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Polyhedral realizations for crystal bases and Young walls of classical affine types

Yuki Kanakubo

Abstract

For affine Lie algebra $\mathfrak{g}$ of type $A^{(1)}_{n-1}$, $B^{(1)}_{n-1}$, $C^{(1)}_{n-1}$, $D^{(1)}_{n-1}$, $A^{(2)}_{2n-2}$, $A^{(2)}_{2n-3}$ or $D^{(2)}_{n}$, let $B(λ)$ and $B(\infty)$ be the crystal bases of integrable highest weight representation $V(λ)$ and negative part $U_q^-(\mathfrak{g})$ of quantum group $U_q(\mathfrak{g})$. We consider the polyhedral realizations of crystal bases, which realize $B(λ)$ and $B(\infty)$ as sets of integer points of some polytopes and cones in $\mathbb{R}^{\infty}$. It is a natural problem to find explicit forms of the polytopes and cones. In this paper, we introduce pairs of truncated walls, which are defined as modifications of level $2$-Young walls and describe inequalities defining the polytopes and cones in terms of level $1$-proper Young walls and pairs of truncated walls. As an application, we also give combinatorial descriptions of $\varepsilon_k^*$-functions on $B(\infty)$ in terms of Young walls and truncated walls.

Polyhedral realizations for crystal bases and Young walls of classical affine types

Abstract

For affine Lie algebra of type , , , , , or , let and be the crystal bases of integrable highest weight representation and negative part of quantum group . We consider the polyhedral realizations of crystal bases, which realize and as sets of integer points of some polytopes and cones in . It is a natural problem to find explicit forms of the polytopes and cones. In this paper, we introduce pairs of truncated walls, which are defined as modifications of level -Young walls and describe inequalities defining the polytopes and cones in terms of level -proper Young walls and pairs of truncated walls. As an application, we also give combinatorial descriptions of -functions on in terms of Young walls and truncated walls.
Paper Structure (24 sections, 15 theorems, 152 equations, 13 tables)

This paper contains 24 sections, 15 theorems, 152 equations, 13 tables.

Key Result

Theorem 2.5

K3NZ There is the unique strict embedding of crystals satisfying $\Psi_{\iota} (u_{\infty}) = \textbf{0}$, where $u_{\infty}\in B(\infty)$ is the highest weight vector and $\textbf{0}:=(\cdots,0,\cdots,0,0)\in \mathbb Z^{\infty}_{\iota}$.

Theorems & Definitions (41)

  • Definition 2.1
  • Example 2.2
  • Example 2.3
  • Definition 2.4
  • Theorem 2.5
  • Theorem 2.6
  • Theorem 2.7
  • Definition 2.8
  • Theorem 2.9
  • Theorem 2.10
  • ...and 31 more