Harish-Chandra Module
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In mathematics, specifically in the
representation theory of Lie groups In mathematics and theoretical physics, a representation of a Lie group is a linear action of a Lie group on a vector space. Equivalently, a representation is a smooth homomorphism of the group into the group of invertible operators on the vect ...
, a Harish-Chandra module, named after the Indian mathematician and physicist
Harish-Chandra Harish-Chandra FRS (11 October 1923 – 16 October 1983) was an Indian American mathematician and physicist who did fundamental work in representation theory, especially harmonic analysis on semisimple Lie groups. Early life Harish-Chandra wa ...
, is a representation of a real
Lie group In mathematics, a Lie group (pronounced ) is a group that is also a differentiable manifold. A manifold is a space that locally resembles Euclidean space, whereas groups define the abstract concept of a binary operation along with the addit ...
, associated to a general representation, with regularity and finiteness conditions. When the associated representation is a (\mathfrak,K)-module, then its Harish-Chandra module is a representation with desirable factorization properties.


Definition

Let ''G'' be a Lie group and ''K'' a compact
subgroup In group theory, a branch of mathematics, given a group ''G'' under a binary operation ∗, a subset ''H'' of ''G'' is called a subgroup of ''G'' if ''H'' also forms a group under the operation ∗. More precisely, ''H'' is a subgrou ...
of ''G''. If (\pi,V) is a representation of ''G'', then the ''Harish-Chandra module'' of \pi is the subspace ''X'' of ''V'' consisting of the K-finite smooth vectors in ''V''. This means that ''X'' includes exactly those vectors ''v'' such that the map \varphi_v : G \longrightarrow V via :\varphi_v(g) = \pi(g)v is smooth, and the subspace :\text\ is finite-dimensional.


Notes

In 1973, Lepowsky showed that any irreducible (\mathfrak,K)-module ''X'' is isomorphic to the Harish-Chandra module of an irreducible representation of ''G'' on a
Hilbert space In mathematics, Hilbert spaces (named after David Hilbert) allow generalizing the methods of linear algebra and calculus from (finite-dimensional) Euclidean vector spaces to spaces that may be infinite-dimensional. Hilbert spaces arise natu ...
. Such representations are ''admissible'', meaning that they decompose in a manner analogous to the prime factorization of integers. (Of course, the decomposition may have infinitely many distinct factors!) Further, a result of Harish-Chandra indicates that if ''G'' is a ''reductive'' Lie group with maximal compact subgroup ''K'', and ''X'' is an irreducible (\mathfrak,K)-module with a positive definite Hermitian form satisfying : \langle k\cdot v, w \rangle = \langle v, k^\cdot w \rangle and : \langle Y\cdot v, w \rangle = -\langle v, Y\cdot w \rangle for all Y\in \mathfrak and k\in K, then ''X'' is the Harish-Chandra module of a unique irreducible unitary representation of ''G''.


References

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See also

* (g,K)-module * Admissible representation *
Unitary representation In mathematics, a unitary representation of a group ''G'' is a linear representation π of ''G'' on a complex Hilbert space ''V'' such that π(''g'') is a unitary operator for every ''g'' ∈ ''G''. The general theory is well-developed in case ' ...
{{DEFAULTSORT:Harish-Chandra Module Representation theory of Lie groups