The Iwahori-Hecke algebra of the group <math> <mi>G</mi><mfenced> <mi>r</mi><mi>r</mi><mn>2</mn> </mfenced> </math> of order <math> <mn>2</mn><mi>r</mi> </math>

The Iwahori-Hecke algebra of the group G rr2 of order 2r

Arun Ram
Department of Mathematics and Statistics
University of Melbourne
Parkville, VIC 3010 Australia
aram@unimelb.edu.au
and

Department of Mathematics
University of Wisconsin, Madison
Madison, WI 53706 USA
ram@math.wisc.edu

Last updates: 28 May 2010

The Iwahori-Hecke algebra of the group G rr2 of order 2r

Let p,q * . The Iwahori-Hecke algebra of the dihedral group H r,r,2 = H r,r,2 pq is the algebra given by the generators T1 , T2 and relations T1 T2 T1 T2 r   factors = T2 T1 T2 T1 r   factors T12 = p- p -1 T1 +1, T22 = q- q -1 T2 +1. The last two relations guarantee that T1 and T2 are invertible. T1 -1 = T1 - p- p -1   and   T2 -1 = T2 - q- q -1 . If r is odd then p=q is forced since T1 T2 T1 T2 r-1   factors -1 T2 T1 T2 T1 T2 r-1   factors = T1 . The elements 1 T1 T2 T1 T2 k   factors T2 T1 T2 T1 k   factors T1 T2 T1 T2 r   factors | 1k<r form a basis of H r,r,2 . If p=q=1 then H r,r,2 =G rr2 is the group algebra of the dihedral group of order 2r.

Assume that p,q satisfy ?????. The irreducible representations of H r,r,2 pq are given as follows. The one dimensional representations ρ ++ and ρ -- are given by ρ ++ T1 =p,  and   ρ ++ T2 =q, and ρ -- T1 =- p -1   and   ρ -- T2 =- q -1 , and, if r is even, there are additional one dimensional representations ρ +- and ρ -+ given by ρ +- T1 =p,  and   ρ +- T2 =- q -1 , and ρ -+ T1 =- p -1   and   ρ -+ T2 =q. The two dimensional representations ρλ ,0<λ<r/2 are given by ρλ T2 = a 1+ad 1 d   and   ρλ T2 = -dξ 1+ad ξ ξ -1 -a ξ -1 where  ξ= e 2πi/r , a= q- q -1 ξ+ p- p -1 ξ- ξ -1 ,  and  d= q- q -1 ξ -1 + p- p -1 ξ -1 -ξ .

Proof.

Instead of repeating the proof of the theorem in the previous section and minding our p's and q's (SLAP! -NS) let us give a proof showing how the result can be derived.

The quadratic relations in ????? are equivalent to T1 -p T1 + p -1 =0  and   T2 -q T2 + q -1 =0, and these imply that any one dimensional representation χ: H r,r,2 must have χ T1 equal to p or p -1 and χ T2 equal to q or q -1 . If r is odd then T1 is conjugate to T2 and so χ T2 =χ T1 . This determines our one dimensional representations of H r,r,2 .

Let ρ: H r,r,2 M2 be an irreducible two dimensional representation of H r,r,2 . By the relation T1 -p T1 + p -1 =0 be the eigenvalues of ρ T1 are in the set p p -1 . If ρ T1 has two equal eigenvalues then it is a multiple of the identity. If v is an eigenvector of ρ T2 , and ρ T1 is a constant multiple of the identity then v is a submodule of ρ and this contradicts the irreducibility of ρ. So ρ T1 must have eigenvalues p and p -1 . Similarly ρ T2 must have eigenvalues q and q -1 .

By the defining relations, T1 T1 T2 m  factors = T1 T2 T1 m  factors = T1 T2 m  factors Ti , where i=1 if r is odd and i=2 if r is even. So T2 T1 T2 m = T1 T1 T2 m  factors T1 T2 m  factors = T1 T2 m  factors Ti T1 T2 m  factors = T1 T2 m  factors T1 T2 m  factors T1 = T2 T1 m T1 , and simiilarly one shows that T2 T1 T2 m = T1 T2 m T2 . So T1 T2 m is in the center of H r,r,2 .

By Schur's lemma, ρ T1 T2 m =cId,for some  c. Since ρ T1 has eigenvalues p and p -1 and ρ T2 has eigenvalues q and q -1 , det ρ T1 =det ρ T2 =-1 and so det ρ T1 T2 m = -1 2m =1. On the other hand, det ρ T1 T2 m = c2 and so c=±1. So ρ T1 T2 m =cId. Thus the eigenvalues of ρ T1 T2 are r th roots of unity. Since det ρ T1 T2 = -1 2 =1, we can write (possibly after some change of basis in the module ρ ) ρ T1 T2 = ξk 0 0 ξ -k where  ξ= e 2πi/r   and  k. If k=0 or (if r is even and) k=r/2 then ρ T1 T2 =±1 and ρ is not invertible. So without loss of generality we can assume that 0<k<r/2.

Suppose that ρ T2 = a b c d . The relation T 2 2 = q- q -1 T2 +1 implies that a+d=q- q -1 and ad-bc=1. So we can assume ρ T2 = a ad+1 1 d ,with  a+d=q- q -1 . Then ρ T1 =ρ T1 T2 T2 -1 =ρ T1 T2 ρ T2 -1 = ξk 0 0 ξ -k -d ad+1 1 -a = -d ξk 1+ad ξk ξ -k -a ξ -k . Now Tr ρ T1 =p- p -1 =-d ξk -a ξ -k ,  and  Tr ρ T2 =q- q -1 =a+d, and these equations determine a and d as given in the statement of the theorem.

References [PLACEHOLDER]

[BG] A. Braverman and D. Gaitsgory, Crystals via the affine Grassmanian, Duke Math. J. 107 no. 3, (2001), 561-575; arXiv:math/9909077v2, MR1828302 (2002e:20083)

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