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Finite-dimensional irreducible representations of the SU(3/1) superalgebra

Bani Mitra

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Abstract

The SU(3/1) superalgebra is constructed using Schwinger’s harmonic oscillator technique. Finite-dimensional irreducible representations of the superalgebra are obtained choosing a suitable weight Ψm, which will be called the maximal weight, using the commutation relations of the superalgebra only and without any knowledge of the matrix elements of the generators of the superalgebra. Atypical representations of the superalgebra are obtained and a comparison of these representations is made with finite-dimensional irreducible representations of SU(4).

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What this paper is about

The SU(3/1) superalgebra is constructed using Schwinger’s harmonic oscillator technique. Finite-dimensional irreducible representations of the superalgebra are obtained choosing a suitable weight Ψm, which will be called the maximal weight, using the commutation relations of the superalgebra only and without any knowledge of the matrix elements of the generators of the superalgebra. Atypical representations of the superalgebra are obtained and a comparison of these representations is made with finite-dimensional irreducible representations of SU(4).

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Available abstract

The SU(3/1) superalgebra is constructed using Schwinger’s harmonic oscillator technique. Finite-dimensional irreducible representations of the superalgebra are obtained choosing a suitable weight Ψm, which will be called the maximal weight, using the commutation relations of the superalgebra only and without any knowledge of the matrix elements of the generators of the superalgebra. Atypical representations of the superalgebra are obtained and a comparison of these representations is made with finite-dimensional irreducible representations of SU(4).

Key concepts: Superalgebra, Supermatrix, Lie superalgebra, Mathematics, Irreducible representation, Pure mathematics, Representation theory of SU, Algebra over a field

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