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Unveiling Crystal Embeddings: New Perspectives on String Polytopes and Atomic Decompositions

Lara Bossinger, Jacinta Torres

TL;DR

This work constructs a family of embeddings $\phi_j$ between string polytopes $\mathcal{S}_{\mathbf{i}}(\lambda)$ and $\mathcal{S}_{\mathbf{i}}(\lambda+\theta)$ in type $A_{n-1}$, where $\theta$ is the highest root, and analyzes their compatibility with the crystal structure. For the endpoint indices $j=1$ and $j=n-1$, these embeddings are crystal morphisms, while other $\phi_j$ exhibit structured compatibility, all culminating in a conjecture that one can produce $n$ distinct atomic decompositions of crystals with highest weight multiples of $\theta$. The paper develops embeddings for arbitrary reduced expressions, leveraging weight-shifting vectors $z_i$ and projection maps that relate to $\mathfrak{sl}_{n-1}$, and provides explicit realizations of the crystal operators via wiring diagrams and Gleizer–Postnikov rigorous paths. If validated, the conjectures offer a new, geometric mechanism to construct atomic decompositions and positively compute Kostka–Foulkes-type polynomials beyond type $A$, linking crystal theory, affine Hecke algebras, and pre-canonical bases. Overall, the approach extends the landscape of atomic decompositions in crystals and suggests a broad, embedding-based strategy for positive combinatorial formulas in representation theory.

Abstract

We present n-1 different embeddings of string polytopes of type A. We characterize their compatibility with the crystal structure on the string polytopes, and formulate a conjecture describing how to obtain n-1 different atomic decompositions of the crystal with highest weight a multiple of the highest root.

Unveiling Crystal Embeddings: New Perspectives on String Polytopes and Atomic Decompositions

TL;DR

This work constructs a family of embeddings between string polytopes and in type , where is the highest root, and analyzes their compatibility with the crystal structure. For the endpoint indices and , these embeddings are crystal morphisms, while other exhibit structured compatibility, all culminating in a conjecture that one can produce distinct atomic decompositions of crystals with highest weight multiples of . The paper develops embeddings for arbitrary reduced expressions, leveraging weight-shifting vectors and projection maps that relate to , and provides explicit realizations of the crystal operators via wiring diagrams and Gleizer–Postnikov rigorous paths. If validated, the conjectures offer a new, geometric mechanism to construct atomic decompositions and positively compute Kostka–Foulkes-type polynomials beyond type , linking crystal theory, affine Hecke algebras, and pre-canonical bases. Overall, the approach extends the landscape of atomic decompositions in crystals and suggests a broad, embedding-based strategy for positive combinatorial formulas in representation theory.

Abstract

We present n-1 different embeddings of string polytopes of type A. We characterize their compatibility with the crystal structure on the string polytopes, and formulate a conjecture describing how to obtain n-1 different atomic decompositions of the crystal with highest weight a multiple of the highest root.

Paper Structure

This paper contains 9 sections, 8 theorems, 28 equations, 4 figures.

Key Result

Theorem 2.3

The cone $\mathcal{S}_{\underline{i}}$ is a semigroup, that is, $x+y \in \mathcal{S}_{\underline{i}}$ for $x,y \in \mathcal{S}_{\underline{i}}$.

Figures (4)

  • Figure 1: The wiring diagram $\operatorname{wd}(\mathbf{i})$ for $n = 5$ and $\mathbf{i} = (1,2,3,4,1,2,3,1,2,1)$ with orientation $(\ell_3,\ell_4)$. In blue, a rigorous path in $\Gamma_3$ determined by its turning points $v_{3,1}$ and $v_{1,4}$.
  • Figure 2: On the left (resp. right) the two red arrows are forbidden in left (resp. right) rigorous paths.
  • Figure 3: Half of the associated crystal graph $\mathcal{B}(\theta)$ for $\mathfrak{sl}(5,\mathbb{C})$ and its adjoint representation with highest root $\theta = \omega_{1} + \omega_{4}$. Arrows $a \overset{i}{\longrightarrow} b$ mean $f_{i}(a) = b$.
  • Figure 4: Notice how the subword of ${\bf i}=(1,3,2,4,1,3,2,4,3,1)$ corresponding to $z_1=f_1f_2f_3f_4.b_{\theta}$ (resp. $z_4=f_4f_3f_2f_1.b_{\theta}$) picks up all crossings along the wire $\ell_1$ (resp. $\ell_5$). This is not true for other $z_i$, $i\not\in\{1,4\}$, as for example, $z_3=f_3f_4f_2f_1.b_\theta$ is parametrized by the crossings marked by ${\color{green}\bullet}$ which are spread over different wires.

Theorems & Definitions (27)

  • Remark 2.1
  • Definition 2.2
  • Theorem 2.3: Berenstein--Zelevinsky BerensteinZelevinsky
  • Theorem 2.4: Littelmann conescrystalspatterns
  • Definition 3.1
  • Definition 3.2
  • Remark 3.3
  • Theorem 3.4: Gleizer-Postnikov Corollary 5.8, beaglebvolker Theorem 6.1
  • Definition 3.5
  • Definition 3.6
  • ...and 17 more