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Combinatorial formulas for shifted dual stable Grothendieck polynomials

Published online by Cambridge University Press:  13 February 2024

Joel Lewis
Affiliation:
Department of Mathematics, George Washington University, 801 22nd St. NW, Washington, DC 20852; E-mail: jblewis@gwu.edu
Eric Marberg
Affiliation:
Department of Mathematics, Hong Kong University of Science and Technology, Clear Water Bay, Hong Kong; E-mail: emarberg@ust.hk

Abstract

The K-theoretic Schur P- and Q-functions $G\hspace {-0.2mm}P_\lambda $ and $G\hspace {-0.2mm}Q_\lambda $ may be concretely defined as weight-generating functions for semistandard shifted set-valued tableaux. These symmetric functions are the shifted analogues of stable Grothendieck polynomials and were introduced by Ikeda and Naruse for applications in geometry. Nakagawa and Naruse specified families of dual K-theoretic Schur P- and Q-functions $g\hspace {-0.1mm}p_\lambda $ and $g\hspace {-0.1mm}q_\lambda $ via a Cauchy identity involving $G\hspace {-0.2mm}P_\lambda $ and $G\hspace {-0.2mm}Q_\lambda $. They conjectured that the dual power series are weight-generating functions for certain shifted plane partitions. We prove this conjecture. We also derive a related generating function formula for the images of $g\hspace {-0.1mm}p_\lambda $ and $g\hspace {-0.1mm}q_\lambda $ under the $\omega $ involution of the ring of symmetric functions. This confirms a conjecture of Chiu and the second author. Using these results, we verify a conjecture of Ikeda and Naruse that the $G\hspace {-0.2mm}Q$-functions are a basis for a ring.

Information

Type
Algebra
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 in any medium, provided the original work is properly cited.
Copyright
© The Author(s), 2024. Published by Cambridge University Press
Figure 0

Figure 1 An example computation of $\mathsf {swap}_{1\leftrightarrow 2'}(T)$. We illustrate each individual operation of the form $\mathsf {swap}_{1\leftrightarrow 2'}( -, {\mathcal {V}}, {\mathcal {H}})$ that results in a new tableau (i.e., that does not fall in case (c) of Definition 3.2). The bars ${\mathcal {H}}_1$, ${\mathcal {H}}_2$, ${\mathcal {H}}_3$, ${\mathcal {H}}_4$ and ${\mathcal {H}}_5$ are respectively gray, green, yellow, blue and white; the bars ${\mathcal {V}}_1$, ${\mathcal {V}}_2$ and ${\mathcal {V}}_3$ are respectively orange, pink and red.

Figure 1

Figure 2 An example computation of $\mathsf {unswap}_{1\leftrightarrow 2'}(\tilde T)$. We illustrate each individual operation of the form $\mathsf {unswap}_{1\leftrightarrow 2'}( -, {\mathcal {V}}, {\mathcal {H}})$ that results in a new tableau (i.e., that does not fall in case (c) of Definition 3.6). The bars $\tilde {\mathcal {H}}_1$, $\tilde {\mathcal {H}}_2$, $\tilde {\mathcal {H}}_3$, $\tilde {\mathcal {H}}_4$ and $\tilde {\mathcal {H}}_5$ are respectively gray, green, yellow, blue and white; the bars $\tilde {\mathcal {V}}_1$, $\tilde {\mathcal {V}}_2$ and $\tilde {\mathcal {V}}_3$ are respectively orange, pink and red.

Figure 2

Figure 3 The special cases (C1), (C2)–(C3), and (C4)–(C5) of Definition 3.14.

Figure 3

Figure 4 Case (3) in the proof of Lemma 4.12: the subcase when $n = 1$, $\Psi = \Gamma $. Forced boxes in $\textsf {SD}_{\Lambda / \Psi }$ are denoted by $\bullet $, removable corners of $\textsf {SD}_{\Gamma }$ off the diagonal are denoted by $\times $, and removable corners on the diagonal are denoted by $*$.

Figure 4

Figure 5 Case (3) in the proof of Lemma 4.12: the subcase when $n> 1$, $\Psi \neq (1)$. Left column $i = 0$, right column $i = 1$; top row $j = 0$, bottom row $j = 1$. The blue cells represent $\Psi / \Gamma $.

Figure 5

Figure 6 Case (3) in the proof of Lemma 4.19: the subcase when $n = 1$, $\Psi = \Gamma $. Forced boxes in $\textsf {SD}_{\Lambda / \Psi }$ are denoted by $\bullet $, diagonally-forced boxes are denoted by $\cdot $, and removable corners of $\textsf {SD}_{\Gamma }$ are denoted by $\times $.

Figure 6

Figure 7 Case (3) in the proof of Lemma 4.19: the subcase when $n> 1$. Left column $J = 0$, right column $J = 1$. The blue cells represent $\Psi / \Gamma $.