Free massless fermionic fields of arbitrary spin in d-dimensional anti-de sitter space |
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| Affiliation: | 1. Hunan Provincial Key Laboratory of Environmental Catalysis & Waste Re-cycling, School of Materials and Chemical Engineering, Hunan Institute of Engineering, Xiangtan 411104, China;2. Department of Chemistry and Chemical Engineering, Chalmers University of Technology, Göteborg SE-412 96, Sweden;3. King Abdullah University of Science and Technology (KAUST), KAUST Solar Center (KSC), Thuwal 23955, Saudi Arabia;4. School of Materials Science and Engineering, Key Laboratory of Environmentally Friendly Polymer Materials of Jiangsu Province, Jiangsu Engineering Laboratory of Light-Electricity-Heat Energy-Converting Materials and Applications, Jiangsu Collaborative Innovation Center of Photovoltaic Science and Engineering, Changzhou University, Changzhou 213164, China;5. Department of Chemistry, Korea University, Anam-ro 145, Seoul 02841, Republic of Korea;6. Department of Organic Chemistry, Kaunas University of Technology, Kaunas LT-50254, Lithuania;7. School of Materials Science and Engineering, Zhengzhou University, Zhengzhou 450001, China;8. Advanced Membranes and Porous Materials Center, Physical Sciences and Engineering Division, King Abdullah University of Science and Technology, Thuwal 23955-6900, Saudi Arabia;1. Departamento de Física, Centro de Investigación y de Estudios Avanzados del IPN, Apdo. Postal 14-740, 07000 Mexico, Distrito Federal, Mexico;2. AHEP Group, Institut de Física Corpuscular – C.S.I.C./Universitat de València, Parc Cientific de Paterna, C/Catedratico José Beltrán, 2, E-46980 Paterna (València), Spain;1. Department of Chemical Engineering, Monash University, Clayton, Victoria 3800, Australia;2. CSIRO Manufacturing, Bayview Avenue, Clayton, Victoria 3168, Australia |
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| Abstract: | Free massless fermionic fields of arbitrary spins, corresponding to fully symmetric tensor-spinor irreducible representations of the flat little group SO(d−2), are described in d-dimensional anti-de Sitter space in terms of differential forms. Appropriate linearized higher-spin curvature 2-forms are found. Explicitly gauge invariant higher-spin actions are constructed in terms of these linearized curvatures. |
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