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Mackey support of Homs between finite principal series
Statement
Let , let be a prime power, put with Borel and diagonal torus , and let with associated principal series modules , (The principal series module for finite GL_n). For let be the conjugate character (Conjugate representations and conjugate characters on conjugate subgroups, Diagonal torus characters and the Weyl action). Then the Harish-Chandra adjunction for the Borel combined with the parabolic Mackey formula gives an isomorphism of -vector spaces each summand is one-dimensional when and zero otherwise, and therefore In particular precisely when lies in the -orbit of . The Mackey decomposition exhibits as a direct sum of one-dimensional subspaces indexed by the set , so its nonzero elements in a single summand each span a basis of that summand; the resulting basis is well defined up to multiplication of each element by a nonzero scalar. No choice principle is used, all direct sums being finite.
Facts & Assumptions
Given: with Borel , characters , the modules and , and the set .
Harish-Chandra adjunction: is left adjoint to (Harish-Chandra induction is left adjoint to restriction); for and the Borel the induction is the principal series module (The principal series module for finite GL_n).
Parabolic Mackey formula for with respect to standard parabolics: for , and a set of representatives of the -double cosets, with , (Parabolic Mackey formula for finite GL_n). The - double cosets are the cells , one for each , by the Bruhat decomposition (Bruhat decomposition of GL_n over a finite field). The conjugate character is (Conjugate representations and conjugate characters on conjugate subgroups).
For finite-dimensional complex -modules the dimension of equals the character inner product; applied to the finite abelian group and one-dimensional characters, the space is one-dimensional when the characters coincide and zero otherwise (The class-function inner product equals ).
Proof
Harish-Chandra adjunction with , , and gives a -linear isomorphism .
Specialize the Mackey formula of [F2] to and : here , and for the representative of a double coset one has and , so , because unipotent elements are conjugate to unipotent ones and the only diagonal unipotent matrix is the identity, and ; hence is the identity functor and . As the double cosets are indexed by with representatives by [F2], this gives an isomorphism of -modules
Substituting step 1.2 into step 1.1 and distributing the finite direct sum over gives . By [F3] each summand is a -vector space of dimension when , and dimension otherwise, because a nonzero homomorphism between the one-dimensional characters and exists exactly when they are equal; here by [F2].
Taking dimensions in step 2.1 gives , and this number is nonzero precisely when lies in the -orbit of , since for some is exactly the statement that and lie in one orbit. The same decomposition exhibits as the direct sum of the one-dimensional subspaces carried by the indices with ; picking any nonzero element in each of these subspaces gives a basis indexed by that set, and any two such choices differ by nonzero scalars.
Steps 1.1 and 1.2 produce the isomorphism, step 2.1 identifies its summands, and step 3.1 records the dimension count, the nonvanishing criterion and the basis statement; all sums are finite over the finite group , and every map used is a given adjunction or Mackey isomorphism, so no choice principle is used.
Depends on
- The principal series module for finite GL_n
- Harish-Chandra induction is left adjoint to restriction
- Parabolic Mackey formula for finite GL_n
- Conjugate representations and conjugate characters on conjugate subgroups
- The class-function inner product $\langle\chi_V,\chi_W\rangle$ equals $\dim\operatorname{Hom}_G(W,V)$
- Diagonal torus characters and the Weyl action
- Bruhat decomposition of GL_n over a finite field
Used by
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Sources
- Masao Oi, Representation Theory of Finite Groups of Lie Type - the Mackey computation in the proofs of Propositions 2.7-2.8 (the direct sum of Hom_T terms indexed by B\G/B), printed pp. 10-13 (standard reference, not scraped)
- Jay Taylor, Finite Reductive Groups - Section 5 (Harish-Chandra restriction and double-coset decompositions), printed pp. 42-46 (standard reference, not scraped)
- Olivier Dudas and Jean Michel, Lectures on Finite Reductive Groups and Their Representations - Section 11.3 (Mackey formula for a split torus), printed pp. 47-49 (standard reference, not scraped)