representation on coordinate rings

In mathematics, a representation on coordinate rings is a representation of a group on coordinate rings of affine varieties.

Let X be an affine algebraic variety over an algebraically closed field k of characteristic zero with the action of a reductive algebraic group G.G is not assumed to be connected so that the results apply to finite groups. G then acts on the coordinate ring k[X] of X as a left regular representation: (g \cdot f)(x) = f(g^{-1} x). This is a representation of G on the coordinate ring of X.

The most basic case is when X is an affine space (that is, X is a finite-dimensional representation of G) and the coordinate ring is a polynomial ring. The most important case is when X is a symmetric variety; i.e., the quotient of G by a fixed-point subgroup of an involution.

Isotypic decomposition

Let k[X]_{(\lambda)} be the sum of all G-submodules of k[X] that are isomorphic to the simple module V^{\lambda}; it is called the \lambda-isotypic component of k[X]. Then there is a direct sum decomposition:

:k[X] = \bigoplus_{\lambda} k[X]_{(\lambda)}

where the sum runs over all simple G-modules V^{\lambda}. The existence of the decomposition follows, for example, from the fact that the group algebra of G is semisimple since G is reductive.

X is called multiplicity-free (or spherical variety{{harvnb|Goodman|Wallach|2009|loc=Remark 12.2.2.}}) if every irreducible representation of G appears at most one time in the coordinate ring; i.e., \operatorname{dim} k[X]_{(\lambda)} \le \operatorname{dim} V^{\lambda}.

For example, G is multiplicity-free as G \times G-module. More precisely, given a closed subgroup H of G, define

:\phi_{\lambda}: V^{{\lambda}*} \otimes (V^{\lambda})^H \to k[G/H]_{(\lambda)}

by setting \phi_{\lambda}(\alpha \otimes v)(gH) = \langle \alpha, g \cdot v \rangle and then extending \phi_{\lambda} by linearity. The functions in the image of \phi_{\lambda} are usually called matrix coefficients. Then there is a direct sum decomposition of G \times N-modules (N the normalizer of H)

:k[G/H] = \bigoplus_{\lambda} \phi_{\lambda}(V^{{\lambda}*} \otimes (V^{\lambda})^H),

which is an algebraic version of the Peter–Weyl theorem (and in fact the analytic version is an immediate consequence.) Proof: let W be a simple G \times N-submodules of k[G/H]_{(\lambda)}. We can assume V^{\lambda} = W. Let \delta_1 be the linear functional of W such that \delta_1(w) = w(1). Then w(gH) = \phi_{\lambda}(\delta_1 \otimes w)(gH).

That is, the image of \phi_{\lambda} contains k[G/H]_{(\lambda)} and the opposite inclusion holds since \phi_{\lambda} is equivariant.

Examples

  • Let v_{\lambda} \in V^{\lambda} be a B-eigenvector and X the closure of the orbit G \cdot v_\lambda. It is an affine variety called the highest weight vector variety by Vinberg–Popov. It is multiplicity-free.

The Kostant–Rallis situation

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See also

Notes

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References

  • {{cite book | last1=Goodman | first1=Roe |last2=Wallach |first2=Nolan R. |author2-link=Nolan R. Wallach | title=Symmetry, Representations, and Invariants | year=2009 | isbn=978-0-387-79852-3 | doi=10.1007/978-0-387-79852-3 | oclc=699068818 | language=de}}

Category:Group theory

Category:Representation theory

Category:Representation theory of groups