Journal of Algebraic Combinatorics 11 (2000), 269–275 c 2000 Kluwer Academic Publishers. Manufactured in The Netherlands. ° On the Connection Between Macdonald Polynomials and Demazure Characters YASMINE B. SANDERSON Department of Mathematics, Rutgers University, New Brunswick, N.J. 08901 sanderso@math.rutgers.edu Received March 30, 1998; Revised November 17, 1998; Accepted December 21, 1998 Abstract. We show that the specialization of nonsymmetric Macdonald polynomials at t = 0 are, up to multid This connection furnishes Lie-theoretic plication by a simple factor, characters of Demazure modules for sl(n). proofs of the nonnegativity and monotonicity of Kostka polynomials. Keywords: affine Lie algebras, Macdonald polynomials, Demazure character 1. Introduction Macdonald defined a special class of polynomials Pλ (z, q, t), called symmetric Macdonald polynomials, which form a basis of the symmetric polynomials in C(q, t)[z 1 , . . . , z n ]. These polynomials are indexed by partitions λ ∈ Nn , λ1 ≥ λ2 ≥ · · · λn ≥ 0. They interpolate between several classes of classical polynomials: Pλ (z, 0, t) are the Hall-Littlewood polynomials, which, in turn are the Schur functions when t = 0. By setting q = t α and letting t go to 1, one obtains Jack polynomials. In [11], Macdonald mentions that there is no similar interpretation of Pλ (z, q, 0). By using the theory of nonsymmetric Macdonald polynomials, we show that the Pλ (z, q, 0) are the characters (up to factor) of certain Demazure modules d This interpretation allows us to obtain Lie-theoretic proofs of the nonnegativity of sl(n). and monotonicity of Kostka polynomials. In addition, it gives us a branching rule for the d decomposition of certain integrable highest weight sl(n)-modules under the action of sl(n). The connection between Demazure characters and symmetric functions has already been explored in [8] using a path realization of the crystal basis. The results in this paper intersect somewhat with those in [8]. The main advantage of our approach is its simplicity and its explanation of the connection with Macdonald polynomials. Nonnegativity and positivity of Kostka polynomials have already been proven by Lascoux-Schützenberger [9], Butler [1], Lusztig [10]. The connection between the branching rule and Kostka polynomials was explored in [5]. A different representation-theoretic interpretation of Pλ (z, q, 0) is given in [4]. 2. Nonsymmetric Macdonald polynomials These nonsymmetric analogues of the symmetric Macdonald polynomials were first introduced in [12, 14]. Nonsymmetric Macdonald polynomials E λ (z, q, t) are indexed by compositions λ ∈ Nn and form a basis of C(q, t)[z 1 , . . . , z n ]. (See [2, 5] for their precise 270 SANDERSON definition). In [6], Knop gives a recursive description of the E λ (z, q, t). We describe this recursion for when t = 0. In this case, we have E λ (z, q, 0) ∈ Z[q, q −1 ][z 1 , . . . , z n ]. For ease of notation, we will denote E λ (z, q, 0) simply by E λ from now on. For i ∈ [1, . . . , n −1] let si be the simple reflection that interchanges z i and z i+1 . Consider the following operators on Z[q, q −1 ][z 1 , . . . , z n ]: (1 − si ) for i ∈ [1, . . . , n − 1] (z i − z i+1 ) 8f (z 1 , . . . , z n ) := z n f (q −1 z n , z 1 , . . . , z n−1 ) H̄i := si − z i+1 H̄0 := 8 H̄1 8−1 = 8−1 H̄n−1 8 Then the recursion relations are given by [6] Theorem 1 The E λ are generated by application of the H̄i (0 ≤ i < n) and 8 to 1. More precisely, set E (0n ) := 1. The action of 8 and the H̄i on the set of E λ for λ ∈ Nn is as follows: q λ1 8E (λ1 ,...,λn ) = E (λ2 ,...,λn ,λ1 +1) ½ E si λ if λi < λi+1 for 1 ≤ i ≤ n − 1 H̄i E λ = Eλ if not where si λ is the composition λ with λi and λi+1 interchanged. ½ E (λn −1,λ2 ,...,λn−1 ,λ1 +1) if λ1 > λn − 1 q λ1 −λn +1 H̄0 E λ = if not Eλ To ease notation, we define the operators H̃0 and 8̃ on the set of nonsymmetric Macdonald polynomials: H̃0 E (λ1 ,...,λn ) := q λ1 −λn +1 H̄0 E (λ1 ,...,λn ) = E (λn −1,λ2 ,...,λn−1 ,λ1 +1) 8̃E (λ1 ,...,λn ) := q λ1 8E (λ1 ,...,λn ) = E (λ2 ,...,λn ,λ1 +1) Although this definition of nonsymmetric Macdonald polynomials is given for only λ ∈ Nn , we can easily extend it to compositions λ ∈ Zn by defining E λ := 8̃−mn E λ+(m n ) = q −(m|λ|+nm(m+1)/2) 8−mn E λ+(m n ) where m is chosen large enough so that λ + (m n ) = (λ1 + m, . . . , λn + m) is in Nn . The E λ are well-defined (don’t depend on the choice of m). In fact, let m 1 and m 2 , with m 1 ≤ m 2 , be two such choices. Then, 8̃−m 2 n E λ+(m n2 ) = 8̃−m 1 n 8̃−(m 2 −m 1 )n E λ+(m n2 ) = 8̃−m 1 n E λ+(m n1 ) , the last equality following from the well-definedness of the E µ for µ ∈ Nn . Note that the E λ are elements of Z[q, q −1 ][z 1 , z 1−1 , . . . , z n , z n−1 ]. MACDONALD POLYNOMIALS AND DEMAZURE CHARACTERS 271 We now check that, for λ ∈ Zn \Nn , the E λ satisfy the recursion relations. For i 6= 0, E si ·λ = 8̃−mn E si ·λ+(m n ) = 8̃−mn H̄i 8̃mn E λ = H̄i E λ Now, let λ∗ := (λn − 1, λ2 , . . . , λn−1 , λ1 + 1) and choose m such that λ∗ + (m n ) ∈ Nn . Then E λ∗ = 8̃−mn E λ∗ +(m n ) = 8̃−mn H̃0 8̃mn E λ = q λ1 −λn +1 H̄0 E λ , the last equality following from the commutativity of the H̄i with 8̃n . This proves that, for all λ ∈ Zn , the E λ satisfy the relations of Theorem 1. Let Bm denote the Z[q, q −1 ]-vector space generated by all E λ with |λ| = m. Then the H̄i Bm ⊂ Bm for all i and 8Bm ⊂ Bm+1 . The action of the H̄i (i 6= 0) and H̃0 on the E λ is related to the action of the affine Weyl group on compositions: si · (λ1 , . . . , λn ) := (λ1 , . . . , λi−1 , λi+1 , λi , λi+2 , . . . , λn ) so · (λ1 , . . . , λn ) := (λn − 1, λ2 , . . . , λn−1 , λ1 + 1) The connection between compositions of a given degree, say m, and elements of the affine Weyl group is as follows. Let m = kn + i where k ≥ 0 and 0 ≤ i < n. Then the smallest composition is ηm := (k, . . . k, k + 1, . . . , k + 1) (i factors of k + 1 and n − i factors of k). Every composition λ of degree m equals w · ηm where w is an affine Weyl group element. For w = si1 , . . . , si j a reduced decomposition, we define H̄w := H̄i1 , . . . , H̄i j and H̃w the same expression but with H̄0 replacedP by H̃0 . For a composition λ ∈ Zn , let u(λ) := i λi (λ2i −1) . Theorem 2 We can write E λ = H̃w 8̃|λ| · 1 = q u(λ) H̄w 8|λ| · 1 where w is determined by λ = wη|λ| . Proof: By the commuting relations of 8 and the H̄i [6], ( i = 1, . . . , n − 2 8 H̄i+1 = H̄i 8 82 H̄1 = H̄n−1 82 we need only prove that the power of q is u(λ) by induction. For i ≥ 1, the actions of the H̄i do not involve any powers of q. The operator H̄0 equals 8 H̄1 8−1 by definition. Therefore, we need only check that this holds for 8. Let µ = (λ1 , . . . , λn−1 , λn + 1). We have E µ = q λn 8E λ = q λn q u(λ) 8Hw 8|λ| · 1 = q u(µ) Hw0 8|µ| · 1 where Hw0 is determined by the above commutation relations. 2 Remark We note that 8̃nk+i · 1 = q u(ηnk+i ) (z 1 , . . . , z n )k z n−i+1 · · · z n . The H̄i (all i) commute with multiplication by q and the symmetric function z 1 · · · z n . Therefore, E λ = q u(ηnk+i ) (z 1 , . . . , z n )k H̃w z n−i+1 · · · z n . We will use this information in Section 4. 272 3. SANDERSON d Demazure modules of sl(n) Let 3 be a dominant integral weight. Let V = V (3) be the unique (up to isomorphism) d irreducible highest weight sl(n)-module with highest weight 3. Let W be the Weyl group d of sl(n). For each w ∈ W , the weight space Vw(3) of weight w(3) is one-dimensional. We consider E w (3), the b-module generated by Vw(3) , where b is the Borel subalgebra. The E w (3), called Demazure modules, are finite-dimensional vector spaces which form a filtration of V which is compatible with the Bruhat order on W : w ≤ w0 ⇔ E w (3) ⊆ E w0 (3). To each Demazure module E w (3), we can associate its character χ(E w (3): X (dim E w (3)µ )eµ χ(E w (3)) := µ weight Since the E w (3) are finite dimensional, the χ(E w (3)) are polynomials in the n simple roots αi and lie in the group ring for the weight lattice P. We now define Demazure operators. For each αi , we define an operator 1i on P: 1i := 1 − e−αi si 1 − e−αi where si is the simple reflection with respect to αi . Let w = si1 si2 · · · si j be a reduced decomposition. Then, we can define 1w := 1i1 1i2 · · · 1i j and 1w does not depend on the choice of reduced decomposition. The connection between characters and Demazure operators is given by [3, 7, 13]: Theorem 3 χ(E w (3)) = 1w (e3 ). 4. Macdonald polynomials and Demazure module characters d defined by (3i , α j ) = δi j . Let Let 30 , . . . , 3n−1 denote the n fundamental weights of sl(n) Pn−1 δ = i=0 αi . Let π be the ring homomorphism π : Z[q, q −1 ][z 1 , . . . , z n ] → P defined by: π(z i ) = e3i −3i−1 for i < n, π(z n ) = e30 −3n−1 and π(q) = e−δ . Theorem 4 The operator H̄i is equivalent to the Demazure operator 1i in the sense that the following diagram commutes: Z[q, q −1 ][z 1 , . . . , z n ] H̄i ↓ Z[q, q −1 ][z 1 , . . . , z n ] →P π ↓1 (e →P π i 30 · ) Proof: We have that H̄i , i 6= 0 (resp. H̄0 ) commutes with multiplication by z j for j 6= i or i +1 (resp. z 1 or z n ). Therefore, one only needs to verify this equivalence on the monomials b (resp. z 1a z nb ). This is done by direct computation. 2 z ia z i+1 MACDONALD POLYNOMIALS AND DEMAZURE CHARACTERS 273 Let C be the following “change of basis” operator on P: C(e30 ) = e3n−1 and C(e3i ) = for 1 ≤ i ≤ n − 1. e 3i−1 −δ Theorem 5 The operator 8 is equivalent to the operator C in the sense that the following diagram commutes: Z[q, q −1 ][z 1 , . . . , z n ] ↓ 8 Z[q, q −1 ][z 1 , . . . , z n ] Proof: →P π ↓C →P π 2 By direct computation. Theorems 1, 4, 5 along with the preceding Remark give us our main result: Theorem 6 Through the π homomorphism, we can identify q −u(λ)+u(η|λ| ) E λ with χ (E w (3i )) where i = |λ| mod n and where w is an affine Weyl group element defined by λ = wη|λ| . Proof: We have that E λ = q u(λ) H̄w 8|λ| · 1 = q u(λ)−u(η|λ| ) (z 1 · · · z n )k H̄w z n−i+1 · · · z n . We have π(z 1 z 2 · · · z n ) = 1 and π(z n−i+1 · · · z n ) = e3i . Therefore, π(E λ ) = q u(λ)−u(η|λ| ) 1w e3i . 2 Remark 1. π(E λ ) having nonnegative coefficients implies that E λ has nonnegative coefficients. 2. By setting q = 1, one obtains the real character of a Demazure module (see [15]). For λ a partition, we have the factorization ([11], p. 324) Pλ (z, 1, 0) = eλ0 (z) = n Y λ −λi+1 ei i (z) i=1 where ei (z) is the ith elementary symmetric function. This gives us a similar factorization of χ(E w (3)) = q −u(λ)+u(η|λ| ) n−1 Y ei (π(z))λi −λi+1 . i=1 Previous examples of this factorization are found in [8, 15]. 274 5. SANDERSON Positivity and monotonicity of Kostka polynomials Recall that Pλ (z, q, t) denotes the symmetric Macdonald polynomial associated to the partition λ. Theorem 7 For λ a partition, we have E λ (z, q, 0) = Pλ (z, q, 0). P Proof: Consider w∈W H̄w E λ (z, q, t). It is symmetric and satisfies the same defining conditions as Pλ (z, q, t) (see [6]), therefore is a scalar multiple of it. When t = 0, we have H̄w E λ (z, q, 0) = E λ (z, q, 0). By comparing coefficients of the leading coefficient z λ in 2 both E λ (z, q, 0) and Pλ (z, q, 0), we see that we have equality. Recall that one has the following order relation on partitions: two partitions γ and µ such that |γ | = |µ| satisfy γ < µ if γ1 + · · · + γi ≤ µ1 + · · · + µi for all i with strict inequality for some i. P It is known [[11], VI (8.11)] that Pλ (z, q, 0) = µ≤λ K µλ (q, 0)sµ (z) where K is the Kostka function and the sµ are the Schur functions. In addition, it is known [[11], p. 355] 0 0 that K µλ (q, 0) = KP µ0 λ0 (q) where µ (resp. λ ) is the dual partition of µ (resp. λ). It follows that Pλ (z, q, 0) = µ≤λ K µ0 λ0 (q)sµ (z). Theorem 8 The K µλ (q) have positive coefficients. Proof: We have that Pλ (z, q, 0) is invariant under the H̄i (for i 6= 0). This is equivalent to saying that the Demazure module E w (30 ) decomposes as a direct sum of simple sl(n)modules. In fact, we have the following decomposition: E w (30 ) = ⊕ j∈Z (E w (30 )) jδ where (E w (30 )) jδ is just the direct sum of weight spaces whose weights are of the form υ = κ + jδ where κ is some weight for sl(n). (In other words, these are all weights that satisfy hυ, di = j where d is the scaling element.) Since δ is orthogonal to the Cartan subalgebra of sl(n), each (E w (30 )) jδ is a direct sum of irreducible sl(n)-modules. Let λ = wν|λ| . The Pλ (z, q, 0) merely represents the character χ(E w (30 )) as seen in this light; since the sµ (z) is a character of an irreducible sl(n)-module, the coefficient of q j in K µ0 λ0 (q) is the multiplicity of the sl(n)-module of highest weight µ − jδ in E w (30 ). Therefore, the 2 K µ0 λ0 (q) have positive coefficients. Remark A consequence of this theorem is that the Kostka numbers K µλ (1) are the multiplicities of the (finite-dimensional) sl(n)-modules in the Demazure modules E w (3). d of highest weight Recall that V = V (3i ) is the irreducible highest weight sl(n)-module 3i . We have that χ (V ) = lim`(w)→∞ χ(E w (3i )). We can now describe the branching rule for V in terms of Kostka polynomials (see [5]). Let {λ j } be an “increasing” sequence of partitions in the sense that λ j := w j ν|λ j | where lim j `(w j ) = ∞ and where |λ j | = i(mod n). We must choose ν|λ j | such that the resulting λ j are still partitions. MACDONALD POLYNOMIALS AND DEMAZURE CHARACTERS 275 Corollary 1 The multiplicity of the sl(n)-module of weight µ in V is given by lim q −u(λ j )+u(ν|λ j | ) j→∞ K µ0 λ j0 (q) We also have a monotonicity result. Let K̃ λµ (q) := q −u(µ) K λµ (q). Recall that if λ = wνm and γ = w0 νm , λ 6= γ are partitions, then λ < γ if and only if w < w0 in the Bruhat order, where w and w 0 are chosen to have smallest length. Theorem 9 K̃ λµ (q) − K̃ λν (q) has nonnegative coefficients when ν ≥ µ. Proof: Let υ < γ be two partitions such that υ = w0 η|λ| and γ = wη|λ| . Then w0 < w and E w0 (3) ⊂ E w (3). The coefficient of q j in K̃ ν 0 γ 0 (q) − K̃ ν 0 υ 0 (q) is the multiplicity of the sl(n)-module of weight ν − jδ ( j ∈ Z) in E w (3)/E w0 (3). Therefore, it has positive coefficients. 2 Acknowledgments The connection between Demazure characters and Macdonald polynomials was pointed out by I. Cherednik. The author thanks the referees for helpful comments. References 1. L.M. Butler, “Subgroup lattices and symmetric functions,” Memoirs of the A.M.S 112(539), (1994). 2. I. Cherednik, “Double affine Hecke algebras and Macdonald’s conjectures,” Ann. Math. 141 (1995), 191–216. 3. M. 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