The symmetric group and Brauer algebras

The symmetric group and Brauer algebras

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: 20 June 2010

The symmetric group Sk and the Brauer algebra

If λ GL^ n then L 𝔤𝔩 n λ V μ/λ= L 𝔤𝔩 n μ as   𝔤𝔩 n -modules, where the sum is over μ 𝔤𝔩 ^ n that are obtained from λ by adding a box. The Young lattice is the graph S^ given by setting vertices on level  k: S^ k = partitions  λ  with  k  boxes ,   and   a labeled edge  λ c λ/μ μ,λ S^ k ,μ S^ k+1 if  μ  is obtained from  λ  by adding a box. It encodes the decompositions in (????).

Define elements m1 ,, mk Sk by m1 =0,  and   mi = l=1 i-1 s li ,for  i>1. Then

  1. mi mj = mj mi ,  for  1i,jn.
  2. The eigenvalues of the elements mi are given by the diagram S^ k=0: k=1: k=2: k=3: k=4:
    in the sense that if S^ k   is the set of vertices on level  k  and   S^ kλ = paths  p= p 1 p 2 p k =λ   to  λ  in   S^ ,  for  λ S^ k , then S^ k   is an index set for the simple   Sk   modules   Skλ   and   Skλ   has basis   vp | p S^ kλ   with   mi vp =c p i vp , where p i = p i / p i-1 is the box added at step i in p and c b denotes the content of the box b.
  3. κ= mk + m k-1 ++ m2 is a central element of Sk and κ  acts on   Skλ   by the constant   bλ c b .

Proof.

The tensor product rule for GL n is L 𝔤𝔩 n μ V λ/μ= L 𝔤𝔩 n μ , where the sum is over all partitions λ such that l λ n,λμ and λ differs from μ by a single box. Since the Sk action and the GL n action commute on V k it follows that as   U 𝔤𝔩 n Sk   bimodules, V k λk,l λ n L 𝔤𝔩 n λ Skλ , where Skλ are some Sk -modules. Comparing the L 𝔤𝔩 n λ components on each side of λ L 𝔤𝔩 n λ Skλ V k = V k-1 V μ L 𝔤𝔩 n μ S k-1 μ V μ λ/μ= L 𝔤𝔩 n λ S k-1 μ λ L 𝔤𝔩 n λ λ/μ S k-1 μ gives Skλ λ/μ= S k-1 μ .

Using the basis v i1 v ik | 1 i1 ,, ik n of V k , the direct computation κ v i1 v in = l=1 k v i1 i,j=1 n E ij E jl v jl v ik + 1l<mk i,j=1 n v i1 E ji vl E ij v im v ik + v i1 E ij v il E ji v im v ik = kn+2 1l<mk s lm v i1 v ik = kn+2 zk v i1 v ik

Shows that κ=kn+2 1l<mk s lm ,  as operators on   V k . Since κ is a central element of U 𝔤𝔩 n and V k λk,l λ n L λ Skλ   as   U 𝔤𝔩 n Sk   bimodules, it follows from (???) that zk = 1l<mk s lm   acts on   Skλ   by   bλ c b . Thus, in (???), mk = 1l<k s lk = zk - z k-1   acts on   S k-1 μ   by the constant  c λ/μ . Since the values c λ/μ are distinct for the distinct summands in (???), S k-1 μ = v Skλ | mk v=c λ/μ v , the c λ/μ , eigenspace of mk in Skλ . Iterating the decomposition (???) gives Skλ = p S^ kλ S1 , and, since S1 is one dimensional, this determines, up to constants, a unique basis of   Skλ vp | p S^ kλ   such that   mi vp =c p i vp .

In Sk , si mi si + si = m i+1 , and so si mi +1= m i+1 si   and   si mj = mj si ,  for  ji,i+1. Write si pq to denote the pq entry of the matrix determined by the action of si on Skλ with respect to the basis in (???). Then si pp mi pp +1= m i+1 pp si pp   giving   si pp = 1 mi pp - mi pp . Then, COPY FROM NOTES .....

As U 𝔤𝔩 n Sk bimodules, V k λk,l λ n L 𝔤𝔩 n λ Skλ , where Skλ are simple Sk modules.

For λ S^ k and μ S^ k-1 , Res S k-1 Sk Skλ λ/ν= S k-1 ν   and   Ind S k-1 Sk S k-1 μ μ/μ= Skν , where the first sum is over all partitions ν that are obtained from λ by removing a box, and the second sum is over all partitions ν which are obtained from μ by adding a box.

Let Sk pq be the pq (simultaneous) eigenspace of Sk with respect to the action of m1 ,, mk by left and right multiplication, Sk pq = a Sk | for  1i,jk, mi a=c p i a  and  a mj =c q j mj . Then dim Sk pq =1 and there exist matrix units e pq λ ,λ S^ k ,p,q S^ kλ such that Sk pq = e pq   and   e pq λ e rs μ = δ λμ δ qr e ps λ .

Let Φ: Sk End V k and Ψ:U 𝔤𝔩 n End V k be the representations of Sk and 𝔤𝔩 n corresponding to their actions on V k . Then End GL n V k =Φ Sk   and   End Sk V k =Ψ U 𝔤𝔩 n , and kerΦ= w S n+1 det w w , the ideal of Sk generated by the alternating sum of the permutations in the subgroup Sn kerΦ=0  if  nk .

The tower B^

If λ O^ n then L O n λ V μ/λ=  or  λ/μ= L On μ ,  as   O n -modules, where the sum is over μ O^ n that are obtained frm λ by adding or removing a box. Build a graph B^ n which encodes the O n module decomposition of V k ,k 0 , by setting vertices on level  k: B^ k n = λ O^ n | k- λ 2 0 , and an edge  λμ,  if  μ B^ k+1 n   is obtained from  λ B^ k n   by adding or removing a box.

Define elements m1 ,, mk Bk n by m1 =0,  and   mi = k n-1 4 + l=1 i-1 s li - e li ,for  i>1. Then

  1. mi mj = mj mi for 1i,jn.
  2. The eigenvalues of the elements mi are given by the diagram
    k=0: k=1: k=2: k=3: k=4:
    in the sense that if B^ k   is the set of vertices on level  k and B^ kλ = paths  p= p 1 p 2 p k   to  λ  in   B^ ,  for  λ B^ k , then B^ k   is an index set for the simple   Bk   modules   Bkλ , and Bkλ   has a basis   vp | p B^ kλ   with   mi vp =c p i vp , where ??????? c p i / p i-1 + n-1 2 , if p i / p i-1 =, -c p i-1 / p i - n-1 2 , if p i-1 / p i =,
  3. κ= mk + m k-1 ++ m2   is a central element of   Bk n and κ  acts on   Bkλ   by the constant   n-1 2 + bλ c b

Proof.

Let κ be the Casimir element of 𝔰𝔬 n as in (???). Then κ v i1 v ik = - 1 4 l=1 k v i1 i,j=1 n E ij - E ji 2 v il v ik - 1 4 2 1l<mk i,j=1 n v i1 E ij - E ji v il E ij - E ji v im v ik = - 1 4 l=1 k 1-n-n+1 - 1 4 2.2 1l<mk e lm - s lm v i1 v ik since E ij - E ji 2 = E ji 2 - E ij E ji - E ji E ij + E ji 2   and   E ji 2 =0 unless i=j= il . Thus, as operators on V k , κ=- 1 4 k 2-2n + 1l<mk s lm - e lm = k n-1 2 + 1l<mk s lm - e lm . Since κ is a central element of U 𝔤𝔩 n and V k λk,l λ n L λ Bkλ   as   U 𝔰𝔬 n Bk n   bimodules, it follows from (???) that k n-1 2 + 1l<mk s lm - e lm   acts on   Bkλ   by   n-1 λ + bλ c b . The last statement follows since m1 ++ mk = k n-1 2 + 1l<mk s lm - e lm , for every k >0 .

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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