Talk:C*-algebra

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$$ \newcommand{\abs}[1]{\left|#1\right|} \newcommand{\norm}[1]{\left\|#1\right\|} $$ A Banach algebra $A$ over the field of complex numbers, with an involution $x \rightarrow x^*$, $x \in A$, such that the norm and the involution are connected by the relation $\norm{x^* x} = \norm{x}^2$ for any element $x \in A$. $C^*$-algebras were introduced in 1943 [GeNe] under the name of totally regular rings; they are also known under the name of $B^*$-algebras. The most important examples of $C^*$-algebras are:

1) The algebra $C_0(X)$ of continuous complex-valued functions on a locally compact Hausdorff space $X$ which tend towards zero at infinity (i.e. continuous functions $f$ on $X$ such that, for any $\epsilon > 0$, the set of points $x \in X$ which satisfy the condition $\abs{f(x)} \geq \epsilon$ is compact in $X$); $C_0(X)$ has the uniform norm $$ \norm{f} = \sup_{x \in X} \abs{f(x)}. $$ The involution in $C_0(X)$ is defined as transition to the complex-conjugate function: $f^*(x) = \overline{f(x)}$. Any commutative $C^*$-algebra $A$ is isometrically and symmetrically isomorphic (i.e. is isomorphic as a Banach algebra $A$ with involution) to the $C^*$-algebra $C_0(X)$, where $X$ is the space of maximal ideals of $A$ endowed with the Gel'fand topology [GeNe], [Na], [Di].

2) The algebra $L(H)$ of all bounded linear operators on a Hilbert space $H$, considered with respect to the ordinary linear operations and operator multiplication. The involution in $L(H)$ is defined as transition to the adjoint operator, and the norm is defined as the ordinary operator norm.

A subset $ $ is said to be self-adjoint if $ $, where $ $. Any closed self-adjoint subalgebra $ $ of a $C^*$-algebra $ $ is a $C^*$-algebra with respect to the linear operations, multiplication, involution, and norm taken from $ $; $ $ is said to be a $ $-subalgebra of $ $. Any $C^*$-algebra is isometrically and symmetrically isomorphic to a $ $-subalgebra of some $C^*$-algebra of the form $ $. Any closed two-sided ideal $ $ in a $C^*$-algebra is self-adjoint (thus $ $ is a $ $-subalgebra of $ $), and the quotient algebra $ $, endowed with the natural linear operations, multiplication, involution, and quotient space norm, is a $C^*$-algebra. The set $ $ of completely-continuous linear operators on a Hilbert space $ $ is a closed two-sided ideal in $ $. If $ $ is a $C^*$-algebra and $ $ is the algebra with involution obtained from $ $ by addition of a unit element, there exists a unique norm on $ $ which converts $ $ into a $C^*$-algebra and which extends the norm on $ $. Moreover, the operations of bounded direct sum and tensor product [Di], [Sa] have been defined for $C^*$-algebras.

As in all symmetric Banach algebras with involution, in a $C^*$-algebra $ $ it is possible to define the following subsets: the real linear space $ $ of Hermitian elements; the set of normal elements; the multiplicative group $ $ of unitary elements (if $ $ contains a unit element); and the set $ $ of positive elements. The set $ $ is a closed cone in $ $, $ $, $ $, and the cone $ $ converts $ $ into a real ordered vector space. If $ $ contains a unit element 1, then 1 is an interior point of the cone $ $. A linear functional $ $ on $ $ is called positive if $ $ for all $ $; such a functional is continuous. If $ $, where $ $ is a $ $-subalgebra of $ $, the spectrum of $ $ in $ $ coincides with the spectrum of $ $ in $ $. The spectrum of a Hermitian element is real, the spectrum of a unitary element lies on the unit circle, and the spectrum of a positive element is non-negative. A functional calculus for the normal elements of a $C^*$-algebra has been constructed. Any $C^*$-algebra $ $ has an approximate unit, located in the unit ball of $ $ and formed by positive elements of $ $. If $ $ are closed two-sided ideals in $ $, then $ $ is a closed two-sided ideal in $ $ and $ $. If $ $ is a closed two-sided ideal in $ $ and $ $ is a closed two-sided ideal in $ $, then $ $ is a closed two-sided ideal in $ $. Any closed two-sided ideal is the intersection of the primitive two-sided ideals in which it is contained; any closed left ideal in $ $ is the intersection of the maximal regular left ideals in which it is contained.

Any *-isomorphism of a $C^*$-algebra is isometric. Any *-isomorphism $ $ of a Banach algebra $ $ with involution into a $C^*$-algebra $ $ is continuous, and $ $ for all $ $. In particular, all representations of a Banach algebra with involution (i.e. all *-homomorphism of $ $ into a $C^*$-algebra of the form $ $) are continuous. The theory of representations of $C^*$-algebras forms a significant part of the theory of $C^*$-algebras, and the applications of the theory of $C^*$-algebras are related to the theory of representations of $C^*$-algebras. The properties of representations of $C^*$-algebras make it possible to construct for each $C^*$-algebra $ $ a topological space $ $, called the spectrum of the $C^*$-algebra $ $, and to endow this space with a Mackey–Borel structure. In the general case, the spectrum of a $C^*$-algebra does not satisfy any separation axiom, but is a locally compact Baire space.

A $C^*$-algebra $ $ is said to be a CCR-algebra (respectively, a GCR-algebra) if the relation $ $ (respectively, $ $) is satisfied for any non-null irreducible representation $ $ of the $C^*$-algebra $ $ in a Hilbert space $ $.

A $C^*$-algebra $ $ is said to be an NGCR-algebra if $ $ does not contain non-zero closed two-sided $ $-ideals (i.e. ideals which are $C^*$-algebras). Any $C^*$-algebra contains a maximal two-sided $ $-ideal $ $, and the quotient algebra $ $ is an $C^*$-algebra. Any $C^*$-algebra contains an increasing family of closed two-sided ideals $ $, indexed by ordinals $ $, $ $, such that $ $, $ $, $ $ is a $C^*$-algebra for all $ $, and $ $ for limit ordinals $ $. The spectrum of a $C^*$-algebra contains an open, everywhere-dense, separable, locally compact subset.

A $C^*$-algebra $ $ is said to be a $C^*$-algebra of type I if, for any representation $ $ of the $C^*$-algebra $ $ in a Hilbert space $ $, the von Neumann algebra generated by the family $ $ in $ $ is a type I von Neumann algebra. For a $C^*$-algebra, the following conditions are equivalent: a) $ $ is a $C^*$-algebra of type I; b) $ $ is a $C^*$-algebra; and c) any quotient representation of the $C^*$-algebra $ $ is a multiple of the irreducible representation. If $ $ satisfies these conditions, then: 1) two irreducible representations of the $C^*$-algebra $ $ are equivalent if and only if their kernels are identical; and 2) the spectrum of the $C^*$-algebra $ $ is a $ $-space. If $ $ is a separable $C^*$-algebra, each of the conditions 1) and 2) is equivalent to the conditions a)–c). In particular, each separable $C^*$-algebra with a unique (up to equivalence) irreducible representation, is isomorphic to the $C^*$-algebra $ $ for some Hilbert space $ $.

Let $ $ be a $C^*$-algebra, and let $ $ be a set of elements $ $ such that the function $ $ is finite and continuous on the spectrum of $ $. If the linear envelope of $ $ is everywhere dense in $ $, then $ $ is said to be a $C^*$-algebra with continuous trace. The spectrum of such a $C^*$-algebra is separable and, under certain additional conditions, a $C^*$-algebra with a continuous trace may be represented as the algebra of vector functions on its spectrum $ $ [Di].

Let $ $ be a $C^*$-algebra, let $ $ be the set of positive linear functionals on $ $ with norm $ $ and let $ $ be the set of non-zero boundary points of the convex set $ $. Then $ $ will be the set of pure states of $ $. Let $ $ be a $ $-subalgebra of $ $. If $ $ is a $C^*$-algebra and if $ $ separates the points of the set $ $, i.e. for any $ $, $ $, there exists an $ $ such that $ $, then $ $ (the Stone–Weierstrass theorem). If $ $ is any $C^*$-algebra and $ $ separates the points of the set $ $, then $ $.

The second dual space $ $ of a $C^*$-algebra $ $ is obviously provided with a multiplication converting $ $ into a $C^*$-algebra isomorphic to some von Neumann algebra; this algebra is named the von Neumann algebra enveloping the $C^*$-algebra [Di], [Sa].

The theory of $C^*$-algebras has numerous applications in the theory of representations of groups and symmetric algebras [Di], the theory of dynamical systems [Sa], statistical physics and quantum field theory [Ru], and also in the theory of operators on a Hilbert space [Do].

Comments

If $ $ over $ $ is an algebra with involution, i.e. if there is an operation $ $ satisfying $ $, $ $, $ $, the Hermitian, normal and positive elements are defined as follows. The element $ $ is a Hermitian element if $ $; it is a normal element if $ $ and it is a positive element if $ $ for some $ $. An element $ $ is a unitary element if $ $. An algebra with involution is also sometimes called a symmetric algebra (or symmetric ring), cf., e.g., [Na]. However, this usage conflicts with the concept of a symmetric algebra as a special kind of Frobenius algebra, cf. Frobenius algebra.

Recent discoveries have revealed connections with, and applications to, algebraic topology. If $ $ is a compact metrizable space, a group, $ $, can be formed from $ $-extensions of the compact operators by $ $,

$$ $$ In [BrDoFi], $ $ is shown to be a homotopy invariant functor of $ $ which may be identified with the topological $ $-homology group, $ $. In [At] M.F. Atiyah attempted to make a description of $ $-homology, $ $, in terms of elliptic operators [Do2], p. 58. In [Ka], [Ka2] G.G. Kasparov developed a solution to this problem. Kasparov and others have used the equivariant version of Kasparov $ $-theory to prove the strong Novikov conjecture on higher signatures in many cases (see [Bl], pp. 309-314).

In addition, deep and novel connections between $ $-theory and operator algebras (cf. Operator ring) were recently discovered by A. Connes [Co]. Finally, V.F.R. Jones [Jo] has exploited operator algebras to provide invariants of topological knots (cf. Knot theory).

Further details on recent developments may be found in [Bl], [Do2].

References

[At]	M.F. Atiyah, "Global theory of elliptic operators", Proc. Internat. Conf. Funct. Anal. Related Topics, Univ. Tokyo Press (1970) MR0266247 Zbl 0193.43601
[Bl]	B. Blackadar, "$ $-theory for operator algebras", Springer (1986) MR0859867 Zbl 0597.46072
[BrDoFi]	L.G. Brown, R.G. Douglas, P.A. Filmore, "Extensions of $C^*$-algebras and $ $-homology" Ann. of Math. (2), 105 (1977) pp. 265–324
[Co]	A. Connes, "Non-commutative differential geometry" Publ. Math. IHES, 62 (1986) pp. 257–360 Zbl 0657.55006 Zbl 0592.46056 Zbl 0564.58002
[Di]	J. Dixmier, "$ $ algebras", North-Holland (1977) (Translated from French) MR0498740 MR0458185 Zbl 0372.46058 Zbl 0346.17010 Zbl 0339.17007
[Do]	R.G. Douglas, "Banach algebra techniques in operator theory", Acad. Press (1972) MR0361893 Zbl 0247.47001
[Do2]	R.G. Douglas, "$C^*$-algebra extensions and $ $-homology", Princeton Univ. Press (1980) MR0571362
[GeNe]	I.M. Gel'fand, M.A. [M.A. Naimark] Neumark, "On the imbedding of normed rings in the rings of operators in Hilbert space" Mat. Sb., 12 (54) : 2 (1943) pp. 197–213 MR9426
[Jo]	V.F.R. Jones, "A polynomial invariant for knots via von Neumann algebras" Bull. Amer. Math. Soc., 12 (1985) pp. 103–111 MR0766964 Zbl 0564.57006
[Ka]	G.G. Kasparov, "The generalized index of elliptic operators" Funct. Anal. and Its Appl., 7 (1973) pp. 238–240 Funkt. Anal. i Prilozhen., 7 (1973) pp. 82–83 MR445561 Zbl 0305.58017
[Ka2]	G.G. Kasparov, "Topological invariants of elliptic operators I. $ $-homology" Math. USSR-Izv., 9 (1975) pp. 751–792 Izv. Akad. Nauk SSSR, 4 (1975) pp. 796–838 MR488027
[Na]	M.A. Naimark, "Normed rings", Reidel (1984) (Translated from Russian) MR1292007 MR0355601 MR0355602 MR0205093 MR0110956 MR0090786 MR0026763 Zbl 0218.46042 Zbl 0137.31703 Zbl 0089.10102 Zbl 0073.08902
[Ru]	D. Ruelle, "Statistical mechanics: rigorous results", Benjamin (1974) MR0289084 Zbl 0997.82506 Zbl 1016.82500 Zbl 0177.57301
[Sa]	S. Sakai, "$C^*$-algebras and $W^*$-algebras", Springer (1971) MR0442701 MR0399878 MR0318902 MR0293415 MR0293414
[Ta]	M. Takesaki, "Theory of operator algebras", 1, Springer (1979) MR0548728 Zbl 0436.46043