensional C*-algebras:

where the (C*-)direct sum consists of elements (*T _{i}*) of the Cartesian product Π

*K*(

*H*) with ||

_{i}*T*|| → 0.

_{i}*K*(*H*) is a two-sided closed ideal of *B*(*H*). For separable Hilbert spaces, it is the unique ideal. The quotient of *B*(*H*) by *K*(*H*) is the Calkin algebra.

Given a Banach *-algebra *A* with an approximate identity, there is a unique (up to C*-isomorphism) C*-algebra **E**(*A*) and *-morphism π from *A* into **E**(*A*) that is universal, that is, every other continuous *-morphism π ' : *A* → *B* factors uniquely through π. The algebra **E**(*A*) is called the **C*-enveloping algebra** of the Banach *-algebra *A*.

Of particular importance is the C*-algebra of a locally compact group *G*. This is defined as the enveloping C*-algebra of the group algebra of *G*. The C*-algebra of *G* provides context for general harmonic analysis of *G* in the case *G* is non-abelian. In particular, the dual of a locally compact group is defined to be the primitive ideal space of the group C*-algebra. See spectrum of a C*-algebra.

Von Neumann algebras, known as W* algebras before the 1960s, are a special kind of C*-algebra. They are required to be closed in the weak operator topology, which is weaker than the norm topology.

The Sherman–Takeda theorem implies that any C*-algebra has a universal enveloping W*-algebra, such that any homomorphism to a W*-algebra factors through it.

A C*-algebra *A* is of type I if and only if for all non-degenerate representations π of *A* the von Neumann algebra π(*A*)′′ (that is, the bicommutant of π(*A*)) is a type I von Neumann algebra. In fact it is sufficient to consider only factor representations, i.e. representations π for which π(*A*)′′ is a factor.

A locally compact group is said to be of type I if and only if its group C*-algebra is type I.

However, if a C*-algebra has non-type I representations, then by results of James Glimm it also has representations of type II and type III. Thus for C*-algebras and locally compact groups, it is only meaningful to speak of type I and non type I properties.

In quantum mechanics, one typically describes a physical system with a C*-algebra *A* with unit element; the self-adjoint elements of *A* (elements *x* with *x** = *x*) are thought of as the *observables*, the measurable quantities, of the system. A *state* of the system is defined as a positive functional on *A* (a **C**-linear map φ : *A* → **C** with φ(*u*u*) ≥ 0 for all *u* ∈ *A*) such that φ(1) = 1. The expected value of the observable *x*, if the system is in state φ, is then φ(*x*).

This C*-algebra approach is used in the Haag-Kastler axiomatization of local quantum field theory, where every open set of Minkowski spacetime is associated with a C*-algebra.