Massless field equations for spin 3/2 in dimension 6

Main topic of the paper is a study of properties of massless fields of spin 3/2. A lot of information is available already for massless fields in dimension 4. Here, we concentrate on dimension 6 and we are using the fact that the group S L ( 4 , C ) is isomorphic with the group S p i n ( 6 , C ) . It makes it possible to use tensor formalism for massless fields. Main problems treated in the paper are a description of fields which need to be considered in the spin 3/2 case, a suitable choice of equations they should satisfy, irreducibility of homogeneous solutions of massless field equations, the Fischer decomposition and the Howe duality for such fields.

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Publication Details

Journal
Journal of Geometry and Physics
Published
2024-10-16
DOI
https://doi.org/10.1016/j.geomphys.2024.105341
Citations
1
Primary Topic
Algebraic and Geometric Analysis
Type
article
Field-Weighted Citation Impact
0.97
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article

Massless field equations for spin 3/2 in dimension 6

Wei Wang, Roman Lávička, Vladimı́r Souček
1 citations
Journal of Geometry and Physics
Algebraic and Geometric Analysis
0.97
article

Massless field equations for spin 3/2 in dimension 6

Wei Wang, Roman Lávička, Vladimı́r Souček
article en
1 citations

Abstract

Main topic of the paper is a study of properties of massless fields of spin 3/2. A lot of information is available already for massless fields in dimension 4. Here, we concentrate on dimension 6 and we are using the fact that the group S L ( 4 , C ) is isomorphic with the group S p i n ( 6 , C ) . It makes it possible to use tensor formalism for massless fields. Main problems treated in the paper are a description of fields which need to be considered in the spin 3/2 case, a suitable choice of equations they should satisfy, irreducibility of homogeneous solutions of massless field equations, the Fischer decomposition and the Howe duality for such fields.

Journal of Geometry and PhysicsVol. 206
Openalex Percentile: Top 24%
Algebraic and Geometric Analysis
0.97
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