Particular boundary condition ensures that a fermion in \(d=1+5\), compactified on a finite disk, manifests in \(d=1+3\) as massless spinor with a charge \(1/2\), mass protected and chirally coupled to the gauge field
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Publication:901678
DOI10.1016/j.physletb.2008.04.017zbMath1328.83169arXiv0710.1956OpenAlexW1977429575MaRDI QIDQ901678
Publication date: 12 January 2016
Published in: Physics Letters. B (Search for Journal in Brave)
Full work available at URL: https://arxiv.org/abs/0710.1956
Quantum field theory on curved space or space-time backgrounds (81T20) Kaluza-Klein and other higher-dimensional theories (83E15)
Related Items (3)
Discrete symmetries in the Kaluza-Klein theories ⋮ Particular boundary condition ensures that a fermion in \(d=1+5\), compactified on a finite disk, manifests in \(d=1+3\) as massless spinor with a charge \(1/2\), mass protected and chirally coupled to the gauge field ⋮ ‘Effective two dimensionality’ cases bring a new hope to the Kaluza–Klein(like) theories
Cites Work
- Fermions with no fundamental charges call for extra dimensions
- Particular boundary condition ensures that a fermion in \(d=1+5\), compactified on a finite disk, manifests in \(d=1+3\) as massless spinor with a charge \(1/2\), mass protected and chirally coupled to the gauge field
- UNIFICATION OF SPINS AND CHARGES IN GRASSMANN SPACE?
- Spinor and vector representations in four-dimensional Grassmann space
- How to generate spinor representations in any dimension in terms of projection and nilpotent operators
- How to generate families of spinors
- Unification of spins and charges
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