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Alternating sign matrices with reflective symmetry and plane partitions: $n+3$ pairs of equivalent statistics and a Cauchy-type identity

Published online by Cambridge University Press:  08 October 2025

Ilse Fischer
Affiliation:
Fakultät für Mathematik, Universität Wien , Wien 1090, Austria; E-mail: ilse.fischer@univie.ac.at
Hans Höngesberg*
Affiliation:
Fakulteta za matematiko in fiziko, Univerza v Ljubljani , Ljubljana 1000, Slovenia
*
E-mail: hans.hoengesberg@fmf.uni-lj.si (corresponding author)

Abstract

Vertically symmetric alternating sign matrices (VSASMs) of order $2n+1$ are known to be equinumerous with lozenge tilings of a hexagon with side lengths $2n+2,2n,2n+2,2n,2n+2,2n$ and a central triangular hole of size $2$ that exhibit a cyclical as well as a vertical symmetry, but finding an explicit bijection proving this belongs to the most difficult problems in bijective combinatorics. Towards constructing such a bijection, we generalize the result by introducing certain natural extensions for both objects along with $n+3$ parameters and show that the multivariate generating functions with respect to these parameters coincide. This is a significant step from a constant number of equidistributed statistics to a linear number of statistics in n. The equinumeracy of VSASMs and the lozenge tilings is then an easy consequence of this result, which is obtained by specializing the generating functions to signed enumerations for both types of objects and then applying certain sign-reversing involutions. Another main result concerns the expansion of the multivariate generating function into symplectic characters as a sum over totally symmetric self-complementary plane partitions, which is in perfect analogy to the situation for ordinary ASMs where the Schur expansion can be written as a sum over totally symmetric plane partitions. This is exciting as it is reminiscent of the well-known Cauchy identity, and the Cauchy identity does have a bijective proof using the Robinson-Schensted-Knuth correspondence, and thus the result raises the question of whether there is a variation of the Robinson–Schensted–Knuth correspondence that does eventually lead to a bijective proof.

Information

Type
Discrete Mathematics
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (https://creativecommons.org/licenses/by/4.0), which permits unrestricted re-use, distribution and reproduction, provided the original article is properly cited.
Copyright
© The Author(s), 2025. Published by Cambridge University Press
Figure 0

Figure 1 Cyclically and vertically symmetric lozenge tiling of a hexagon with a central triangular hole and the corresponding family of nonintersecting lattice paths. The gray tilings are forced due to the symmetry.

Figure 1

Figure 2 Example of the lattice paths in Theorem 2.4 for $n=6$. The associated permutation is $\sigma = (1\;2\;3\;6\;4\;5)$ and the weight is $(-u v)^5 w^9 X_1^5 X_2^5 X_3^5 X_4^5 X_5^5 X_6^5(u X_3+v X_3^{-1}) (u X_6 + v X_6^{-1})$. In the second region, we draw the even and odd paths in different colors.

Figure 2

Figure 3 An example of the bijective correspondence between cyclically symmetric lozenge tilings of a holey hexagon and descending plane partitions. The lozenge tiling on the left side is the same as in Figure 1 but rotated by $30^\circ $. The dotted lines mark a third of the lozenge tiling as the fundamental area.

Figure 3

Figure 4 Example of a lattice path interpretation of (4.4) with $i=5$, $j=3$, $p=8$ and $q=6$. The steps contribute the factor $-u v w^2 (u X_1+v X_1^{-1})^2 (u X_3 + v X_3^{-1})$ to the weight of the path. In the second region, the path is even.

Figure 4

Figure 5 Fundamental area $\mathcal {H}_n$.

Figure 5

Figure 6 The different cases of the sign-reversing involution on strongly intersecting paths.

Figure 6

Figure 7 This family of lattice paths corresponds to the pair of CStrPP and RStrPP in Section 2.

Figure 7

Figure 8 Rules for transforming an uncolored B-path into a colored A-path.

Figure 8

Figure 9 The transformation of a B-path into a family of A-paths for $p=5$ and $j=2$.

Figure 9

Figure 10 The transformation of an A-path into a B-path for $p=7$ and $j=2$.

Figure 10

Figure 11 Example of the lattice path interpretation of the left-hand side of (6.2) for $i=5$, $j=3$ and $p=6$. The weight of the path is $(-1)^4=1$.

Figure 11

Figure 12 Sign-reversing involution for $i=4$ and $j=3$.

Figure 12

Figure 13 Example of the lattice paths in Theorem 7.1 for $n=6$. The paths are drawn in alternating colors for a better distinction.

Figure 13

Figure 14 Example of the lattice paths in Theorem 7.3 for $n=4$. The weight of this family of nonintersecting lattice paths is $(-uv)^{3-1} w^2 (u X_1) (u X_2) (u X_{3}) (v X_{3}^{-1}) X_1^3 X_2^3 X_3^3 X_4^3$, which is equal to $u^5 v^3 w^2 X_1^4 X_2^4 X_3^3 X_4^3$.

Figure 14

Figure 15 Example of the lattice path interpretation of (A.10) for $n=6$. The weight of these paths is $u^7 v^9 w^5 X_1^{-2} X_2^{-1} X_3^{-1} X_4 X_5$. Note that this family of nonintersecting lattice paths corresponds to the pair of CStrPP and RStrPP in Section 2.