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Introduction. Aquestionofimportance,inrepresentationtheoryofgroups,istheconstructionofprimitiveidempotentsinagroupalgebra.Forthesymmetricgroup,aftertheearlyconstructionbyA.Young(see[17],[9]fordetails),severalcompletesetsofprimitiveidempotents(i.e.generati

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BANACH CENTER PUBLICATIONS, VOLUME 36 INSTITUTE OF MATHEMATICS POLISH ACADEMY OF SCIENCES

WARSZAWA 1996

INTERTWINING SPACES ASSOCIATED WITH q-ANALOGUES OF THE YOUNG SYMMETRIZERS

IN THE HECKE ALGEBRA

G ´ E R A R D D U C H A M P L.I.R., Universit´ e de Rouen,

Place E. Blondel, B.P. 118, 76134 Mont-Saint-Aignan Cedex, France

S U N G S O O N K I M L.I.T.P., Universit´ e Paris 7,

2 place Jussieu, 75251 Paris Cedex 05, France

Abstract. Let H be the Hecke algebra of the symmetric group. With each subset S ⊂ [1, n − 1], we associate two idempotents S and ∇ S which are q-deformations of the symmetrizer and antisymmetrizer relative to the Young subgroup S I

S

generated by the simple transpositions {(i, i + 1)} i∈S . We give here explicit bases for the intertwining space S

1

H∇ S

2

, indexed by the double classes S I

S1

\ S n / S I

S2

. We also compute bases and characters of the right ideals

I (I, J ) = S

1

H∇ S

2

H.

esum´ e. Soit H, l’alg` ebre de Hecke du groupe sym´ etrique. ` A chaque sous ensemble S ⊂ [1, n − 1], on associe deux idempotents S et ∇ S qui sont les q-d´ eformations des sym´ etriseur et antisym´ etriseur du sous groupe de Young S I

S

engendr´ e par les transpositions simples {(i, i + 1)} i∈S . Nous donnons ici des bases explicites pour le sous espace d’entrelacement S

1

H∇ S

2

, index´ ees par les doubles classes S I

S1

\ S n / S I

S2

. Nous calculons ´ egalement des bases et les caract` eres des id´ eaux

I (I, J ) = S

1

H∇ S

2

H.

Introduction. A question of importance, in representation theory of groups, is the construction of primitive idempotents in a group algebra. For the symmetric group, after the early construction by A. Young (see [17], [9] for details), several complete sets of primitive idempotents (i.e. generating irreducible ideals) have been proposed ([10], [14], [15] and [3], [6], [16] for the Hecke algebra).

1991 Mathematics Subject Classification: 20C30, 05E10.

The paper is in final form and no version of it will be published elsewhere.

[61]

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The original idea of Young (see e.g. [5], [9]) for computing a primitive idempotent in the algebra of the symmetric group consists in starting from a tableau without repetition

5 7

2 4

1 3 6

and deriving two idempotents, the row symmetrizer P (i.e. the sum of the permutations that preserve each row, in the picture S {1,3,6} × S {2,4} × S {5,7} ) and the column anti- symmetrizer N (i.e. the alternating sum of the permutations that preserve each column, in the picture S {1,2,5} × S {3,4,7} × S {6} ). Now, P N is (up to a scalar) an idempotent and the associated representation is irreducible, of index equal to the shape of the tableau.

The idempotence of P N is due to two facts, the first being that P.C[S n ].N is one dimensional and the second being that there is a natural isomorphism

P.C[S n ].N ∼ = Hom S

n

(N.S n , P.S n )

Let H be the Hecke algebra of the symmetric group with basis (T w ) w∈S

n

. The pre- ceding construction does not give in general idempotents in this algebra (even in the simplest case of a tableau of shape (1,2)). However, for a single row (or column), we get the following q-analogues of Young symmetrizers and antisymmetrizers

= X

w∈S

n

T w and ∇ = X

w∈S

n

(−q) l

max

−l(w) T w

with l max = n(n−1) 2 and l(w) being the length of the permutation w.

We can get also, with the same formulas, analogues of the Young row (resp. column) symmetrizers providing that the filling of the tableau is done with consecutive numbers in the rows (resp. columns). This explains why Young’s construction cannot be adapted trivially. The elements so obtained, denoted by ω

I

and ∇ ω

I

, are particular cases of the µ and ∇ µ , µ ∈ S n constructed elsewhere using solutions of the Yang-Baxter equation [4].

A complete set of primitive idempotents for the generic Hecke algebra have been de- fined (see [3], [4], [6]) with q-analogues of Young symmetrizers associated with partitions.

The idempotence of these elements is based (as for the symmetric group) on the combinatorial fact that, for I and J conjugate, the spaces ω

I

H∇ ω

J

and ∇ ω

J

H ω

I

are both one-dimensional.

The preceding property still holds when I and J are no longer partitions but com- positions associated with conjugate partitions. (This fact is characteristic free and inde- pendent of the choice of q.) Then, when the Hecke algebra is semi-simple, we can derive primitive idempotents of the form ω

I

h 0 ∇ ω

J

h 00 (see Corollary 3 below).

Our main concern here is the combinatorial structure of the spaces ω

I

H∇ ω

J

and of the right ideals

I(I, J ) = w

I

H∇ w

J

H,

i.e. the sum of the ideals w

I

h∇ w

J

H for h ∈ H (I, J are arbitrary compositions). A motivation also to the study of these more general spaces is the exploration of alternative computations for elements of Kazdhan-Lusztig basis as it can be easily checked that the elements ∇ ω

I

and ω

I

belong to invariant bases.

The paper is organized as follows. In the first section, we give the classical isomorphism

e.H.f ∼ = Hom H (f.H, e.H).

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Dimensions and bases of the intertwining space ω

I

.H.∇ ω

J

are then given. These bases are indexed by well-known combinatorial objects, namely matrices with entries in {0, 1}

and prescribed row (and column) sums.

The second part is devoted to the study of the structure of I(I, J ) (isotypic decom- position, bases and characters).

Acknowledgement. The authors are grateful to the referee for many useful remarks and corrections.

I. Intertwining spaces.

I.1. Intertwining two right direct summand ideals. Let H be a k-algebra (k is a ring) and U, V two right H-modules. In classical representation theory [2] Hom H (U, V ) is called the intertwining space between U and V . In case U, V are principal (right) ideals of H generated by idempotents (i.e. factors of decompositions H = I ⊕ J where I and J are ideals) the space Hom H (U, V ) has a concrete realization within H.

Proposition 1. Let e, f be two idempotents of H. Then the mapping ψ : eHf −→ Hom H (f H, eH)

defined by

ψ(ehf ) : f x −→ ehf x is an isomorphism.

P r o o f. It is obvious that ψ(ehf ) ∈ Hom H (f H, eH). Now, for θ ∈ Hom H (f H, eH) we have θ(f ) ∈ eH, but θ(f ) = θ(f 2 ) = θ(f )f ∈ eHf . The reader may then easily verify that

φ : Hom H (f H, eH) −→ eHf defined by φ(θ) = θ(f ) is the inverse isomorphism.

I.2. Background for symmetrizers in the Hecke algebra. Let us begin with some stan- dard facts about combinatorics of partitions.

Let I = (i 1 , i 1 , · · · , i k ) be a vector with (strictly) positive integral entries. This object is called a composition of |I| = P

1≤r≤k i r whereas the entries (i r ) are called the parts of I. The set

CS(I) = {i 1 , i 1 + i 2 , · · · , |I|} = n X

1≤r≤s

i r

o

1≤s≤k

is the set of cumulated sums of I. A decreasing composition J is called a partition of |J | and we write J ` |J |. Partitions can be represented by plane diagrams of boxes, called Ferrers’ diagrams. Such a diagram can be transposed (i.e. transformed by the orthogonal symmetry with axis x = y), the result being the diagram of the conjugate partition I e.

For example

Partition 322 331, conjugate of 322

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Now, to each composition, there corresponds a unique partition I 0 obtained by reordering the parts and we will say that two compositions I, J are conjugate iff I 0 = J 0 e (see [1]).

We will also need some well known results about the Hecke algebra of the symmetric group (which is a deformation of the group algebra).

Let k be a ring, q ∈ k, n ∈ N . The Hecke algebra H k n,q is the associative k-algebra with unit presented with generators (T i ) 1≤i<n and relations

T i T j = T j T i , |i − j| ≥ 2 (T i − 1)(T i + q) = 0, 1 ≤ i < n T i T i+1 T i = T i+1 T i T i+1 , 1 ≤ i < n − 1.

As a consequence of Murphy and Diper-James papers [15], [16], [3] it turns out that, if q.[n]! q is invertible in k ([r] q := 1 + q + · · · q r−1 and [n]! q = [1] q .[2] q . · · · [n] q ), then H k n,q is a direct product of full matrix algebras.

H k n,q ∼ = Y

λ`n

M(n λ , k) (I.1)

n λ being the dimension of the irreducible representation associated with the partition λ of the symmetric group (the numbers n λ can be computed directly by the “hook formula”

[5]).

If k is a field, (I.1) implies that H k n,q is semi-simple and the decomposition (I.1) is unique. Each component M(n λ , k) is called a block of H k n,q , its neutral element is a minimal central idempotent that we will denote by e λ and call the central idempotent of shape λ. This idempotent splits into indecomposables ones that are primitive idempotents of shape λ. We here briefly indicate how to construct an exhaustive (this means at least one for each shape) family of them.

Let I = (i 1 , i 2 , · · · i k ) be a composition of n. With I we associate a decomposition [1, n] = I 1 ] I 2 ] · · · ] I k

where I s is the interval [1 + i 1 + · · · + i s−1 , i 1 + i 2 + · · · i s ].

The subgroup

S I = {σ ∈ S n | ∀s ≤ k σ(I s ) = I s }

is also the subgroup generated by the elementary transpositions σ i = (i, i + 1) with i 6∈ CS(I). This subgroup is called the Young subgroup associated with I. S I is naturally isomorphic (by restrictions) to

S i

1

× S i

2

· · · × S i

k

(I.2)

and, in particular, its cardinality is I! := i 1 !i 2 ! · · · i k !. There is a unique longest element ω I in S I which acts by reversion in every interval I s . More precisely, with 0 ≤ h ≤ i s − 1

ω I (1 + i 1 + · · · i s−1 + h) = i 1 + i 2 · · · + i s − h.

Define elements

I := X

µ∈S

I

T µ ; ∇ I := X

µ∈S

I

(−q) l(ω

I

)−l(µ) T µ = X

µ∈S

I

(−q) l(ω

I

µ) T µ

In the spirit of [5], they will be called the symmetrizer (resp. antisymmetrizer) relative

to S I . These elements act as scalars on the elementary generators of S I and therefore

define idempotents (see [4]).

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Proposition 2. For i 6∈ CS(I) we have i) T i I = I T i = q I

ii) T i ∇ I = ∇ I T i = −∇ I

iii) If q, I! ∈ k then q.I! 1 I and I! 1I are idempotents.

iv) If I, J are conjugate, the spaces I .H.∇ J and ∇ J .H. I are one-dimensional.

P r o o f. i), ii) For every i 6∈ CS(I) let R i (resp. D i ) be the set of µ ∈ S I such that l(σ i µ) = l(µ) + 1 (resp. l(σ i µ) = l(µ) − 1). It is straightforward to see that D i = σ i .R i . Then

I = ( X

µ∈R

i

T µ + X

µ∈D

i

T µ ) = (1 + T i )( X

µ∈R

i

T µ ),

and the claim follows from the fact that T i (T i + 1) = q(T i + 1). The other identities of i) and ii) have a similar proof.

iii) is an immediate consequence of i) and ii).

iv) If I, J are conjugate, then it is easy to verify that (see also below Remark 6) there is only one ν ∈ S n such that

i 6∈ CS(I), j 6∈ CS(J ) =⇒ l(σ i ν) = l(ν) + 1, l(νσ j ) = l(ν) + 1.

It follows from i) and ii) that I .T ν .∇ J is a generator of I .H.∇ J . Now, from the general theory of Coxeter groups, one has l(ω I .ν.ω J ) = l(ω I ) + l(ν) + l(ω J ) = m and then

I .T ν .∇ J = T ω

I

νω

J

+ X

l(µ)<m

R µ T µ .

This proves that I .T ν .∇ J is torsion free and then the claim follows.

By virtue of the general theory of semi-simple algebras, Proposition 2.iv) above implies the corollary:

Corollary 3. Suppose that k is a field and H k n,q is semi-simple. Let I, J be two conjugate compositions. Then there exist elements µ 0 , µ 00 ∈ S n such that I T µ

0

J T µ

00

is a primitive idempotent of shape I.

In the previous case, the elements I h 0 and ∇ J h 00 can be defined by means of a solution of the Yang-Baxter equation (see Remark 6.ii) below). Let us say now a word on this construction.

Recall that the action of S n from the right on the words of length n, is defined by (a 1 a 2 · · · a n ).σ := a σ(1) a σ(2) · · · a σ(n) .

Let σ i

1

σ i

2

· · · σ i

p

be a reduced decomposition of the permutation µ. The fact that this decomposition is reduced implies that the sequence w 0 , w 1 , . . . defined inductively by:

 w 0 := 12 · · · n w k := w k−1 .σ i

k

,

is such that, at each step, w k = uijv and w k+1 = ujiv with i < j. Then supposing that [r] q ∈ k for r < n and setting s k := [j−i−1] [j−i]

q

q

we deduce that the products (∇ i

1

+ s 1 )(∇ i

2

+ s 2 ) · · · (∇ i

p

+ s p )

and ( i

1

− s 1 )( i

2

− s 2 ) · · · ( i

p

− s p )

do not depend on the choice of the reduced decomposition of µ, but only of µ (see [4] for

a complete proof). We will denote the first product by ∇ µ and the second one by µ .

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The link with the symmetrizers become transparent with the following formulas [4]

ω

I

= X

h∈S

I

T h ∇ ω

I

= X

h∈S

I

(−q) l(ω

I

h) T h

R e m a r k 4. It is not hard to see that the leading term of µ (resp. ∇ µ ) is T µ . In other words, we have

µ = T µ + X

l(ν)<l(µ)

R ν (q)T ν ∇ µ = T µ + X

l(ν)<l(µ)

S ν (q)T ν

with R ν , S ν ∈ k(q).

From now on, we will write ω

I

(resp. ∇ ω

I

) instead of I (resp. ∇ I ).

I.3. Bases for ω

I

.H.∇ ω

J

. In this section, we construct a basis of ω

I

H∇ ω

J

con- sisting of elements of the type ω

I

T σ ∇ ω

J

. This basis is closely related to the minimal representatives of the double classes S I \S n /S J (see [11]). Let us state their properties.

Proposition 5. Let I, J be two compositions of n, and W (I, J ) be the set of σ ∈ S n

such that

l(ω I σω J ) = l(ω I ) + l(σ) + l(ω J ). (I.3) Then

i) W (I, J ) is the set of elements of minimal length in each double class S I .µ.S J and, hence, W (I, J ) is a set of representatives for S I \S n /S J .

ii) ( ω

I

T σ ∇ ω

J

) σ∈W (I,J ) is a basis of the k-module ω

I

H∇ ω

J

. P r o o f. i) is classical.

ii) The family ( ω

I

T µ ∇ ω

J

) µ∈W (I,J ) is linearly independent over k as the dominant term of ω

I

T µ ∇ ω

J

is T ω

I

µω

J

. Now, let M be the linear span of the elements ( ω

I

T µ ∇ ω

J

) µ∈W (I,J ) . It is sufficient to prove that every ω

I

T ν ∇ ω

J

belongs to M for ν ∈ S n . Suppose that it is not the case, then there exists α ∈ S n of minimal length with

ω

I

T α ∇ ω

J

6∈ M . Now, α 6∈ W (I, J ) and then α = σ i α 1 for some i 6∈ CS(I) or α = α 2 σ j

for some j 6∈ CS(J ). Then, for example in the first case,

ω

I

T σ

i

α

1

∇ ω

J

= ω

I

T σ

i

T α

1

∇ ω

J

= q ω

I

T α

1

∇ ω

J

— a contradiction. The other case is similar.

R e m a r k 6. i) Let I = (i 1 , i 2 , · · · i r ), J = (j 1 , j 2 , · · · j s ). Then the set W (I, J ) is in one-to-one correspondence with the set of r × s-matrices with entries in {0, 1} and column (resp. row) sums given by I (resp. J ). We first need a description of ω I .W (I, J ), the elements of which have a simple characterization in terms of subwords on consecutive letters and increasing conditions. Namely an element µ belongs to ω I .W (I, J ) iff:

(a) µ has the decreasing subwords of ω I .

(b) µ is increasing on each interval defined by J .

We now describe the correspondence on an example (for practical reasons, as the parts involved here will be less than 10, we will write I = 1311 instead of I = (1, 3, 1, 1)).

For example, with I = 1311, J = 231, the permutations µ are (written as words)

143562, 451362, 461352. The matrices to be found have 3 rows and 4 columns. Index the

columns by the subwords (condition (a) above), here (1, 432, 5, 6) and the rows by the

intervals of places where the permutation has to be increasing (condition (b) above), here

12, 345, 6. For the first permutation we have

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subwords 1 432 5 6 ↓ places

• • − − 12

− • • • 345

− • − − 6

P ermutation 143562 And, for the two remaining elements of ω 1311 .W (1311, 231)

1 432 5 6

− • • − 12

• • − • 345

− • − − 6

P ermutation 451362

1 432 5 6

− • − • 12

• • • − 345

− • − − 6

P ermutation 461352

ii) For ν ∈ W (I, J ), the leading term of ω

I

T ν ∇ ω

J

is T ω

I

νω

J

, because the lengths add (see Proposition 5). So any family of the form

( ω

I

B ν ∇ ω

J

) ν∈W (I,J )

such that the leading term of B ν is T ν , is also a basis of ω

I

H∇ ω

J

. Its transition matrix with respect to

( ω

I

T ν ∇ ω

J

) ν∈W (I,J )

is triangular. In particular, this is the case of ω

I

ν ∇ ω

J

as one has the factorization

ω

I

ν = ω

I

B ν for some B ν with leading term T ν (see [4] for details).

iii) In general, we deduce from Propositions 1 and 5 that

|W (I, J )| = X

λ`n

m 0 λ .m 00 λ

where m 0 λ (resp. m 00 λ ) is the number of irreducible components of shape λ in ω

I

.H (resp. ∇ ω

J

H). In particular, if I, J are conjugate compositions then |W (I, J )| = 1 and

ω

I

H∇ ω

J

is one-dimensional. In the semi-simple case, this allows to construct primitive idempotents for all possible shapes (see [4]).

iv) Notice that it can happen that W (I, J ) = ∅. This is the case, for example, with I = J = [n], n ≥ 2.

I.4. Characters. When k is of characteristic 0 and q = 1 one can compute the char- acteristics of ω

I

H and ∇ ω

J

H considered as right S n -modules. Here, we have

char( ω

I

H) = S I := S i

1

S i

2

· · · S i

k

, char(∇ ω

J

H) = Λ J := Λ i

1

Λ i

2

· · · Λ i

k

. If I, J are conjugate, these symmetric functions have only one common irreducible com- ponent S λ , λ being the diagram with the row lengths given by I and the column lengths given by J (in fact, we could write λ = I) [12], [13]. We recover the fact that ω

I

H∇ ω

J

is one-dimensional in this case.

I.5. Permutation of parts. Suppose that the symmetric group S k acts on compositions of n into k parts by

I σ = (i 1 , i 2 · · · i k ) σ = (i σ(1) , i σ(2) , · · · i σ(k) ).

Here we show that ω

I

(resp. ∇ ω

I

) and ω

(resp. ∇ ω

) are conjugate.

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Proposition 7. Let I be a composition of n belonging to N k . For every σ ∈ S k there exists τ (σ) ∈ S n such that

ω

= T τ (σ) ω

I

T τ (σ) −1ω

= T τ (σ)ω

I

T τ (σ) −1 .

P r o o f. This is a direct consequence of the fact that the Young subgroups S ω

and S ω

I

are conjugate.

Corollary 8. I(I σ

1

, J σ

2

) = T τ (σ

1

) I(I, J ).

This explains how the results for general I, J can be computed from the case when I, J are partitions.

II. Structure of I(I, J ).

II.1. Isotypic decomposition of I(I, J ). From now on we suppose that k is a field and q.[n!] q 6= 0 (this implies that H n,q is semi-simple). The following result is classical and can be derived from the thesis of Hoefsmith [7] or the orthogonal family of idempotents of Jucys-Murphy [10], [16].

Proposition 9. There is a family of orthogonal central idempotents (e λ ) λ`n . Hence H n,q = M

λ`n

e λ .H n,q ,

each summand being a matrix algebra

e λ .H n,q ∼ = M(n λ , k)

where n λ is the dimension of the representation associated with the partition λ.

We derive the following decomposition of I(I, J ).

Theorem 10. I(I, J ) = L

λ`n (S

λ

J

)6=0

ω

I

H.e 0 λ .H where e 0 λ is any minimal idempotent of shape λ. In particular, there exists h 0 , h 00 ∈ H such that e 0 λ = ω

λ

h 0 ∇ ω

λ˜

h 00 .

P r o o f. Of course, we have I(I, J ) = M

λ`n

e λ .I(I, J ) = M

λ`n (S

λ

J

)6=0

ω

I

.H.e λ .∇ ω

J

.H

as, if (S λ , Λ J ) = 0, then H.e λ .∇ ω

J

.H = {0} and H.e λ .I(I, J ) = ω

I

.H.e λ .∇ ω

J

.H = {0} (indeed, this is the case also if (S λ , S J ) = 0). Otherwise, there exists a minimal idempotent e 0 λ of shape λ such that ∇ ω

J

.H ⊃ e 0 λ .H, and hence

H.e λ .H ⊃ H.e λ ∇ ω

J

.H ⊃ H.e 0 λ .H = H.e λ .H.

This proves the claim.

R e m a r k 11. Let J be an ideal of H. Then, with the previous notation, we have Je λ = Je 0 λ .H.

This ideal is the sum of the components of “type λ” in J. We will denote this ideal by J λ . One has

dim(J λ ) = m λ .n λ

where m λ is the multiplicity of the representation associated with λ and n λ — its dimen-

sion.

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Here, we have

e λ .I(I, J ) = ω

I

.H.e 0 λ .H = ( ω

I

.H) λ .

II.2. Character and basis of I(I, J ). Let, as above, m λ be the multiplicity of e 0 λ .H in I(I, J ). From Remark 11 we deduce that, if (S λ , Λ J ) 6= 0, then

m λ = dim(Hom H ( ω

I

.H, e 0 λ .H)) = dim( ω

I

.H.e 0 λ ).

This allows us to construct bases of I(I, J ).

Proposition 12. Let ( ω

I

.h i e 0 λ ) i∈I

λ

be a basis in each non-vanishing ω

I

.H.e 0 λ and (e 0 λ .h 0 j ) j∈J

λ

a basis of e 0 λ .H. Then

( ω

I

h i e 0 λ h 0 j ) (i,j)∈I

λ

×J

λ

is a basis of I λ (I, J ).

P r o o f. Let ( ω

I

.h i e 0 λ ) i∈I

λ

(resp. (e 0 λ .h 0 j ) j∈J

λ

) be a basis of ω

I

.H.e 0 λ (resp. e 0 λ .H).

It is obvious that ( ω

I

h i e 0 λ h 0 j ) (i,j)∈I

λ

×J

λ

generates I λ (I, J ). But Remark 11 states that dim(I λ (I, J )) = card (I λ × J λ ) and, then, this family is a basis of I λ (I, J ).

R e m a r k 13. Since

I(I, J ) = M

λ`n

I λ (I, J ),

the sum being taken over all λ such that (S λ , S I )(S λ , Λ J ) 6= 0 (otherwise I λ (I, J ) = {0}), we get a basis of I(I, J ) by union of bases of Proposition 12.

Example. With I = 211, J = 22, we have S 211 = S 4 + 2S 13 + S 22 + S 112 and Λ 22 = S 22 + S 112 + S 1111 then I λ (I, J ) 6= 0 for λ = 211 and λ = 22. We get a basis of I 211 : 2341 ∇ 3214 and a basis of I 22 : 2413 ∇ 2143 . Then the desired basis of I(211, 22) is

{ 2341 ∇ 3214 , 2413 ∇ 2143 }.

III. Conclusion. Bases and characters of the ideal I(I, J ) have been described. In general, bases for an isotypic component are indexed by two indices. For the second range, we have a nice description for a basis of e 0 λ .H in case e 0 λ is chosen to be of the form

ω

λ

h 0 ∇ ω

λ˜

h 00 [4], [3].

References

[1] G. E. A n d r e w s, The theory of partitions, Addison-Wesley, London, 1976.

[2] C. W. C u r t i s, I. R e i n e r, Representations theory of finite groups and associative algebras, Interscience, New York, 1962.

[3] R. D i p p e r and G. J a m e s, Blocks and idempotents of Hecke algebras of general linear groups, Proc. London Math. Soc. (3) 54 (1987), 57–82.

[4] G. D u c h a m p, D. K r o b, B. L e c l e r c, A. L a s c o u x, T. S c h a r f, J. Y. T h i b o n, Euler- Poincar´ e characteristic and polynomial representations of Iwahori-Hecke algebras, Publ.

Res. Inst. Math. Sci. 31 (1995), 179–201.

[5] W. F u l t o n and J. H a r r i s, Representation Theory, a first course, Graduate Texts in Mathematics 129, Springer, New York, 1991.

[6] A. G y o j a, A q-analogue of Young symmetrizer , Osaka J. Math. 23 (1986), 841–852.

[7] P. N. H o e f s m i t h, Representations of Hecke algebras of finite groups with BN-pairs of

classical type, Ph.D. Thesis, Univ. of British Columbia, 1974.

(10)

[8] J. E. H u m p h r e y s, Reflection Groups and Coxeter Groups, Cambridge Studies in Ad- vanced Mathematics 29, Cambridge University Press, Cambridge, 1990.

[9] G. J a m e s, A. K e r b e r, The Representation Theory of the Symmetric Group, Encyclopedia of Mathematics and its Application 16, Addison-Wesley, Reading, 1981.

[10] A. A. A. J u c y s, Symmetric polynomials and the center of the symmetric group ring , Institute of Physics and Mathematics of the Academy of Sciences, Lithuanian SSR, USSR, Reports on Mathematical Physics 5 (1974).

[11] A. K e r b e r, Algebraic Combinatorics Via Finite Group Actions, Wissenschaftsverlag, Mannheim, 1991.

[12] A. L a s c o u x and M.-P. S c h ¨ u t z e n b e r g e r, Formulaire Raisonn´ e de fonctions Sym´ e- triques, LITP, U.E.R. Maths, Paris VII, Oct. 1985.

[13] A. L a s c o u x and M.-P. S c h ¨ u t z e n b e r g e r, Le monoide plaxique, Quaderni de ’La ricerca scientifica’, No. 109, ROMA, CNR, 1981.

[14] V. F. M o lˇ c a n o v, On matrix elements of irreducible representations of a symmetric group, Vestnik Moskov. Univ. Ser. I Mat. Mekh. 21 (1966), No. 1, 52–57.

[15] G. E. M u r p h y, The idempotents of the symmetric group and Nakayama’s conjecture, J.

Algebra 81 (1983), 258–265.

[16] G. E. M u r p h y, On the Representation theory of the Symmetric Groups and Associated Hecke Algebras, J. Algebra 152 (1992), 492–513.

[17] D. E. R u t h e r f o r d, Substitutional Analysis, University Press, Edinburgh, 1948.

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