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Main Authors: Sun, Binni, Zhao, Yufeng
Format: Preprint
Published: 2023
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Online Access:https://arxiv.org/abs/2304.11601
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author Sun, Binni
Zhao, Yufeng
author_facet Sun, Binni
Zhao, Yufeng
contents Let $\mathfrak{g}$ be a complex simple Lie algebra and $Z(\mathfrak{g})$ be the center of the universal enveloping algebra $U(\mathfrak{g})$. Denote by $V_λ$ the finite-dimensional irreducible $\mathfrak{g}$-module with highest weight $λ$. Lehrer and Zhang defined the notion of strongly multiplicity free representations for simple Lie algebras motivated by studying the structure of the endomorphism algebra $\text{End}_{U(\mathfrak{g})}(V_λ^{\otimes r})$ in terms of the quotients of the Kohno's infinitesimal braid algebra. Kostant introduced the $\mathfrak{g}$-invariant endomorphism algebras $R_λ(\mathfrak{g})= (\text{End} V_λ\otimes U(\mathfrak{g}))^\mathfrak{g}$ and $R_{λ,π}(\mathfrak{g})=(\text{End} V_λ\otimes π(U(\mathfrak{g})))^\mathfrak{g}.$ In this paper, we give some other criteria for a multiplicity free representation to be strongly multiplicity free by classifying the pairs $(\mathfrak{g}, V_λ)$, which are multiplicity free and for such pairs, $R_λ(\mathfrak{g})$ and $R_{λ,π}(\mathfrak{g})$ are generated by generalizations of the quadratic Casimir elements of $Z(\mathfrak{g})$.
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publishDate 2023
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spellingShingle Descriptions of strongly multiplicity free representations for simple Lie algebras
Sun, Binni
Zhao, Yufeng
Representation Theory
Let $\mathfrak{g}$ be a complex simple Lie algebra and $Z(\mathfrak{g})$ be the center of the universal enveloping algebra $U(\mathfrak{g})$. Denote by $V_λ$ the finite-dimensional irreducible $\mathfrak{g}$-module with highest weight $λ$. Lehrer and Zhang defined the notion of strongly multiplicity free representations for simple Lie algebras motivated by studying the structure of the endomorphism algebra $\text{End}_{U(\mathfrak{g})}(V_λ^{\otimes r})$ in terms of the quotients of the Kohno's infinitesimal braid algebra. Kostant introduced the $\mathfrak{g}$-invariant endomorphism algebras $R_λ(\mathfrak{g})= (\text{End} V_λ\otimes U(\mathfrak{g}))^\mathfrak{g}$ and $R_{λ,π}(\mathfrak{g})=(\text{End} V_λ\otimes π(U(\mathfrak{g})))^\mathfrak{g}.$ In this paper, we give some other criteria for a multiplicity free representation to be strongly multiplicity free by classifying the pairs $(\mathfrak{g}, V_λ)$, which are multiplicity free and for such pairs, $R_λ(\mathfrak{g})$ and $R_{λ,π}(\mathfrak{g})$ are generated by generalizations of the quadratic Casimir elements of $Z(\mathfrak{g})$.
title Descriptions of strongly multiplicity free representations for simple Lie algebras
topic Representation Theory
url https://arxiv.org/abs/2304.11601