From sl_q(2) to a Parabosonic Hopf Algebra

A Hopf algebra with four generators among which an involution (reflection) operator, is introduced. The defining relations involve commutators and anticommutators. The discrete series representations are developed. Designated by sl_{−1}(2), this algebra encompasses the Lie superalgebra osp(1|2). It...

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Main Authors: Satoshi Tsujimoto, Luc Vinet, Alexei Zhedanov
Format: Article
Language:English
Published: National Academy of Science of Ukraine 2011-11-01
Series:Symmetry, Integrability and Geometry: Methods and Applications
Subjects:
Online Access:http://dx.doi.org/10.3842/SIGMA.2011.093
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author Satoshi Tsujimoto
Luc Vinet
Alexei Zhedanov
author_facet Satoshi Tsujimoto
Luc Vinet
Alexei Zhedanov
author_sort Satoshi Tsujimoto
collection DOAJ
description A Hopf algebra with four generators among which an involution (reflection) operator, is introduced. The defining relations involve commutators and anticommutators. The discrete series representations are developed. Designated by sl_{−1}(2), this algebra encompasses the Lie superalgebra osp(1|2). It is obtained as a q=−1 limit of the sl_q(2) algebra and seen to be equivalent to the parabosonic oscillator algebra in irreducible representations. It possesses a noncocommutative coproduct. The Clebsch-Gordan coefficients (CGC) of sl_{−1}(2) are obtained and expressed in terms of the dual −1 Hahn polynomials. A generating function for the CGC is derived using a Bargmann realization.
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spelling doaj.art-bd06a3ea51204192bce52f02be1c02772022-12-21T21:46:07ZengNational Academy of Science of UkraineSymmetry, Integrability and Geometry: Methods and Applications1815-06592011-11-017093From sl_q(2) to a Parabosonic Hopf AlgebraSatoshi TsujimotoLuc VinetAlexei ZhedanovA Hopf algebra with four generators among which an involution (reflection) operator, is introduced. The defining relations involve commutators and anticommutators. The discrete series representations are developed. Designated by sl_{−1}(2), this algebra encompasses the Lie superalgebra osp(1|2). It is obtained as a q=−1 limit of the sl_q(2) algebra and seen to be equivalent to the parabosonic oscillator algebra in irreducible representations. It possesses a noncocommutative coproduct. The Clebsch-Gordan coefficients (CGC) of sl_{−1}(2) are obtained and expressed in terms of the dual −1 Hahn polynomials. A generating function for the CGC is derived using a Bargmann realization.http://dx.doi.org/10.3842/SIGMA.2011.093parabosonic algebradual Hahn polynomialsClebsch-Gordan coefficients
spellingShingle Satoshi Tsujimoto
Luc Vinet
Alexei Zhedanov
From sl_q(2) to a Parabosonic Hopf Algebra
Symmetry, Integrability and Geometry: Methods and Applications
parabosonic algebra
dual Hahn polynomials
Clebsch-Gordan coefficients
title From sl_q(2) to a Parabosonic Hopf Algebra
title_full From sl_q(2) to a Parabosonic Hopf Algebra
title_fullStr From sl_q(2) to a Parabosonic Hopf Algebra
title_full_unstemmed From sl_q(2) to a Parabosonic Hopf Algebra
title_short From sl_q(2) to a Parabosonic Hopf Algebra
title_sort from sl q 2 to a parabosonic hopf algebra
topic parabosonic algebra
dual Hahn polynomials
Clebsch-Gordan coefficients
url http://dx.doi.org/10.3842/SIGMA.2011.093
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