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GROUP ALGEBRA OF A FINITE GROUP Given a Finite Group ''G'', define the group algebra ''CG'' as the Vector Space over the Complex Number s, with Basis Vector s corresponding to the elements . The Algebra structure on this vector space is defined as :. A Representation of the algebra ''CG'' on a vector space ''V'' is the algebra homomorphism :. That is, a representation is a Left ''CG''-module . Any group representation then extends linearly to an algebra representation . Thus, representations of the group correspond exactly to representations of the algebra, and so, in a certain sense, talking about the one is the same as talking about the other. The ''center'' of the group algebra is the set of vectors which commute with the action of the group ''G'' on the vector space ''V'': : GROUP ALGEBRAS OF TOPOLOGICAL GROUPS: ''C''<SUB>''C''</SUB>(''G'') For the purposes of Functional Analysis , and in particular of Harmonic Analysis , one wishes to carry over the group ring construction to Topological Group s ''G''. In case ''G'' is a Locally Compact Hausdorff Group , ''G'' carries an essentially unique left-invariant countably additive Borel Measure μ called Haar Measure . Using the Haar measure, one can define a Convolution Operation on the space ''C''''c''(''G'') of complex-valued functions on ''G'' with Compact Support ; ''C''''c''(''G'') can then be given any of various Norm s and the Completion will be a group algebra. To define the convolution operation, let ''f'' and ''g'' be two functions in ''C''''c''(''G''). For ''t'' in ''G'', define
''C''''c''(''G'') also has a natural involution defined by:
Theorem. If ''C''''c''(''G'') is given the norm | ||
|   | :<math> \f\ {C^} : | \sup_\pi \\pi(f)\ \quad </math> |
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