The Littlewood-Richardson rule and Gelfand-Tsetlin patterns

We give a survey on the Littlewood-Richardson rule. Using Gelfand-Tsetlin patterns as the main machinery of our analysis, we study the interrelationship of various combinatorial descriptions of the Littlewood-Richardson rule.

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Hauptverfasser: Doolan, P., Kim, S.
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spelling irk-123456789-1557442019-06-18T01:25:22Z The Littlewood-Richardson rule and Gelfand-Tsetlin patterns Doolan, P. Kim, S. We give a survey on the Littlewood-Richardson rule. Using Gelfand-Tsetlin patterns as the main machinery of our analysis, we study the interrelationship of various combinatorial descriptions of the Littlewood-Richardson rule. 2016 Article The Littlewood-Richardson rule and Gelfand-Tsetlin patterns / P. Doolan, S. Kim // Algebra and Discrete Mathematics. — 2016. — Vol. 22, № 1. — С. 21-47. — Бібліогр.: 29 назв. — англ. 1726-3255 2010 MSC:05E10, 20G05, 52B20. http://dspace.nbuv.gov.ua/handle/123456789/155744 en Algebra and Discrete Mathematics Інститут прикладної математики і механіки НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
description We give a survey on the Littlewood-Richardson rule. Using Gelfand-Tsetlin patterns as the main machinery of our analysis, we study the interrelationship of various combinatorial descriptions of the Littlewood-Richardson rule.
format Article
author Doolan, P.
Kim, S.
spellingShingle Doolan, P.
Kim, S.
The Littlewood-Richardson rule and Gelfand-Tsetlin patterns
Algebra and Discrete Mathematics
author_facet Doolan, P.
Kim, S.
author_sort Doolan, P.
title The Littlewood-Richardson rule and Gelfand-Tsetlin patterns
title_short The Littlewood-Richardson rule and Gelfand-Tsetlin patterns
title_full The Littlewood-Richardson rule and Gelfand-Tsetlin patterns
title_fullStr The Littlewood-Richardson rule and Gelfand-Tsetlin patterns
title_full_unstemmed The Littlewood-Richardson rule and Gelfand-Tsetlin patterns
title_sort littlewood-richardson rule and gelfand-tsetlin patterns
publisher Інститут прикладної математики і механіки НАН України
publishDate 2016
url http://dspace.nbuv.gov.ua/handle/123456789/155744
citation_txt The Littlewood-Richardson rule and Gelfand-Tsetlin patterns / P. Doolan, S. Kim // Algebra and Discrete Mathematics. — 2016. — Vol. 22, № 1. — С. 21-47. — Бібліогр.: 29 назв. — англ.
series Algebra and Discrete Mathematics
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fulltext Algebra and Discrete Mathematics RESEARCH ARTICLE Volume 22 (2016). Number 1, pp. 21–47 © Journal “Algebra and Discrete Mathematics” The Littlewood-Richardson rule and Gelfand-Tsetlin patterns Patrick Doolan and Sangjib Kim Communicated by V. A. Artamonov Abstract. We give a survey on the Littlewood-Richardson rule. Using Gelfand-Tsetlin patterns as the main machinery of our analysis, we study the interrelationship of various combinatorial descriptions of the Littlewood-Richardson rule. 1. Introduction 1.1. Let us consider Schur polynomials sµ, sν and sλ in n variables labelled by partitions µ, ν and λ, respectively. The Littlewood-Richardson (LR) coefficient is the multiplicity cλ µ,ν of sν in the product of sµ and sν : sµsν = ∑ λ cλ µ,νsλ and its description is called the LR rule. The same number appears in the tensor product decomposition prob- lem in the representation theory of the complex general linear group GLn and Schubert calculus in the cohomology of the Grassmannians, and is also related to the eigenvalues of the sum of Hermitian matrices. For more details, we refer readers to [8, 15,27,29]. 2010 MSC: 05E10, 20G05, 52B20. Key words and phrases: Littlewood-Richardson rule, Gelfand-Tsetlin patterns. 22 The Littlewood-Richardson rule 1.2. The LR rule is usually stated in terms of combinatorial objects called LR tableaux. Recall that a Young tableau is a filling of the boxes of a Young diagram with positive integers. We shall use the English convention of drawing Young diagrams and tableaux as in [7, 26] and assume a basic knowledge of these objects. Definition 1. A tableau T on a skew Young diagram is called a LR tableau if it satisfies the following conditions: 1) it is semistandard, that is, the entries in each row of T weakly increase from left to right, and the entries in each column strictly increase from top to bottom; and 2) its reverse reading word is a Yamanouchi word (or lattice permuta- tion). That is, in the word x1x2x3 . . . xr obtained by reading all the entries of T from left to right in each row starting from the bottom one, the sequence xrxr−1xr−2 . . . xs contains at least as many a’s as it does (a+ 1)’s for all a > 1. For example, the following is a LR tableau on a skew Young diagram (11, 7, 5, 3)/(5, 3, 1) 1 1 1 1 1 1 1 2 2 2 2 3 3 3 2 4 4 and its reverse reading word is 24423331222111111. Remark 1. (1) In this paper we assume each tableau’s entries weakly increase from left to right in every row. (2) From the second condition in the above definition, which we will call the Yamanouchi condition, the bth row of a LR tableau does not contain any entries strictly bigger than b for all b > 1. The number of LR tableaux on the skew shape λ/µ with content ν is equal to the LR number cλ µ,ν . Here, the content ν = (ν1, . . . , νn) of a tableau means that the entry k appears νk times in the tableau for k > 1. See, for example, [24, §I.9] and [15]. 1.3. In this paper, we survey variations of the semistandard and Ya- manouchi conditions with an emphasis on dualities in combinatorial descriptions of the LR rule. Although many of the results in this paper can be found in the literature, we will give complete and elementary proofs of our statements. P. Doolan, S. Kim 23 (1) In Theorem 1 and Theorem 2, we analyse hives, introduced by Knutson and Tao along with their honeycomb model [21], in terms of Gelfand-Tsetlin(GT) patterns [10]. We then show how the interlacing conditions in GT patterns are intertwined to form the defining conditions of hives. For the relevant results, see for example [1–4]. (2) In Theorem 3, we show that the semistandard and Yamanouchi conditions in LR tableaux are equivalent to, respectively, the interlacing and exponent conditions in GZ schemes introduced by Gelfand and Zelevinsky [11]. As a corollary we obtain a correspondence between LR tableaux and hives equivalent to [18, (3.3)]. We then observe how conditions on LR tableaux, GZ schemes and hives are translated between objects by this bijection. For the relevant results, see, for example, [1, 5, 18,19]. (3) In Theorem 4, we show that the semistandard and Yamanouchi conditions in LR tableaux are equivalent to, respectively, the exponent and semistandard conditions in their companion tableaux introduced by van Leeuwen [29]. Here the correspondence between conditions is obtained by taking the transpose of matrices. As a consequence, we obtain bijections between the families of combi- natorial objects counting the LR number. 1.4. In [16,17], Howe and his collaborators constructed a polynomial model for the tensor product of representations in terms of two copies of the multi-homogeneous coordinate ring of the flag variety, and then studied its toric degeneration with the SAGBI-Gröbner method. Through the characterization of the leading monomials of highest weight vectors, their toric variety is encoded by the LR cone [25]. On the other hand, via toric degenerations, the flag variety may be described in terms of the lattice cone of GT patterns [13,20,23]. These results led us to study the LR rule in terms of two sets of interlacing or semistandard conditions and to investigate the interrelationship of various combinatorial descriptions of the LR rule with GT patterns. 2. Hives and GT patterns I In this section, we define GT patterns, hives, and objects related to them. We also describe hives in terms of pairs of GT patterns. 2.1. We set, once and for all, three polynomial dominant weights of the complex general linear group GLn, that is, the sequences of nonnegative 24 The Littlewood-Richardson rule integers: λ = (λ1, . . . , λn), µ = (µ1, . . . , µn), ν = (ν1, . . . , νn) such that λi > λi+1, µi > µi+1, and νi > νi+1 for all i. We define the dual λ∗ of λ to be λ∗ = (−λn,−λn−1, . . . ,−λ1), and define µ∗ and ν∗ similarly. 2.2. Let us consider an array of integers, which we will call a t-array T = ( t (1) 1 , . . . , t (i) j , . . . , t(n) n ) ∈ Z n(n+1)/2 where 1 6 j 6 i 6 n. We are particularly interested in the case when the entries of T are either all non-negative or all non-positive integers. Definition 2. A t-array T = (t (i) j ) ∈ Z n(n+1)/2 is called a GT pattern for GLn if it satisfies the interlacing conditions: IC(1): t (i+1) j > t (i) j IC(2): t (i) j > t (i+1) j+1 for all i and j. We shall draw a t-array in the reversed pyramid form. For example, a generic GT pattern for GL5 is t (5) 1 t (5) 2 t (5) 3 t (5) 4 t (5) 5 t (4) 1 t (4) 2 t (4) 3 t (4) 4 t (3) 1 t (3) 2 t (3) 3 t (2) 1 t (2) 2 t (1) 1 where the entries are weakly decreasing along the diagonals from left to right. Then, the dual array T ∗ = (s (i) j ) of T is the t-array obtained by reflecting T over a vertical line and then multiplying −1, i.e., s (i) j = −t (i) i+1−j for all 1 6 j 6 i 6 n. P. Doolan, S. Kim 25 Definition 3. For a t-array T = (t (i) j ) ∈ Z n(n+1)/2, 1) the kth row of T is t(k) = (t (k) 1 , t (k) 2 , . . . , t (k) k ) ∈ Z k for 1 6 k 6 n. The type of T is its nth row; 2) the weight of T is (w1, w2, . . . , wn) ∈ Z n where w1 = t (1) 1 and wi = i ∑ k=1 t (i) k − i−1 ∑ k=1 t (i−1) k for 2 6 i 6 n. Note that if T is of type λ and weight w ∈ Z n, then T ∗ is of type λ∗ and weight −w. GT patterns were introduced by Gelfand and Tsetlin in [10] to label the weight basis elements of an irreducible representation of the general linear group. The weight of T is exactly the weight of the basis element labelled by T in the irreducible representation V µ n whose highest weight is µ = t(n). It follows that the dual array T ∗ of T corresponds to a weight vector in the contragradiant representation of V µ n . 2.3. Let us consider an array of nonnegative integers, which we will call a h-array, (h0,0, . . . , ha,b, . . . , hn,n) ∈ Z (n+1)(n+2)/2 where 0 6 a 6 b 6 n and h0,0 = 0. Definition 4. A hive for GLn is a h-array H = (ha,b) ∈ Z (n+1)(n+2)/2 satisfying the rhombus conditions: RC(1): (ha,b + ha−1,b−1) > (ha−1,b + ha,b−1) for 1 6 a < b 6 n, RC(2): (ha−1,b + ha,b) > (ha,b+1 + ha−1,b−1) for 1 6 a 6 b < n, RC(3): (ha,b + ha,b+1) > (ha+1,b+1 + ha−1,b) for 1 6 a 6 b < n. We shall draw a h-array in the pyramid form. For example, a generic hive for GL3 is shown below. h0,0 h0,1 h1,1 h0,2 h1,2 h2,2 h0,3 h1,3 h2,3 h3,3 26 The Littlewood-Richardson rule The rhombus conditions RC(1), RC(2), and RC(3) then say that, for each fundamental rhombus of one of the following forms, A O′ A′ O O′ A′ O A O , A′ , O′ A the sum of entries at the obtuse corners is bigger than or equal to the sum of entries at the acute corners, i.e., O +O′ > A+A′. For polynomial dominant weights µ, ν, and λ of GLn, we let H(µ, ν, λ) denote the set of all h-arrays such that µ = (h0,1 − h0,0, h0,2 − h0,1, . . . , h0,n − h0,n−1), ν = (h1,n − h0,n, h2,n − h1,n, . . . , hn,n − hn−1,n), (1) λ = (h1,1 − h0,0, h2,2 − h1,1, . . . , hn,n − hn−1,n−1). That is, the three boundary sides of H ∈ H(µ, ν, λ) are fixed: h0,i = µ1 + µ2 + · · · + µi hi,n = n ∑ j=1 µj + ν1 + ν2 + · · · + νi hi,i = λ1 + λ2 + · · · + λi for 1 6 i 6 n. Recall that we always set h0,0 = 0. Let H◦(µ, ν, λ) be the subset of H(µ, ν, λ) satisfying the rhombus conditions. This is the set of hives whose boundaries are described by (1). Hives were introduced by Knutson and Tao in [21] along with their honeycomb model to prove the saturation conjecture. In particular, the number of hives in H◦(µ, ν, λ) is equal to the LR number cλ µ,ν . See also [5, 22,25]. 2.4. For each h-arrayH = (ha,b) ∈ Z (n+1)(n+2)/2, let us define its derived t-arrays T1 = (x (i) j ), T2 = (y (i) j ), T3 = (z (i) j ) whose entries are obtained from the differences of adjacent entries of H. More specifically, for each fundamental triangle in H, ha,b ha,b+1 ha+1,b+1 P. Doolan, S. Kim 27 h0,0 χ (3) 1 z (3) 1 h0,1 y (1) 1 h1,1 χ (3) 2 z (2) 1 χ (2) 1 z (3) 2 h0,2 y (2) 1 h1,2 y (2) 2 h2,2 χ (3) 3 z (1) 1 χ (2) 2 z (2) 2 χ (1) 1 z (3) 3 h0,3 y (3) 1 h1,3 y (3) 2 h2,3 y (3) 3 h3,3 Figure 1. A h-array and its three derived t-arrays. the entries of the derived t-arrays (x (i) j ), (y (i) j ), and (z (i) j ) are x (n−a) b+1−a = ha,b+1 − ha,b (SW–NE direction) y (b+1) a+1 = ha+1,b+1 − ha,b+1 (E–W direction) (2) z (n+a−b) a+1 = ha+1,b+1 − ha,b (SE–NW direction) for 0 6 a 6 b 6 n− 1. This rather involved indexing is to make the entries of the derived arrays compatible with those of GT patterns. We may visualize the derived t-arrays by placing their entries between the entries of the h-array used to compute them. For example, if n = 3, then a h-array and its three derived t-arrays may be drawn as Figure 1. 2.5. The rhombus conditions for h-arrays are closely related to the interlacing conditions for their derived t-arrays. Proposition 1. Let Tk = Tk(H) be a derived t-array of a h-array H for k = 1, 2, 3. 1) H satisfies RC(1) if and only if T1 satisfies IC(2) and T2 satisfies IC(1). 2) H satisfies RC(2) if and only if T1 and T3 satisfy IC(1). 3) H satisfies RC(3) if and only if T2 and T3 satisfy IC(2). 4) T3 satisfies IC(1) if and only if T1 satisfies IC(1). 5) T3 satisfies IC(2) if and only if T2 satisfies IC(2). 28 The Littlewood-Richardson rule Proof. Let us consider five adjacent entries of H of the forms Z1 Z3 Y1 W1 Y2 W2 Y3 W3 X1 V1 , X2 V2 U2, V3 U3. Then, in the first and the third ones, RC(2) says that Yi +Wi > Zi +Vi for i = 1 and 3. This is equivalent to Y1−Z1 > V1−W1 andW3−Z3 > V3−Y3, which are IC(1) for T1 and T3, respectively. This proves the statement (2). The statements (1) and (3) can be shown similarly. Next, let us consider fundamental rhombi of the following forms in H K L N P S M , Q R. Note that N − K > M − L if and only if L − K > M − N , which proves (4). Similarly, P −Q > S−R if and only if P −S > Q−R, which proves (5). Suppose a h-array H satisfies RC(1), RC(2), and RC(3). Then, by the statements (1) and (2) of Proposition 1, T1(H) satisfies IC(1) and IC(2). Similarly, by the statements (1) and (3), T2(H) satisfies IC(1) and IC(2). This shows that T1(H) and T2(H) are GT patterns. Conversely, if T1(H) and T2(H) are GT patterns, then, by the statements (4) and (5), T3(H) is also a GT pattern. This means all three derived t-arrays satisfy both IC(1) and IC(2), and therefore, from the statements (1), (2), and (3), H is a hive. Theorem 1. For a h-array H ∈ Z (n+1)(n+2)/2 and its derived t-arrays T1(H) and T2(H), H is a hive if and only if T1(H) and T2(H) are GT patterns for GLn. We remark that, in the above result, T1(H) and T2(H) are not in- dependent. Let T1 = (x (i) j ) and T2 = (y (i) j ) be the derived t-arrays of a h-array H. Then, for each rhombus of the form B A C D P. Doolan, S. Kim 29 we have (D − C) + (C −B) = (D −A) + (A−B), or (C −B) − (D −A) = (A−B) − (D − C) which is, using (2), x (n−a−1) b−a − x (n−a) b+1−a = y (b+1) a+1 − y (b) a+1 (3) for 0 6 a < b < n. Note that hives (respectively, GT patterns) for GLn with non-negative entries form a subsemigroup of Z (n+1)(n+2)/2 >0 (respectively, Z n(n+1)/2 >0 ). Theorem 1 and (3) imply that the semigroup ⋃ (µ,ν,λ) H◦(µ, ν, λ) of hives is a fiber product of, over Z n(n−1)/2 >0 , two affine semigroups S1 GT and S2 GT of GT patterns with respect to φk : Sk GT −→ Z n(n−1)/2 >0 such that, for 0 6 a < b < n, φ1(T1) = ( . . . , x (n−a−1) b−a − x (n−a) b+1−a, . . . ) , φ2(T2) = ( . . . , y (b+1) a+1 − y (b) a+1, . . . ) where T1 = (x (i) j ) ∈ S1 GT and T2 = (y (i) j ) ∈ S2 GT . We also remark that by exchanging the roles of T1(H), T2(H) and T3(H), one can read the symmetry of the LR rule. See, for example, [28]. 3. Hives and GT patterns II In this section, we study the set H◦(µ, ν, λ) of hives with a given boundary condition in terms of a single GT pattern. 3.1. Gelfand and Zelevinsky counted the LR number cλ µ,ν with GT patterns of type µ and weight λ− ν satisfying the following additional condition. Lemma 1 ([11]). For a t-array T = (t (i) j ) ∈ Z n(n+1)/2, we define its exponents as ε (i) j (T ) = ∑ 16h<j (t (i+1) h − 2t (i) h + t (i−1) h ) + (t (i+1) j − t (i) j ). 30 The Littlewood-Richardson rule Then the cardinality of the set GZ(µ, λ − ν, ν) of all GT patterns T of type µ with weight λ− ν such that, for all i and j, ε (i) j (T ) 6 νi − νi+1 is equal to the LR number cλ µ,ν . The elements of GZ(µ, λ− ν, ν) will be called GZ schemes. 3.2. Note that, for a h-array H, since the derived t-arrays are defined from the differences of the entries in H, if the boundaries of H are fixed, then any one of the derived t-array of H uniquely determines H. Moreover, we can characterize the derived t-arrays as follows. Theorem 2. For a h-array H in H(µ, ν, λ), consider its derived t-arrays T1(H) and T2(H). 1) H is a hive if and only if T ∗ 1 (H) = (T1(H))∗ is a GZ scheme in GZ(µ∗, λ∗ − ν∗, ν∗); 2) H is a hive if and only if T2(H) is a GZ scheme in GZ(ν, λ−µ, µ). Note that this theorem, in particular, gives bijections between hives and GZ schemes: H◦(µ, ν, λ) −→ GZ(µ∗, λ∗ − ν∗, ν∗) H 7−→ T ∗ 1 (H) and H◦(µ, ν, λ) −→ GZ(ν, λ− µ, µ) H 7−→ T2(H) . For the rest of this section, we will prove Theorem 2 by showing the following. (a) T ∗ 1 (H) satisfies IC(2) if and only if ε (i) j (T2(H)) 6 µi − µi+1; (b) T ∗ 1 (H) satisfies IC(1) if and only if T2(H) satisfies IC(1); (c) T ∗ 1 (H) satisfies ε (i) j (T ∗ 1 (H)) 6 ν∗ i −ν∗ i+1 if and only if T2(H) satisfies IC(2). The weights of the derived t arrays will also be computed. 3.3. Let us first compute the weights of T1(H) and T2(H) for H ∈ H(µ, ν, λ). Lemma 2. For a h-array H = (ha,b) ∈ H(µ, ν, λ), P. Doolan, S. Kim 31 1) the weight of T1(H) is ν∗ − λ∗, i.e., (λn − νn, λn−1 − νn−1, . . . , λ1 − ν1) therefore, the weight of T ∗ 1 (H) is λ∗ − ν∗; 2) the weight of T2(H) is λ− µ, i.e., (λ1 − µ1, λ2 − µ2, . . . , λn − µn). Proof. We will prove the second statement. The proof of the first case is similar. From Definition 3, (2) and the expressions for λ and µ in terms of the h-array elements it follows w1 = y (1) 1 = h1,1 − h0,1 = (h1,1 − h0,0) + (h0,0 − h0,1) = λ1 − µ1. Using the same approach for wi, i > 2, we see wi = i ∑ k=1 y (i) k − i−1 ∑ k=1 y (i−1) k = i ∑ k=1 (hk,i − hk−1,i) − i−1 ∑ k=1 (hk,i−1 − hk−1,i−1) = (hi,i − h0,i) − (hi−1,i−1 − h0,i−1) = λi − µi. Therefore wi = λi − µi for all i, and the weight of T2(H) is λ− µ. 3.4. Next, we study the relations between the interlacing conditions and the exponents conditions for derived arrays. Note that, from the definition of dual arrays, a t-array T satisfies IC(1) if and only if T ∗ satisfies IC(2), and T satisfies IC(2) if and only if T ∗ satisfies IC(1). Proposition 2. For a h-array H = (ha,b) ∈ H(µ, ν, λ) and its derived t-arrays T1(H) = (x (i) j ) and T2(H) = (y (i) j ), T1(H) satisfies IC(1) if and only if ε (i) j (T2(H)) 6 µi − µi+1. Proof. Let us assume j > 1. Then the exponent of T2(H), ε (i) j (T2(H)) = ∑ 16h<j ( (y (i+1) h − y (i) h ) − (y (i) h − y (i−1) h ) ) + ( y (i+1) j − y (i) j ) 32 The Littlewood-Richardson rule can be rewritten in terms of the entries of T1(H). By using (3), ε (i) j (T2(H)) = ∑ 16h<j ( (x (n−h) i−h+1 − x (n−h+1) i−h+2 ) − (x (n−h) i−h − x (n−h+1) i−h+1 ) ) + ( x (n−j) i−j+1 − x (n−j+1) i−j+2 + y (i) j ) − ( x (n−j) i−j − x (n−j+1) i−j+1 + y (i−1) j ) and we see that parts of the consecutive terms cancel to give ε (i) j (T2(H)) = ( x (n) i − x (n) i+1 ) + ( x (n−j) i−j+1 − x (n−j) i−j + y (i) j − y (i−1) j ) . (4) Now note that the interlacing condition IC(1) for T1(H) implies x (n−j+1) i−j+1 > x (n−j) i−j+1 or equivalently, by using (3), x (n−j) i−j > ( x (n−j) i−j+1 + y (i) j − y (i−1) j ) therefore 0 > ( x (n−j) i−j+1 − x (n−j) i−j + y (i) j − y (i−1) j ) . Hence, from (4), the interlacing condition IC(1) for T1(H) is equivalent to ε (i) j (T2(H)) 6 ( x (n) i − x (n) i+1 ) = µi − µi+1. The case j = 1 can be shown similarly for all i. Proposition 3. For a h-array H = (ha,b) ∈ H(µ, ν, λ) and its derived t-arrays T1(H) = (x (i) j ) and T2(H) = (y (i) j ), T1(H) satisfies IC(2) if and only if T2(H) satisfies IC(1). Proof. Using the equality (3), ( x (i) j > x (i+1) j+1 ) if and only if ( y (n−i+j) n−i > y (n−i+j−1) n−i ) and therefore, by setting i′ = n− i+ j − 1 and j′ = n− i, we have ( x (i) j > x (i+1) j+1 ) if and only if ( y (i′+1) j′ > y (i′) j′ ) for 1 6 j 6 i 6 n − 1 and 1 6 j′ 6 i′ 6 n − 1. This shows that IC(2) holds for T1(H) if and only if IC(1) holds for T2(H). Proposition 4. For a h-array H = (ha,b) ∈ H(µ, ν, λ) and its derived t- arrays T1(H) = (x (i) j ) and T2(H) = (y (i) j ), T ∗ 1 (H) satisfies ε (i) j (T ∗ 1 (H)) 6 ν∗ i − ν∗ i+1 if and only if T2(H) satisfies IC(2). P. Doolan, S. Kim 33 Proof. Let us assume j > 1. Write the exponents of T ∗ 1 (H) = (s (i) j ) using s (i) j = −x (i) i+1−j . ε (i) j (T ∗ 1 (H)) = ∑ 16h<j ( −x (i+1) i−h+2 + 2x (i) i−h+1 − x (i−1) i−h ) + ( −x (i+1) i−j+2 + x (i) i−j+1 ) = ∑ 16h<j ( (x (i) i−h+1 − x (i+1) i−h+2) − (x (i−1) i−h − x (i) i−h+1) ) + ( x (i) i−j+1 − x (i+1) i−j+2 ) Then, using the identity (3), we can rewrite the exponents in terms of the entries of T2(H) as ε (i) j (T ∗ 1 (H)) = ∑ 16h<j ( (y (n−h+1) n−i − y (n−h) n−i ) − (y (n−h+1) n−i+1 − y (n−h) n−i+1) ) + ( y (n−j+1) n−i − y (n−j) n−i ) 6 ∑ 16h<j ( (y (n−h+1) n−i − y (n−h) n−i ) − (y (n−h+1) n−i+1 − y (n−h) n−i+1) ) + ( y (n−j+1) n−i − y (n−j+1) n−i+1 ) where the inequality is by IC(2): y (n−j) n−i > y (n−j+1) n−i+1 in T2(H). Parts of the consecutive terms in the right hand side cancel to give ε (i) j (T ∗ 1 (H)) 6 ( (y (n) n−i − y (n−j+1) n−i ) − (y (n) n−i+1 − y (n−j+1) n−i+1 ) ) + ( y (n−j+1) n−i − y (n−j+1) n−i+1 ) = ( y (n) n−i − y (n) n−i+1 ) = νn−i − νn−i+1 = ν∗ i − ν∗ i+1. So the interlacing condition IC(2) for T2(H) is equivalent to ε (i) j (T ∗ 1 (H)) 6 ν∗ i − ν∗ i+1 as required. The case j = 1 can be shown similarly for all i. 3.5. Suppose we have a hive H. From Lemma 2, the weights of T ∗ 1 (H) and T2(H) are λ∗ −ν∗ and λ−µ, respectively. Theorem 1 states that H is a hive if and only if T1(H) and T2(H), and hence T ∗ 1 (H) and T2(H), satisfy both IC(1) and IC(2). Therefore since H is a hive, Proposition 2 and 34 The Littlewood-Richardson rule Proposition 4 imply T ∗ 1 (H) and T2(H) satisfy the exponent conditions, and consequently they are GZ schemes in GZ(µ∗, λ∗ − ν∗, ν∗) and GZ(ν, λ− µ, µ), respectively. Conversely, if T ∗ 1 (H) is a GZ scheme from GZ(µ∗, λ∗−ν∗, ν∗) it satisfies IC(1), IC(2), and the exponent condition, thus from Propositions 2 – 4, T2(H) is a GZ scheme. In particular, T1(H) and T2(H) are GT patterns, meaning H is a hive by Theorem 1. Similarly, if T2(H) ∈ GZ(ν, λ− µ, µ), then H is a hive. This proves Theorem 2. 4. LR tableaux and GT patterns I In this section we introduce a bijection between LR tableaux and GZ schemes (Theorem 3). In proving this we will see that the semistandard and Yamanouchi conditions for tableaux are equivalent to, respectively, the interlacing and exponent conditions for t-arrays. As an interesting consequence we then combine Theorem 3 with Theorem 2 (1) to arrive at a correspondence between LR tableaux and hives (Corollary 1). It turns out that Corollary 1 is equivalent to [18, (3.3)], so we compare the two constructions. The main difference is that our method has an intermediate GZ scheme, which is an artefact of composing Theorem 3 and Theorem 2. To conclude the section we summarise how the conditions on LR tableaux (semistandard and Yamanouchi conditions), GZ schemes (semistandard and exponent conditions) and hives (the rhombus conditions) are translated by the bijections. The reader may find relevant results and further developments in, for example, [1–4,6, 18,19,25]. 4.1. A well-known bijection between semistandard tableaux and GT patterns. Our bijection between LR tableaux and GZ schemes is an extension of a well-known bijection between semistandard tableaux and GT patterns, seen in, for example, [11]. We now review this bijection and state it in the form most useful for our purposes. For this we require some relevant notation. A non-skew semistandard tableau Y is uniquely determined by its associated matrix (ai,j(Y )) where ai,j(Y ) = the number of i’s in the jth row (5) for all 1 6 i, j 6 n. Note that ai,j(Y ) = 0 for i < j. We also note that ∑n k=1 ak,j(Y ) for 1 6 j 6 n give the shape of the tableau Y , and ∑n k=1 ai,k(Y ) for 1 6 i 6 n give the content of Y . The reader is warned P. Doolan, S. Kim 35 that these are not the same aij as those in [18, (3.4)]. Those label hive entries, not content of a tableau. We remark that if Y is a semistandard tableau on the skew shape λ/µ, then the ai,j(Y )’s are well defined, and the ai,j(Y )’s with λ or µ uniquely define Y . It is possible to develop the theory of tableaux exclusively in terms of their associated matrices. See [6] for this direction. Now consider a semistandard Young tableau. Removing all instances of the largest entry simultaneously yields a tableau with a new shape. Repeating this process, we would achieve a list of successively shrinking shapes, which written downwards would form the rows of a GT pattern. This process is a bijection. See Example 1. It is easy to symbolically describe the inverse of the bijection. Given a GT pattern T = (t (i) j ) of type λ with non-negative entries, it creates a semistandard Young tableau YT of shape λ whose entries are elements of {1, 2, . . . , n} and defined by ai,j(YT ) = t (i) j − t (i−1) j (6) for 1 6 i, j 6 n with the conventions t (i) j = 0 for j > i > 0. Manipulating (6), it follows that the bijection takes a semistandard tableau Y and creates a GT pattern TY = (t (i) j ) according to the rule t (i) j = i ∑ k=1 ak,j(Y ) (7) for 1 6 j 6 i 6 n. Since ak,j(Y ) = 0 for k < j in every non-skew semistandard tableau Y , we can in fact write this as t (i) j = i ∑ k=j ak,j(Y ). (8) See also, for example, [14, §8.1.2] or [20] for further background on this bijection. Example 1. As an example we apply the bijection to the tableau 1 1 2 2 3 3 36 The Littlewood-Richardson rule and list the successive shapes λ(i) as they are created. 1 1 2 2 3 3 = (0) = 3, 2, 1 1 1 2 2 (0) = 3, 2, 1 (1) = 3, 1 1 1 (0) = 3, 2, 1 (1) = 3, 1 (2) = 2 Clearly, the shapes form a GT pattern. It is straightforward to check that the expressions (8) and (6) both hold. Under this bijection, the content of the tableau is equal to the weight of the t-array. We also note that in this bijection, the semistandard condition on the tableau is implied by the interlacing conditions on the t-array and vice versa (cf. Remark 2). 4.2. A well-known bijection between semistandard skew tableaux and truncated GT patterns. The bijection of §4.1 can be extended to act on skew tableaux. Again, this is a well known result included in [11], [12] and [3], among others. Lemma 3. There is a bijection between the set of skew semistandard Young tableaux of shape λ/µ with entries from {1, 2, . . . , n} and the set of GT patterns for GL2n whose type is λ′ = (λ1, . . . , λn, 0, · · · , 0) ∈ Z 2n and whose kth row is (µ1, µ2, . . . , µk) for 1 6 k 6 n. Proof. For a given semistandard Young tableau Y of shape λ/µ, replace the i entries with (n+i)’s for 1 6 i 6 n, then fill in the empty boxes in the ℓth row of Y with ℓ’s for 1 6 ℓ 6 n. Then this process uniquely determines a non-skew semistandard Young tableau of shape λ with entries from {1, 2, . . . , 2n}, and under the bijection given by (6), its corresponding GT pattern for GL2n is the one described in the statement. The first half of Example 2 shows Lemma 3 applied to a skew tableau. We remark that the GT pattern for GLn whose kth row is (µ1, µ2, . . . , µk) for 1 6 k 6 n corresponds to the highest weight vector of the repre- sentation V µ n labelled by a Young diagram µ. In fact, the GT patterns described in Lemma 3 encode the weight vectors of V λ′ 2n , which are the highest weight vector for V µ n under the branching of GL2n down to GLn. The bottom n− 1 rows of a GT pattern described by Lemma 3 hold redundant information because they are determined by µ. It is therefore convention to omit them and achieve what is called a truncated GT pattern. It is also common to omit the upper-right portion of this pattern, P. Doolan, S. Kim 37 since the interlacing conditions force those entries to be zero. For example, the first half of the bijection described by [18, (3.3)] uses Lemma 3 with these conventions. There is an excellent example of Lemma 3 and further explanation in [1, §2]. 4.3. Symbolic forms of the semistandard and Yamanouchi con- ditions. We are almost ready to use Lemma 3 to establish the bijection between LR tableaux and GZ schemes. However, we first need symbolic forms of both the semistandard and Yamanouchi conditions. Let us express the semistandard condition for a tableau Y in terms of the ai,j(Y ) defined in (5). By rearranging the entries in each row if necessary, we can always make the entries of Y weakly increasing along each row from left to right. The strictly increasing condition on the columns of Y can then be rephrased as follows: the number of entries up to ℓ in the (m+ 1)th row is not bigger than the number of entries up to (ℓ− 1) in the mth row, i.e., ℓ−1 ∑ k=1 ak,m(Y ) > ℓ ∑ k=1 ak,m+1(Y ) (9) for 1 6 ℓ 6 n and 1 6 m < n. Here, if ℓ = 1, then the left hand side is 0 as an empty sum and the inequality implies that a1,m+1(Y ) = 0 for m > 1. Inductively, we can obtain ai,m+1(Y ) = 0 for m > i from the inequality with ℓ = i. This shows that for a semistandard Young tableau Y, ai,j(Y ) = 0 for j > i, as we noted after (5). Remark 2. By using the conversion formula (7), one can directly compute that IC(2) on a GT pattern T is equivalent to the semistandard condition (9) in YT corresponding to T . On the other hand, IC(1) in T is equivalent to a rather trivial condition ai,j(YT ) > 0 for all i, j. If Y is a skew tableau of shape λ/µ, then, using the same argument as for (9), it is straightforward to see that we can make Y semistandard by rearranging elements along each row if and only if µm+1 + ℓ ∑ k=1 ak,m+1(Y ) 6 µm + ℓ−1 ∑ k=1 ak,m(Y ) (10) for 1 6 ℓ 6 n and 1 6 m < n. The Yamanouchi condition in a LR tableau Y can be expressed as j ∑ k=1 ai+1,k(Y ) 6 j−1 ∑ k=1 ai,k(Y ) (11) 38 The Littlewood-Richardson rule for 1 6 j 6 n and 1 6 i < n. Here, if j = 1, then the right hand side is 0 as an empty sum and the inequality implies that ai+1,1(Y ) = 0 for i > 1. Inductively, we can obtain ai+1,ℓ(Y ) = 0 for i > ℓ from the inequality with j = ℓ. This shows that for an LR tableau Y, ai,j(Y ) = 0 for i > j, as we noted in Remark 1 (2). 4.4. Bijection between LR tableaux and GZ schemes. We now establish a bijection between LR tableaux and GZ schemes using Lemma 3. After applying the lemma to an LR tableau, a center section of the resulting GT pattern is removed. Taking the dual of the removed array we get the desired GZ scheme. In doing this we observe how the conditions on the tableau become those of the scheme. For a specific example of this bijection, see the first half of Example 2. Theorem 3. There is a bijection φ between LR(λ/µ, ν) and GZ(µ∗, λ∗ − ν∗, ν∗). In particular, the semistandard and Yamanouchi conditions in L ∈ LR(λ/µ, ν) are equivalent to, respectively, the interlacing and exponent conditions in φ(L) ∈ GZ(µ∗, λ∗ − ν∗, ν∗). Proof. Let L ∈ LR(λ/µ, ν) be given. By applying Lemma 3 we find its corresponding GT pattern T = (t (i) j ) for GL2n and remove the bottom n− 1 rows to achieve a truncated GT pattern of n+ 1 rows. Furthermore, the truncated pattern for L can be divided into three subtriangular arrays TX , TY and TZ , as in Figure 2. Note that these are the same size. TZ TYTX Figure 2. Dividing a truncated GT pattern into 3 subpatterns. The upper left subarray TX is completely determined by λ because of the Yamanouchi condition (see Remark 1 (2)). The upper right subarray TY contains only zeroes. Therefore, given fixed λ, µ, and ν, the LR tableau L ∈ LR(λ/µ, ν) is uniquely determined by TZ . We want to show that the dual array T ∗ Z of TZ is an element of GZ(µ∗, λ∗ − ν∗, ν∗), and from that P. Doolan, S. Kim 39 establish a bijection LR(λ/µ, ν) −→ GZ(µ∗, λ∗ − ν∗, ν∗) L 7−→ T ∗ Z . Let us rewrite the middle subarray TZ as follows by reflecting it over a horizontal line. TZ = t (n) 1 t (n) 2 · · · t (n) n−1 t (n) n t (n+1) 2 t (n+1) 3 · · · t (n+1) n t (n+2) 3 t (n+2) n . . . . . . t (2n−1) n Then µi = t (n) i for 1 6 i 6 n and TZ satisfies the interlacing conditions induced from the truncated GT pattern T , which are assured by the semistandardness of L. Therefore TZ is a GT pattern of type µ. From the fact that the weights of TX , TY , and T are (λ1, . . . , λn), (0, . . . , 0), and (µ1, . . . , µn, ν1, . . . , νn) respectively, it is easy to show that the weight of TZ is ν∗ − λ∗. Hence its dual T ∗ Z is a GT pattern (see §3.4) of type µ∗ and weight λ∗ − ν∗. Next, we want to show that T ∗ Z satisfies the exponent conditions. Let ai,j = ai,j(L), i.e., be the number of i’s in the jth row of L for all i and j. Then ai,j = t (n+i) j − t (n+i−1) j and ak,k = λk − t (n+k−1) k (12) for 1 6 i < j 6 n and 1 6 k 6 n. Since the content of L is ν with νq = ∑n k=1 aq,k for 1 6 q 6 n, we can write (−νi+1) − (−νi) = n ∑ k=1 (ai,k − ai+1,k) (13) for 1 6 i < n. On the other hand, from the Yamanouchi condition (11) in L, we have j ∑ k=1 ai+1,k 6 j−1 ∑ k=1 ai,k or equivalently, ai+1,j 6 j−1 ∑ k=1 (ai,k − ai+1,k). Then, using this inequality, (13) becomes (−νi+1) − (−νi) > n ∑ k=j+1 (ai,k − ai+1,k) + ai,j 40 The Littlewood-Richardson rule and the right hand side is, via (12), the exponents of T ∗ Z . Therefore, T ∗ Z ∈ GZ(µ∗, λ∗ − ν∗, ν∗). 4.5. A bijection between LR tableaux and hives. Composing Theorem 3 and Theorem 2 (1) gives a bijection between the set of LR tableaux and the set of hives. GZ(µ∗, λ∗ − ν∗, ν∗) ւր ցտ LR(λ/µ, ν) H◦(µ, ν, λ) Corollary 1. [18, (3.3)] There is a bijection between LR(λ/µ, ν) and H◦(µ, ν, λ). Proof. For L ∈ LR(λ/µ, ν), we compute the corresponding truncated GT pattern and its middle subarray TZ . Then, by Theorem 3, its dual T ∗ Z belongs to GZ(µ∗, λ∗ − ν∗, ν∗). Similarly, for H ∈ H◦(µ, ν, λ), its first derived subarray T1(H) satisfies T ∗ 1 (H) ∈ GZ(µ∗, λ∗ − ν∗, ν∗) by Theorem 2. We can therefore identify a H such that T1(H) = TZ and this gives us a bijection from LR(λ/µ, ν) to H◦(µ, ν, λ). We give an example of Corollary 1 below. Example 2. We start by using Theorem 3 to map the LR tableau below to a GT pattern (whose dual array is a GZ scheme). Let λ = (11, 7, 5, 3), µ = (5, 3, 1, 0) and ν = (7, 5, 3, 2). The LR tableau from LR(λ/µ, ν) 1 1 1 1 1 1 1 2 2 2 2 3 3 3 2 4 4 considered as an object for GL4, corresponds to the following truncated GT pattern. 11 7 5 3 0 0 0 0 11 7 5 1 0 0 0 11 7 2 1 0 0 11 4 1 0 0 5 3 1 0 P. Doolan, S. Kim 41 Taking out the middle section, we find TZ is 5 3 1 0 4 1 0 2 1 1 with a dual array T ∗ Z belonging to GZ(µ∗, λ∗ − ν∗, ν∗). For the second half of the process, we apply the bijection between hives and GZ schemes (Theorem 2 (1)) to T ∗ Z . We know the corresponding hive H will have boundaries given by µ = (5, 3, 1, 0), ν = (7, 5, 3, 2) and λ = (11, 7, 5, 3) so that it appears as follows 0 5 11 8 p 18 9 q r 23 9 16 21 24 26 with some inner entries p, q and r. Adding (T ∗ Z)∗ = TZ along the NE-SW diagonals as if it were T1(H) we find p = 15, q = 16 and r = 20. Of course, there are many known bijections between LR tableaux and hives. For example, in the appendix of [5] Fulton gave a bijection between LR tableaux and hives using contratableaux. It is interesting to note that his first step is to construct partitions from the hive that are equivalent to the derived t-array T1. However, that approach diverges from ours once he uses the partitions to form a contratableau. Our Corollary 1 is simpler than most other bijections between LR tableaux and hives, such as the one by Fulton, but is in fact equivalent to [18, (3.3)]. There, the authors also take an LR tableau and compute the truncated GT pattern via Lemma 3. They then take row sums in the pattern and separate out a bottom section, which becomes the hive. This is simply our process in reverse, since we separate a section of the truncated GT pattern in Theorem 3 by removing TZ , and then successively add those entries to the boundary of the hive in Theorem 2 (1). The key difference, however, is that here we establish GZ schemes as an intermediate object in the bijection, which is absent from the simple and elegant treatment in [18]. This provides background as to why their simple bijection works, and also allows us to track the conditions as they move between objects (see tables 1 and 2). We also note that Corollary 42 The Littlewood-Richardson rule 1 is not the main focus of our discussion. Rather, it is an interesting consequence that appears when piecing together two sets of combinatorial theory – the derived t-arrays of hives on one hand, and the classical bijection between tableaux and t-arrays on the other. To complete the section we combine the two approaches for some insights. Though not clear from our presentation, the elegant formula [18, (3.4)] states that the elements of the hive H = (hl,m) are given by hl,m = the number of empty boxes and entries 6 l in the first m rows of the LR tableau. Finally, in proving [18, Proposition 3.2], King et al. show that, under their bijection, conditions1 on hives correspond to conditions on LR tableaux. Table 1 summarises these equivalences. Hive LR tableau RC(1) trivial RC(2) Semistandard condition RC(3) Yamanouchi Table 1. Equivalent LR tableau and hive conditions in [18, (3.3)] Using our results from Proposition 1, Theorem 2, Remark 2 and Theorem 3 we are able to add a middle column showing the equivalent conditions in the intermediate GZ scheme object. See Table 2. Hive GZ scheme LR tableau RC(1) IC(1) trivial RC(2) IC(2) Semistandard condition RC(3) Exponents Yamanouchi Table 2. Equivalent LR tableau, GZ scheme and hive conditions in Corollary 1 5. LR Tableaux and GT Patterns II In this section, we show that the semistandard and Yamanouchi conditions for tableaux are equivalent to, respectively, the exponent and semistandard conditions for their companion tableaux. This correspondence 1The conditions RC(1), RC(2) and RC(3) are referred to as R2, R3 and R1 respec- tively by [18]. P. Doolan, S. Kim 43 is obtained by taking the transpose of matrices describing tableaux. As a result, we show that the companion tableaux of LR tableaux are GZ schemes under the tableau-pattern bijection. 5.1. For a (skew) semistandard tableau Y , as in (5), we let ai,j(Y ) denote the number of i’s in the jth row. Definition 5. For a (skew) semistandard tableau Y , its companion tableau Y c is defined as a non-skew tableau whose entries are weakly increasing along each row and whose number of i’s in the jth row is equal to aj,i(Y ); that is, for 1 6 i, j 6 n, ai,j(Y c) = aj,i(Y ). (14) Example 3. For the LR tableau Y from Example 2, the associated matrix is ai,j(Y ) =      6 1 0 0 0 3 1 1 0 0 3 0 0 0 0 2      . Then, from its transpose, we have the following companion tableau Y c. 1 1 1 1 1 1 2 2 2 2 3 4 3 3 3 4 4 Note that Y is of shape (11, 7, 5, 3)/(5, 3, 1, 0) and content (7, 5, 3, 2) while its companion tableau Y c is of shape (7, 5, 3, 2) and content (6, 4, 4, 3), which is (11, 7, 5, 3) − (5, 3, 1, 0). The GT pattern TY c corresponding to Y c is 7 5 3 2 7 4 3 7 3 6 . We want to show that this correspondence Y 7→ TY c gives another bijection from the set of LR tableaux to the set of GZ schemes. In [29], van Leeuwen replaced the Yamanouchi condition in LR tableaux with the semistandard condition in their companion tableaux. Here, we show that the semistandard condition in LR tableaux has a counterpart in the companion tableaux as well, and then we identify the companion tableaux as an independent object equivalent to GZ schemes. 44 The Littlewood-Richardson rule Theorem 4. For a LR tableau Y , we let Y c denote its companion tableau and let TY c denote the GT pattern corresponding to Y c. The map ψ(Y ) = TY c gives a bijection from LR(λ/µ, ν) to GZ(ν, λ− µ, µ). In particular, the Yamanouchi and semistandard conditions in Y are equivalent to, respectively, the interlacing condition IC(2) and the exponent condition in TY c. Proof. From (14), Y is a tableau of shape λ/µ if and only if the content of Y c is equal to λ−µ. The content of Y is equal to the shape of Y c. The type and weight of TY c are therefore ν and λ− µ, respectively. Recall the Yamanouchi condition in Y (11): for 0 6 i < n and 1 6 j < n, i ∑ k=1 aj,k(Y ) > i+1 ∑ k=1 aj+1,k(Y ). (15) Since ai,j(Y ) = aj,i(Y c) for all i and j, this inequality, in terms of the entries in Y c, is saying that the number of entries less than or equal to i+ 1 in the (j+ 1)th row is not more than the number of entries less than or equal to i in the jth row. It is the semistandard condition for Y c and therefore the interlacing condition for TY c . To show this, consider expressing the elements of the GT pattern TY c = (t (i) j ) in terms of ai,j(Y c). From the standard bijection between semistandard tableaux and GT patterns, (7), we have t (i) j = i ∑ k=1 ak,j(Y c) where ai,j(Y c) is the number of i entries in the jth row of Y c. Consider the interlacing condition IC(2): t (i) j > t (i+1) j+1 where 0 6 i < n and 1 6 j < n. Writing this with the above relation gives i ∑ k=1 ak,j(Y c) > i+1 ∑ k=1 ak,j+1(Y c) ⇔ i ∑ k=1 aj,k(Y ) > i+1 ∑ k=1 aj+1,k(Y ) which is exactly the expression for the Yamanouchi condition (15). It can be similarly shown that, as mentioned in Remark 2, IC(1) is equivalent to ai,j(Y ) > 0. Using (10), the semistandard condition for Y says we have, for all 1 6 ℓ 6 n and 1 6 m < n, ( ℓ ∑ k=1 ak,m+1(Y ) − ℓ−1 ∑ k=1 ak,m(Y ) ) 6 (µm − µm+1) (16) P. Doolan, S. Kim 45 or ℓ−1 ∑ k=1 (am+1,k(Y c) − am,k(Y c)) + am+1,ℓ(Y c) 6 (µm − µm+1) . To finish our proof, it is enough to show that the left hand side of the above inequality is the exponent ε (m) ℓ (TY c). This can be easily seen, by using (8), as ε (m) ℓ (TY c) = ∑ 16h<ℓ ( t (m+1) h − 2t (m) h + t (m−1) h ) + ( t (m+1) ℓ − t (m) ℓ ) = ∑ 16h<ℓ ( m+1 ∑ k=h ak,h(Y c) − 2 m ∑ k=h ak,h(Y c) + m−1 ∑ k=h ak,h(Y c) ) + ( m+1 ∑ k=ℓ ak,ℓ(Y c) − m ∑ k=ℓ ak,ℓ(Y c) ) = ∑ 16k<ℓ (am+1,k(Y c) − am,k(Y c)) + am+1,ℓ(Y c). We now have an alternative proof of Corollary 1. Corollary 2. There is a bijection between LR(λ/µ, ν) and H◦(µ, ν, λ). Proof. We can map any Y ∈ LR(λ/µ, ν) to TY c ∈ GZ(ν, λ − µ, µ) via the bijection in Theorem 4. 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Thomas and A. Yong, An S3-symmetric Littlewood-Richardson rule. Math. Res. Lett. 15 (2008), no. 5, 1027–1037. [29] M.A.A. van Leeuwen, The Littlewood-Richardson rule, and related combinatorics. Interaction of combinatorics and representation theory, 95–145, MSJ Mem., 11, Math. Soc. Japan, Tokyo, 2001. Contact information Patrick Doolan School of Mathematics and Physics The University of Queensland St Lucia, QLD 4072, Australia E-Mail(s): patrick.doolan@uqconnect.edu.au Sangjib Kim Department of Mathematics Korea University 145 Anam-ro, Seongbuk-gu, Seoul, 02841, South Korea E-Mail(s): sk23@korea.ac.kr Received by the editors: 22.09.2015 and in final form 04.10.2015.