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Infunctional analysis, a branch ofmathematics, anoperator algebra is analgebra ofcontinuouslinear operators on atopological vector space, with the multiplication given by thecomposition of mappings.
The results obtained in the study of operator algebras are often phrased inalgebraic terms, while the techniques used are often highlyanalytic.[1] Although the study of operator algebras is usually classified as a branch of functional analysis, it has direct applications torepresentation theory,differential geometry,quantum statistical mechanics,quantum information, andquantum field theory.
Operator algebras can be used to study arbitrary sets of operators with little algebraic relationsimultaneously. From this point of view, operator algebras can be regarded as a generalization ofspectral theory of a single operator. In general, operator algebras arenon-commutativerings.
An operator algebra is typically required to beclosed in a specified operatortopology inside the whole algebra of continuous linear operators. In particular, it is a set of operators with both algebraic and topological closure properties. In some disciplines such properties areaxiomatized and algebras with certain topological structure become the subject of the research.
Though algebras of operators are studied in various contexts (for example, algebras ofpseudo-differential operators acting on spaces ofdistributions), the termoperator algebra is usually used in reference to algebras ofbounded operators on aBanach space or, even more specifically in reference to algebras of operators on aseparableHilbert space, endowed with theoperator norm topology.
In the case of operators on a Hilbert space, theHermitian adjoint map on operators gives a naturalinvolution, which provides an additional algebraic structure that can be imposed on the algebra. In this context, the best studied examples areself-adjoint operator algebras, meaning that they are closed under taking adjoints. These includeC*-algebras,von Neumann algebras, andAW*-algebras. C*-algebras can be easily characterized abstractly by a condition relating the norm, involution and multiplication. Such abstractly defined C*-algebras can be identified to a certain closedsubalgebra of the algebra of the continuous linear operators on a suitable Hilbert space. A similar result holds for von Neumann algebras.
Commutative self-adjoint operator algebras can be regarded as the algebra ofcomplex-valued continuous functions on alocally compact space, or that ofmeasurable functions on astandard measurable space. Thus, general operator algebras are often regarded as a noncommutative generalizations of these algebras, or the structure of thebase space on which the functions are defined. This point of view is elaborated as the philosophy ofnoncommutative geometry, which tries to study various non-classical and/or pathological objects by noncommutative operator algebras.
Examples of operator algebras that are not self-adjoint include: