Arun Ram
Department of Mathematics and Statistics
University of Melbourne
Parkville, VIC 3010 Australia
aram@unimelb.edu.au
Last update: 09 April 2012
Multisegments
Let
The elements of index the (isomorphism classes) of simple representations of the quiver.
Consider a sheet of graph paper with diagonals indexed by The content of a box on this sheet of graph paper is
Let
denote a sequence of boxes in a row which has length with the leftmost box of content and the rightmost box of content The set of segments is
The elements of index the (isomorphism classes) of indecomposable (nilpotent) representations of the quiver.
A multisegment is a (unordered) collection of segments, i.e. an elements of
For example
(the numbers in the boxes in the picture are the contents of the boxes).
A multisegment is aperiodic if it does not contain
Pictorially, a multisegment is aperiodic if it does not contain a box of height Let
In types and
The elements of index the isomorphism classes of nilpotent representations of the quiver.
The partial order
Consider an (infinite) sheet of graph paper which has its diagonals labeled consecutively by
The contentc(b) of a box b on this sheet of graph paper is
c(b)=
the diagonal number of the box b.
A segment is a row of boxes on a sheet of graph paper with diagonals indexed by ℤ.
Consider a graph paper with diagonals indexed by ℤ. A segment is a sequence of boxes
[i,j]=
in a row with the leftmost box of content i and the rightmost box of content j. A multisegment is a (unordered) collection of segments. For example
has λ([3,7])=2,λ([5,7])=1,λ([1,5])=1,λ([3,5])=1,
and
λ([i,j])=0
for all other segments [i,j] (the numbers in the boxes in the picture are the contents of the boxes). Alternatively a multisegment λ can be viewed as a function
λ:{segments}→ℤ≥0 where λ([i,j])=(# of rows [i,j] in λ).
The set of segments is ordered by inclusion. Define
λ(⊇[i,j])=∑[r,s]⊇[i,j]λ([r,s]). (MS 2)
Then
λ([i,j])=λ(⊇[i-1,j+1])-λ(⊇[i-1,j])-λ(⊇[i,j+1])+λ(⊇[i,j])
PICTURE
and so the multisegment λ can be specified by the numbers
λ(⊇[i,j]).
Note that
λ(⊇[i])=(# of boxes in λ in diagonal i).
Define a partial order on multisegments by
λ≥μ if λ(⊇[i,j])≥μ(⊇[i,j])
for all segments [i,j].
If
[b,c]⊆[a,d]
are segments define a degenerationR[b,c],[a,d]:{multisegments}→{multisegments}
by
R[b,c],[a,d]λ([a,d])=λ([a,d])-1,R[b,c],[a,d]λ([b,d])=λ([b,d])+1,R[b,c],[a,d]λ([a,c])=λ([a,c])+1,R[b,c],[a,d]λ([b,c])=λ([b,c])-1,R[b,c],[a,d]λ([i,j])=λ([i,j]), if
[i,j]≠[a,d],[a,c],[b,d],[b,c].
The degeneration
R[b,c],[a,d]λ
is elementary if
λ([i,j])=0
for all
[b,c]⊆[i,j]⊆[a,d]
except
[i,j]=[b,c],[a,c],[b,d]
or
[a,d].
Pictorially a degeneration takes
PICTURE→PICTURE
and
PICTURE→PICTURE for
c=b-1,
or, equivalently,
PICTURE→PICTURE.
Let A∞ be the quiver (I,Ω+) with
I=ℤ,Ω+={i→i+1|i∈ℤ}.
Fix an I-graded vector space
V=⨁i∈IVi,
and let
EV=⨁i→i+1Hom(Vi,Vi+1),GLV=∏i∈ℤGL(Vi), which acts on
EV, and
𝒩V={x∈EV|x is a nilpotent element of Hom(V,V)}.
The map
𝒩V→{multisegments}x↦λx given by
λ(⊇[i])=dim(Vi) and λ(⊇[i,j])=rank(λ:Vi→⋯→Vj)
provides a bijection
{multisegments λ|λ(⊇[i])=dim(Vi)}↔{GLV orbits in 𝒩V}.
Let λ and μ be multisegments and let 𝕆λ and 𝕆μ be the corresponding orbits in 𝒩V/GLV. Then the following are equivalent:
λ≥μ,
𝕆λ_⊇𝕆μ,
λ=Ri1⋯Rirμ for some sequence of elementary degenerations Ri1,...,Rir.
Proof.
(1)⇒(2):
PICTURE+εPICTURE≅PICTURE,
and so
𝕆PICTURE⊆𝕆PICTURE_.
(2)⇒(3):
If 𝕆μ⊆𝕆λ_ then
μ(⊇[i,j])=rank(μ:Vi→⋯→Vj)≤rank(λ:Vi→⋯→Vj)=λ(⊇[i,j]).
(3)⇒(1):
Assume
λ(⊇[i,j])≥μ(⊇[i,j])
for all segments [i,j]. Find (THIS STILL NEEDS DOING) a sequence Ri1⋯Rir of elementary degenerations which takes μ to λ, i.e.
Ri1⋯Rirμ=λ.
□
Hecke algebra representations
Let Hk˜ be the affine Hecke algebra at an lth root of unity so that ql=1 (all l=∞ if desired). For each
b∈B˜(∞)
let
b=∑j[sj,nj) and define the standard moduleM(b)=IndH˜νH˜k(ℂs),
where ν=(n1,...,nr) and k=n1+⋯+nr. The simple H˜k-modules are indexed by
b∈B(∞)
and are determined by the equations
[M(b)]=[L(b)]+∑b′>bb′∈B(∞)db′b[L(b′)],b∈B(∞),db′b∈ℤ≥0,
in the Grothendieck group of H˜k(q)-modules.
The Fock space representation of Uv𝔰𝔩^l
The crystal graph
Let
λ=[(λ+ρ)1(λ+ρ)2⋯(λ+ρ)n(μ+ρ)1(μ+ρ)2⋯(μ+ρ)n]=((λ+ρ)1(λ+ρ)2⋯(λ+ρ)nd1d2⋯dn]
be a multisegment and assume that it is ordered so that
(λ+ρ)i≥(λ+ρ)i+1,
(μ+ρ)i≤(μ+ρ)i+1
if
(λ+ρ)i=(λ+ρ)i+1.
These conditions are equivalent to saying that
The 𝔤𝔩(n)-weight λ is integrally dominant,
μ=w∘ν where ν is integrally dominant and w is longest in its coset
Wλ+ρwWμ+ρ.
Place
-1 above each
(λ+ρ)j=i,
+1 above each
(λ+ρ)j=i-1,
0 above each
(λ+ρ)j≠i,i-1.
Then, ignoring 0s, read the sequence of +1s, -1s left to right and successively cancel adjacent (-1,+1) pairs to get a sequence of the form
cogood
good
↓↓+1+1⋯+1⏟
conormal modes
-1-1⋯-1⏟
normal modes
The -1s in this sequence are the normal nodes and the +1s are the conormal nodes. The good node is the leftmost normal node and the cogood node is the rightmost conormal node.
Define
wt(λ)=∑i∈I-(
number of boxes of content i in λ)αi, and
εi(λ)=(number of normal nodes),φi(λ)=( number of conormal nodes ),e˜iλ=(
same as λ but with the good node
(λ+ρ)j=i
changed to i-1),f˜iλ=(
same as λ but with the cogood node
(λ+ρ)j=i-1
changed to i),
for each i∈I.
If this algorithm is being executed where I=ℤ/lℤ then take
(λ+ρ)j=l, when i=0 and (λ+ρ)j≡0modl, and
(λ+ρ)j=0, when i=1 and (λ+ρ)j≡0modl.
In type Al-1(1),B(∞) is the connected component of ∅ in the crystal graph B˜(∞).
B(∞) is the crystal graph of Uv-𝔤.
The crystals B(Λ)
Type Al-1: Let
λ=∑i=1lλiϵi=∑i∈Iγiωi∈P+,
and identify λ with the partition which has λi boxes in row i. Let
B(λ)={column strict tableaux of shape λ}
and define an imbedding
B(λ)→B(∞)P↦[11⋯122⋯2⋯nn⋯ni1i2⋯iλ1iλ1+1⋯iλ1+λ2⋯⋯ik]
where the entries i1i2⋯ik are the entries of P read in Arabic reading order.
The tensor product representation
The l-dimensional simple Uq𝔰𝔩l-module of highest weight ω1 is given by
L(ω1)=ℂ-span {v0,...,vl-1}
with Uq𝔰𝔩l-action
eivj={vi-1,
if j=i,0,
if j≠i,}fivj={vi,
if j=i-1,0,
if j≠i-1,}kivj={qvi-1,
if j=i,q-1vi,
if j=i-1,vj,
if j≠i,i-1.}
Then
L(ω1)⊗k=ℂ-span
{vj1⊗⋯⊗vjk|1≤j1,j2,...,jk≤l}.
If
v=vj1⊗⋯⊗vjk
place
+1 over each vi-1 in v,
-1 over each vi in v,
0 over each vj,j≠i,i-1.
Then the Uq𝔰𝔩l-action on L(ω1)⊗k is given by
ei(v)=∑v-q-(sum of ±1s before v/v-)v-,fi(v)=∑v+q-(sum of ±1s after v+/v)v+,ki(v)=q(sum of ±1s for v)v,
where the first sum is over all v- which are obtained from v by changing a vi to vi-1 and the second sum is over all v+ which are obtained from v by changing a vi-1 to vi.
The Fock space
Let μ∈𝔥* for 𝔤𝔩n. Define
ℱμ=ℂ-span
{multisegments λ=λ/μ}.
Define an action of Uv𝔰𝔩^l on ℱμ by
eλ=∑c(λ/λ-)≡iq(sum of ±1s before λ/λ-)λ-,fiλ=∑c(λ+/λ)≡iq(sum of ±1s after λ+/λ)λ+,kiλ=q(sum of the ±1 sequence for λ)λ,Dλ=q(# of boxes of content 0 in λ)λ.
These formulas make ℱμ into a Uv𝔰𝔩^l-module.
If
Lμ=ℤ[q,q-1]-span
{multisegments λ=λ/μ}
so that the multisegments form a
ℤ[q,q-1]
basis of Lμ then
e˜i[λ]=[e˜iλ]modqLμ and f˜i[λ]=[f˜iλ]modqLμ.
Proof.
The permutations of the sequence
+1,+1,...,+1,-1,-1,...,-1
are indexed by the elements of
St/Sk×St-k
where t is the number of nodes after (-1,+1) pairing. The group
(ℤ/2ℤ)p
acts on the (-1,+1) pairs by changing a pair (-1,+1) to (+1,-1). For each 1≤k≤r define
uk=∑σ∈St/Sk×St-k∑τ∈(ℤ/2ℤ)tql(σ)(-1)l(τ)(στλ[k]).
Then
uk=λ[k]modqLμ and eiuk=[k]uk-1.
The first statement is clear. To obtain the second statement
eiuk=∑σ∈St/Sk×St-k∑τ∈(ℤ/2ℤ)tql(σ)(-1)l(τ)(eiστλ[k])=∑ei changes a pair
∑σ∈St/Sk×St-k∑τ∈(ℤ/2ℤ)tql(σ)(-1)l(τ)(στλ[k])-+∑ei changes a node
∑σ∈St/Sk×St-k∑τ∈(ℤ/2ℤ)tql(σ)(-1)l(τ)(στλ[k])-=0+∑τ∈(ℤ/2ℤ)t∑σ∈St/Sk×St-k∑ei changes a node
ql(σ)(-1)l(τ)(στλ[k])-=∑τ∈(ℤ/2ℤ)t[k]∑σ∈St/Sk×St-kql(σ)(-1)l(τ)(στλ[k])-
□
A Schur-Weyl duality connection to affine Hecke algebras
A multisegment is a collection of rows of boxes (segments) placed on graph paper. We can label this multisegment by a pair of weights
λ=λ1ε1+⋯+λn+1εn+1
and
μ=μ1ε1+⋯+μn+1εn+1
by setting
(λ+ρ)i=
content of the last box in row i, and
(μ+ρ)i=(content of the last box in row i)-1.
For example
corresponds to λ+ρ=77755
and
μ+ρ=22402 (MS 3)
(the numbers in the boxes in the picture are the contents of the boxes). The construction forces the condition
(λ+ρ)i-(μ+ρ)i∈ℤ≥0,
and since we want to consider unordered collections of boxes it is natural to take the following pseudo-lexicographic ordering on the segments,
(λ+ρ)i≥(λ+ρ)i+1,
(μ+ρ)i≤(μ+ρ)i+1
if
(λ+ρ)i=(λ+ρ)i+1,
when we denote the multisegment λ/μ by a pair of weights λ,μ. In terms of weights the conditions (a), (b) and (c) can be restated as (note that in this case both λ and μ are integral)
λ-μ is a weight of V⊗k, where k is the number of boxes in λ/μ,
λ is integrally dominant,
μ=w∘ν with ν integrally dominant and w maximal length in the coset
Wλ+ρwWν+ρ.
Let λ/μ be a multisegment with k boxes and number the boxes of λ/μ from left to right (like a book). Define
H˜λ/μ=
subalgebra of
H˜k
generated by
{Xλ,Tj|λ∈L,boxj
is not at the end of its row },
so that H˜λ/μ is the "parabolic" subalgebra of H˜k corresponding to the multisegment λ/μ. Define a one-dimensional H˜λ/μ module
ℂλ/μ=ℂvλ/μ
by setting
Xεivλ/μ=q2c(boxi)vλ/μ, and Tjvλ/μ=qvλ/μ, (MS 4)
for 1≤i≤k and j such that boxj is not at the end of its row.
Let 𝔤 be of type An and let Fλ be the functor
HomUh𝔤(M(λ),⋅⊗V⊗k)
where V=L(ω1). The standard module for the affine Hecke algebra H˜k is
ℳλ/μ=Fλ(M(μ)) (MS 5)
as defined in (4.1). It follows from the above discussion that these modules are naturally indexed by multisegments λ/μ. The following proposition shows that this standard module coincides with the usual standard module for the affine Hecke algebra as considered by Zelevinsky [Ze2] (see also [Ar], [CG] and [KL]).
Let λ/μ be a multisegment determined by a pair of weights (λ,μ) with λ integrally dominant. Let ℂλ/μ be the one dimensional representation of the parabolic subalgebra H˜λ/μ of the affine Hecke algebra H˜k defined in (???). Then
ℳλ/μ≅IndH˜λ/μH˜k(ℂλ/μ).
Proof.
To remove the constants that come from the difference between 𝔤𝔩n and 𝔰𝔩n the affine braid group action in Theorem 6.17a should be normalized so that
Φk(Xε1)=q2|μ|/(n+1)Rˇ02
and
Φk(Ti)=q1(n+1)Rˇi.
By Proposition 4.3a,
cMλ/μ≅(V⊗k)λ-μ
as a vector space. Let
{v1,v2,...,vn+1}
be the standard basis of
V=L(ω1)
with
wt(vi)=εi.
If we let the symmetric group Sk act on V⊗k by permuting the tensor factors then
(V⊗k)λ-μ=span-{π⋅v⊗(λ-μ)|π∈Sk}=span-{π⋅v⊗(λ-μ)|π∈Sk/Sλ-μ},
where
v⊗(λ-μ)=v1⊗⋯⊗v1⏟λ1-μ1⊗⋯⊗vn⊗⋯⊗vn⏟λn-μn and Sλ-μ=Sλ1-μ1×⋯×Sλn-μn
is the parabolic subgroup of Sk which stabilizes the vector
v⊗(λ-μ)∈V⊗k.
This shows that, as vector spaces,
ℳλ/μ≅IndH˜λ/μH˜k(ℂλ/μ)=span-{Tπ⊗vλ/μ|π∈Sk/Sλ-μ} (MS 6)
are isomorphic.
For notational purposes let
bλ/μ=vμ+⊗v⊗(λ-μ)=vμ+⊗vi1⊗⋯⊗vik
and let b_λ/μ be the image of bλ/μ in
(M⊗V⊗k)[λ].
Since λ is integrally dominant and b_λ/μ has weight λ it must be a highest weight vector. We will show that Xεl acts on b_λ/μ by the constant qc(boxl), where c(boxl) is the content of the lth box of the multisegment λ/μ (read left to right and top to bottom like a book).
Consider the projections
prl:M(μ)⊗V⊗k→(M(μ)⊗V⊗l)[λ(l)]⊗V⊗(k-l) where λ(l)=μ+∑j≤lwt(vil)
and pri acts as the identity on the last k-i factors of
M(μ)⊗V⊗k.
Then
b_λ/μ=prkprk-1⋯pr1bλ/μ,
and for each 1≤l≤k, (the first l components of)
prl-1⋯pr1(bλ/μ)
form a highest weight vector of weight λ(l) in
M⊗V⊗l.
It is the "highest" highest weight vector of
((M(μ)⊗V⊗(l-1))[λ(l-1)]⊗V)[λ(l)] (MS 7)
with respect to the ordering in Lemma 4.2 and thus it is deepest in the filtration constructed there. Note that the quantum Casimir element acts on the space in (6.29) as the constant
q⟨λ(l),λ(l)+2ρ⟩
times a unipotent transformation, and the unipotent transformation must preserve the filtration coming from Lemma 4.2. Since
prl(bλ/μ)
is the highest weight vector of the smallest submodule of this filtration (which is isomorphic to a Verma module by Lemma 4.2b) it is an eigenvector for the action of the quantum Casimir. Thus, by (2.11) and (2.13), Xεl acts on
prl(bλ/μ)
by the constant
q⟨λ(l),⟨(l)+2ρ⟩-⟨λ(l-1),λ(l-1)+2ρ⟩-⟨ω1,ω1+2ρ⟩=q2c(boxl),
(see [LR]). Since Xεl commutes with prj for j>l this also specifies the action of Xεl on
b_λ/μ=prl(bλ/μ).
The explicit R-matrix
RˇVV:V⊗V→V⊗V
for this case (𝔤 of type A and V=L(ω1)) is well known (see, for example, the proof of [LR, Prop. 4.4]) and given by
(vi⊗vj)q1(n+1)RˇVV={vj⊗vi,
if i (LESS THAN?) j,(q-q-1)vi⊗vj+vj⊗vi,
if i (GREATER THAN?) j,qvi⊗vj,
if i=j.}
Since Ti acts by RˇVV on the ith and (i+1)st tensor factors of V⊗k and commutes with the projection prλ it follows that
Tj(b_λ/μ)=qb_λ/μ,
if boxj is not a box at the end of a row of λ/μ. This analysis of the action of H˜λ/μ on b_λ/μ shows that there is an H˜k-homomorphism
IndH˜λ/μH˜k(ℂvλ/μ)→ℳλ/μvλ/μ↦b_λ/μ.
This map is surjective since ℳλ/μ is generated by b_λ/μ (the ℬk action on vλ-μ generates all of
(V⊗k)λ-μ).
Finally, (6.28) guarantees that it is an isomorphism.
□
In the same way that each weight μ∈𝔥* has a normal formμ=w∘μ˜, with μ˜ integrally dominant, andw maximal length in the coset wWμ˜+ρ,
every multisegment λ/μ has a normal formλ/μ=ν/(w∘ν˜), with ν+ρ
the sequence of contents of boxes of
λ/μ,ν˜=ν-11...1, and
w maximal length in
Wν+ρwWν+ρ.
The element w in the normal form
ν/(w∘ν˜)
of λ/μ can be constructed combinatorially by the following scheme. We number (order) the boxes of λ/μ in two different ways.
First ordering: To each box b of λ/μ associate the following triple
(
content of the box to the left of b,-(content of b),-(row number of b))
where, if a box is the leftmost box in a row "the box to its left" is the rightmost box in the same row. The lexicographic ordering on these triples induces an ordering on the boxes of λ/μ.
Second ordering: To each box b of λ/μ associate the following pair
(
content of b,-(the number of box b in the first ordering)).
The lexicographic ordering of these pairs induces a second ordering on the boxes of λ/μ.
If v is the permutation defined by these two numberings of the boxes then w=w0vw0. For example, for the multisegment λ/μ displayed in (6.24) the numberings of the boxes are given by
first ordering of boxes and second ordering of boxes
and the normal form of λ/μ is
ν=777666555554444333321,ν˜=666555444443333222210, and
w=w0vw0 where
v=123456789101112131415161718192021151212014265431910987131211181716.
Let 𝔤 be of type An and V=L(ω1) and let
ℒλ/μ=Fλ(L(μ)), (MS 8)
as defined in (4.1). It is known (a consequence of Proposition 6.27 and Proposition 4.3c) that ℒλ/μ is always a simple H˜k-module or 0. Furthermore, all simple H˜k modules are obtained by this construction. See [Su] for proofs of these statements. The following theorem is a reformulation of Proposition 4.12 in terms of the combinatorics of our present setting.
Let λ/μ and ρ/τ be multisegments with k boxes (with μ and τ assumed to be integral) and let
λ/μ=ν/(w∘ν˜) and ρ/τ=γ/(v∘γ˜)
be their normal forms. Then the multiplicities of ℒρ/τ in a Jantzen filtration of ℳλ/μ are given by
∑j≥0[(ℳλ/μ)(j)(ℳλ/μ)(j+1):ℒρ/τ]v12(l(y)-l(w)+j)={Pwv,
if ν=γ,0,
if ν≠γ,}
where Pwv(v) is the Kazhdan-Lusztig polynomial for the symmetric group Sk.
Theorem 6.31 says that every decomposition number for affine Hecke algebra representations is a Kazhdan-Lusztig polynomial. The following is a converse statement which says that every Kazhdan-Lusztig polynomial for the symmetric group is a decomposition number for affine Hecke algebra representations. This statement is interesting in that Polo [Po] has shown that every polynomial in
1+vℤ≥0[v]
is a Kazhdan-Lusztig polynomial for some choice of n and permutations v,w∈Sn. Thus, the following proposition also shows that every polynomial arises as a generalized decomposition number for an appropriate pair of affine Hecke algebra modules.
Let
λ=rr...r=(rr)
and
μ=00...0=(0r).
Then, for each pair of permutations v,w∈Sr, the Kazhdan-Lusztig polynomial Pvw(v) for the symmetric group Sr is equal to
Pvw(v)=∑j≥0[(ℳλ/w∘μ)(j)(ℳλ/w∘μ)(j+1):ℒλ/v∘μ]v12(l(y)-l(w)+j).
Proof.
Since μ+ρ and λ+ρ are both regular,
Wλ+ρ=Wμ+ρ=1
and the standard and irreducible modules
ℒλ/(w∘μ)
and
ℳλ/(v∘μ)
ranging over all v,w∈Sk. Thus, this statement is a corollary of Proposition 4.12.
□
References
[GL]
S. Gaussent, P. Littelmann,
LS galleries, the path model, and MV cycles,
Duke Math. J. 127 (2005), no. 1, 35-88.
[GR]
S. Griffeth and A. Ram,
Affine Hecke algebras and the Schubert calculus,
European J. Combin. 25 (2004), no. 8, 1263-1283.
[Ka]
J. Kamnitzer,
Mirkovic-Vilonen cycles and polytopes,
math.AG/050136.5.
[KM]
M. Kapovich and J.J. Millson,
A path model for geodesics in Euclidean buildings and its applications to representation thoery,
math.RT/0411182.
[LP]
C. Lenart and A. Postnikov,
Affine Weyl groups in K-theory and representation theory,
math.RT/0309207.
[PR]
H. Pittie and A. Ram,
A Pieri-Chevalley formula in the K-theory of a G/B-bundle,
Electronic Research Announcements 5 (1999), 102-107, and A Pieri-Chevalley formula for K(G/B), math.RT/0401332.
[1]
A. Ram,
Affine Hecke algebras and generalized standard Young tableaux,
J. Algebra, 230 (2003), 367-415.
[2]
A. Ram,
Skew shape representations are irreducible,
in Combinatorial and Geometric representation theory,
S.-J. Kang and K.-H. Lee eds.,
Contemp. Math. 325 Amer. Math. Soc. 2003,
161-189,
math.RT/0401326.
[3]
RR A. Ram and J. Ramagge,
Affine Hecke algebras, cyclotomic Hecke algebras and Clifford theory,
in A tribute to C.S. Seshadri: Perspectives in Geometry and Representation theory,
V. Lakshimibai et al eds.,
Hindustan Book Agency,
New Delhi (2003),
428-466,
math.RT/0401322.
[Sc]
C. Schwer,
Ph.D. Thesis,
University of Wuppertal,
2006.