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Crystal base of the negative half of quantum orthosymplectic superalgebra

Il-Seung Jang, Jae-Hoon Kwon, Akito Uruno

TL;DR

This work constructs a crystal base for the negative half ${\mathcal U}(\mathfrak g)^-$ of a quantum orthosymplectic superalgebra, realized as a limit of crystals from $q$-oscillator representations and organized through parabolic Verma modules. The authors develop a PBW-type crystal realization and establish a sequence of compatible crystal bases for modules $V(\lambda,\ell)$, $P(\lambda)$, $Q(\lambda)$, and $R(\lambda)$, ultimately assembling ${\mathcal U}(\mathfrak g)^-$ and its crystal ${\mathscr B}(\infty)$. A central achievement is a combinatorial embedding of $\mathscr B(V(\lambda,\ell))$ into $\mathscr B(P(\lambda))$, mediated by separation algorithms and crystal isomorphisms: in type $B$ and $C$ via a super-analogue of the RSK correspondence, and in type $D$ via a Burge-type correspondence. The paper also proves a Burge theorem for orthosymplectic type, clarifying the interplay between crystal bases, Lusztig data, and parabolic inductions, thereby extending the oscillator- and parabolic-Verma-approach to nontrivial superalgebra settings with $n>0$. These results enrich the crystal-theoretic toolbox for quantum superalgebras and connect to broader combinatorial frameworks such as spinor models and RSK/Burge correspondences.

Abstract

We construct a crystal base of the negative half of a quantum orthosymplectic superalgebra. It can be viewed as a limit of the crystal bases of $q$-deformed irreducible oscillator representations. We also give a combinatorial description of the embedding from the crystal of a $q$-oscillator representation to that of the negative half subalgebra given in terms of a PBW type basis. It is given as a composition of embeddings into the crystals of intermediate parabolic Verma modules, where the most non-trivial one is from an oscillator module to a maximally parabolic Verma module with respect to a quantum subsuperalgebra for $\mathfrak{gl}_{m|n}$. A new crystal theoretic realization of Burge correspondence of orthosymplectic type plays an important role for the description of this embedding.

Crystal base of the negative half of quantum orthosymplectic superalgebra

TL;DR

This work constructs a crystal base for the negative half of a quantum orthosymplectic superalgebra, realized as a limit of crystals from -oscillator representations and organized through parabolic Verma modules. The authors develop a PBW-type crystal realization and establish a sequence of compatible crystal bases for modules , , , and , ultimately assembling and its crystal . A central achievement is a combinatorial embedding of into , mediated by separation algorithms and crystal isomorphisms: in type and via a super-analogue of the RSK correspondence, and in type via a Burge-type correspondence. The paper also proves a Burge theorem for orthosymplectic type, clarifying the interplay between crystal bases, Lusztig data, and parabolic inductions, thereby extending the oscillator- and parabolic-Verma-approach to nontrivial superalgebra settings with . These results enrich the crystal-theoretic toolbox for quantum superalgebras and connect to broader combinatorial frameworks such as spinor models and RSK/Burge correspondences.

Abstract

We construct a crystal base of the negative half of a quantum orthosymplectic superalgebra. It can be viewed as a limit of the crystal bases of -deformed irreducible oscillator representations. We also give a combinatorial description of the embedding from the crystal of a -oscillator representation to that of the negative half subalgebra given in terms of a PBW type basis. It is given as a composition of embeddings into the crystals of intermediate parabolic Verma modules, where the most non-trivial one is from an oscillator module to a maximally parabolic Verma module with respect to a quantum subsuperalgebra for . A new crystal theoretic realization of Burge correspondence of orthosymplectic type plays an important role for the description of this embedding.

Paper Structure

This paper contains 36 sections, 172 equations.