1,464 research outputs found

    Weyl group action and semicanonical bases

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    Let U be the enveloping algebra of a symmetric Kac-Moody algebra. The Weyl group acts on U, up to a sign. In addition, the positive subalgebra U^+ contains a so-called semicanonical basis, with remarkable properties. The aim of this paper is to show that these two structures are as compatible as possible

    How to compute the Frobenius-Schur indicator of a unipotent character of a finite Coxeter system

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    For each finite, irreducible Coxeter system (W,S)(W,S), Lusztig has associated a set of "unipotent characters" \Uch(W). There is also a notion of a "Fourier transform" on the space of functions \Uch(W) \to \RR, due to Lusztig for Weyl groups and to Brou\'e, Lusztig, and Malle in the remaining cases. This paper concerns a certain WW-representation ϱW\varrho_{W} in the vector space generated by the involutions of WW. Our main result is to show that the irreducible multiplicities of ϱW\varrho_W are given by the Fourier transform of a unique function \epsilon : \Uch(W) \to \{-1,0,1\}, which for various reasons serves naturally as a heuristic definition of the Frobenius-Schur indicator on \Uch(W). The formula we obtain for ϵ\epsilon extends prior work of Casselman, Kottwitz, Lusztig, and Vogan addressing the case in which WW is a Weyl group. We include in addition a succinct description of the irreducible decomposition of ϱW\varrho_W derived by Kottwitz when (W,S)(W,S) is classical, and prove that ϱW\varrho_{W} defines a Gelfand model if and only if (W,S)(W,S) has type AnA_n, H3H_3, or I2(m)I_2(m) with mm odd. We show finally that a conjecture of Kottwitz connecting the decomposition of ϱW\varrho_W to the left cells of WW holds in all non-crystallographic types, and observe that a weaker form of Kottwitz's conjecture holds in general. In giving these results, we carefully survey the construction and notable properties of the set \Uch(W) and its attached Fourier transform.Comment: 38 pages, 4 tables; v2, v3, v4: some corrections and additional reference

    Higher Laminations and Affine Buildings

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    We give a Thurston-like definition for laminations on higher Teichmuller spaces associated to a surface SS and a semi-simple group GG for G−SLmG-SL_m and PGLmPGL_m. The case G=SL2G=SL_2 or PGL2PGL_2 corresponds to the classical theory of laminations. Our construction involves positive configurations of points in the affine building. We show that these laminations are parameterized by the tropical points of the spaces \X_{G,S} and \A_{G,S} of Fock and Goncharov. Finally, we explain how these laminations give a compactification of higher Teichmuller spaces.Comment: 46 page

    Induced characters of the projective general linear group over a finite field

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    Using a general result of Lusztig, we find the decomposition into irreducibles of certain induced characters of the projective general linear group over a finite field of odd characteristic.Comment: 17 page

    Graded Hecke algebras for disconnected reductive groups

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    We introduce graded Hecke algebras H based on a (possibly disconnected) complex reductive group G and a cuspidal local system L on a unipotent orbit of a Levi subgroup M of G. These generalize the graded Hecke algebras defined and investigated by Lusztig for connected G. We develop the representation theory of the algebras H. obtaining complete and canonical parametrizations of the irreducible, the irreducible tempered and the discrete series representations. All the modules are constructed in terms of perverse sheaves and equivariant homology, relying on work of Lusztig. The parameters come directly from the data (G,M,L) and they are closely related to Langlands parameters. Our main motivation for considering these graded Hecke algebras is that the space of irreducible H-representations is canonically in bijection with a certain set of "logarithms" of enhanced L-parameters. Therefore we expect these algebras to play a role in the local Langlands program. We will make their relation with the local Langlands correspondence, which goes via affine Hecke algebras, precise in a sequel to this paper.Comment: Theorem 3.4 and Proposition 3.22 in version 1 were not entirely correct as stated. This is repaired in a new appendi
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