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The orientifold Temperley--Lieb algebra

Chris Bowman, Zajj Daugherty, Maud De Visscher, Rob Muth, Loic Poulain D'andecy

TL;DR

The work develops a graded representation-theoretic framework for two-boundary algebras by realizing them as finite-dimensional graded quotients of orientifold quiver Hecke algebras, establishing a graded cellular structure for the symplectic blob algebra, and deriving a conjectural LLT-style algorithm to compute graded decomposition numbers. The approach connects transfer-matrix algebras from statistical mechanics with categorification via orientifold quiver Hecke algebras, offering an explicit construction of graded simples in non-generic parameter regimes. A key outcome is the identification of a graded cellular basis for the orientifold TL algebra and a detailed combinatorial model using orientifold paths, ladder tableaux, and standard tableaux, which yields both structural results and computational tools. The paper moreover analyzes decomposition matrices across root-of-unity vs non-root-of-unity cases and demonstrates phenomena (e.g., Nakayama-type failures) that illuminate the rich block structure of these algebras and potential links to $ extit{imath}$quantum groups.

Abstract

We construct gradings on the simple modules of 2-boundary Temperley--Lieb algebras and symplectic blob algebras by realising the latter algebras as quotients of Varagnolo--Vasserot's orientifold quiver Hecke algebras. We prove that the symplectic blob algebras are graded cellular and provide a conjectural algorithm for calculating their graded decomposition matrices. In doing so, we give the first explicit family of finite-dimensional graded quotients of the orientifold quiver Hecke algebras, providing a new entry point for the structure of these algebras -- in the spirit of Libedinsky--Plaza's ``blob algebra approach'' to modular representation theory.

The orientifold Temperley--Lieb algebra

TL;DR

The work develops a graded representation-theoretic framework for two-boundary algebras by realizing them as finite-dimensional graded quotients of orientifold quiver Hecke algebras, establishing a graded cellular structure for the symplectic blob algebra, and deriving a conjectural LLT-style algorithm to compute graded decomposition numbers. The approach connects transfer-matrix algebras from statistical mechanics with categorification via orientifold quiver Hecke algebras, offering an explicit construction of graded simples in non-generic parameter regimes. A key outcome is the identification of a graded cellular basis for the orientifold TL algebra and a detailed combinatorial model using orientifold paths, ladder tableaux, and standard tableaux, which yields both structural results and computational tools. The paper moreover analyzes decomposition matrices across root-of-unity vs non-root-of-unity cases and demonstrates phenomena (e.g., Nakayama-type failures) that illuminate the rich block structure of these algebras and potential links to quantum groups.

Abstract

We construct gradings on the simple modules of 2-boundary Temperley--Lieb algebras and symplectic blob algebras by realising the latter algebras as quotients of Varagnolo--Vasserot's orientifold quiver Hecke algebras. We prove that the symplectic blob algebras are graded cellular and provide a conjectural algorithm for calculating their graded decomposition matrices. In doing so, we give the first explicit family of finite-dimensional graded quotients of the orientifold quiver Hecke algebras, providing a new entry point for the structure of these algebras -- in the spirit of Libedinsky--Plaza's ``blob algebra approach'' to modular representation theory.
Paper Structure (24 sections, 23 theorems, 171 equations, 24 figures)

This paper contains 24 sections, 23 theorems, 171 equations, 24 figures.

Key Result

Proposition 2.1

The set of all reduced diagrams forms a basis of the (infinite dimensional) 2-boundary Temperley--Lieb algebra.

Figures (24)

  • Figure 1: The nine possible two row shapes for $n=2$ (where $9=1+2^2+2^2$ for the choices of $j=1,2$).
  • Figure 2: Example for the proof of \ref{['prop:calibrated B modules']} when $n=5$ and $i= \frac{5+1}{2} = 3$. Pictured below are the standard tableaux $\mathsf{t}$ of shape $\gamma = (\beta q^{-4}, \beta q^{-2}, \beta , \beta q^{2}, \beta q^{4})$. They are marked by which of $e_0, e_1, \dots, e_4$ act by $0$ on the corresponding weight vector $v_\mathsf{t}$ in $N(\gamma)$ (where $e_0$ acts by $0$ if and only if $\beta \in\{ \alpha_1,\alpha_2\}$). The tableau marked $\mathsf{t}_\star$ is the unique tableau for which $e_j v_{\mathsf{t}_\star} \ne 0$ for all $j = 1,\dots, 4$. The other tableaux marked by $\star$ are the remaining of the elements of $F_\mathrm{odd}$, those whose corresponding weight vectors are not annihilated by any odd $e_{2j-1}$. Below that list, find the orbits of $\mathsf{t}_\star$ under the action of $S_\mathrm{odd}= \langle s_1,s_3\rangle$ and of $S_\mathrm{even} = \langle s_2,s_4\rangle$.
  • Figure 3: Example for the proof of \ref{['prop:calibrated B modules']} when $n=6$ and $i= \frac{6}{2} = 3$. Pictured below are the standard tableaux $\mathsf{t}$ of shape $\gamma = (\beta q^{-4}, \beta q^{-2}, \beta , \beta q^{2}, \beta q^{4}, \beta q ^6)$. They are marked by which of $e_0, e_1, \dots, e_5$ act by $0$ on the corresponding weight vector $v_\mathsf{t}$ in $N(\gamma)$ (where $e_0$ acts by $0$ if and only if $\beta \in\{ \alpha_1,\alpha_2\}$). The tableau marked $\mathsf{t}_\star$ is the unique tableau for which $e_j v_{\mathsf{t}_\star} \ne 0$ for all $j = 2,3,\dots, 5$. The other tableaux marked by $\star$ are the remaining of the elements of $F_\mathrm{even}$, those whose corresponding weight vectors are not annihilated by any even $e_{2j}$. Below that list, find the orbits of $\mathsf{t}_\star$ under the action of $S_\mathrm{odd}= \langle s_3,s_5\rangle$ and of $S_\mathrm{even} = \langle s_2,s_4\rangle$.
  • Figure 4: A standard tableau of shape $(k,\beta)$ for $k=3$ and $n=19$.
  • Figure 5: The tableau $\mathsf{t}_{(k,\beta)}$ for $k=3$ and $n=19$. We have that $\mathrm{res}(\mathsf{t}_{(k,\beta)})=(\beta,\,\beta^{-1}q^{2},\,\beta q^2,\, \beta^{-1}q^{4} ,\, \beta q^{4},\,\beta^{-1}q^{6},\,\beta q ^6,\,\dots)$.
  • ...and 19 more figures

Theorems & Definitions (65)

  • Proposition 2.1: GN
  • Lemma 2.2
  • proof
  • Definition 2.3: GN
  • Remark 2.4
  • Remark 3.1
  • Definition 3.2
  • Example 3.3
  • Theorem 3.4: DR25a, DR25b
  • Proposition 3.5
  • ...and 55 more