How to generate spinor representations in any dimension in terms of projection and nilpotent operators
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Publication:4832824
DOI10.1063/1.1505125zbMath1060.81038OpenAlexW2054041358MaRDI QIDQ4832824
Norma Susana Mankoč Borštnik, Holger Bech Nielsen
Publication date: 14 December 2004
Published in: Journal of Mathematical Physics (Search for Journal in Brave)
Full work available at URL: https://doi.org/10.1063/1.1505125
Spinor and twistor methods applied to problems in quantum theory (81R25) Clifford algebras, spinors (15A66)
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Cites Work
- UNIFICATION OF SPINS AND CHARGES IN GRASSMANN SPACE?
- SPINORS, VECTORS AND SCALARS IN GRASSMANN SPACE AND CANONICAL QUANTIZATION FOR FERMIONS AND BOSONS
- Spinor and vector representations in four-dimensional Grassmann space
- Spinors in n Dimensions
- Why odd-space and odd-time dimensions in even-dimensional spaces?
- Unification of spins and charges