Spin dependent masses and Sim(2) symmetry
- 1. Department of Physics, Yale University, New Haven, CT 06520 (United States)
Description
Recently, Cohen and Glashow pointed out that all known experimental tests of relativistic kinematics are consistent with invariance of physics under the four-parameter subgroup Sim(2) of the Lorentz group. The massive one-particle irreducible representations of ISim(2), that is Sim(2) times spacetime translations, are all one-dimensional, labeled by spin along a preferred axis. Consequently particle theories based on this symmetry can accommodate lepton number conserving masses for left-handed neutrinos without the need to introduce sterile states. The same property of massive particle representations, however, also leads to the possibility that particle masses may be split within the different spins of a representation of the ordinary Poincare group. In this Letter we investigate the low-energy structure of theories with spin dependent masses and comment on the bounds on such effects
Additional details
Identifiers
- DOI
- 10.1016/j.physletb.2007.03.055;
- arXiv
- arXiv:hep-ph/0611049v1;
- PII
- S0370-2693(07)00419-4;
Publishing Information
- Journal Title
- Physics Letters. Section B
- Journal Volume
- 649
- Journal Issue
- 2-3
- Journal Page Range
- p. 186-190
- ISSN
- 0370-2693
- CODEN
- PYLBAJ
INIS
- Country of Publication
- Netherlands
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 39027516
- Subject category
- S71: CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS;
- Descriptors DEI
- IRREDUCIBLE REPRESENTATIONS; LEPTON NUMBER; LORENTZ GROUPS; MASS; NEUTRINOS; ONE-DIMENSIONAL CALCULATIONS; RELATIVISTIC RANGE; SPACE-TIME; SPIN; SYMMETRY
- Descriptors DEC
- ANGULAR MOMENTUM; ELEMENTARY PARTICLES; ENERGY RANGE; FERMIONS; LEPTONS; LIE GROUPS; MASSLESS PARTICLES; PARTICLE PROPERTIES; POINCARE GROUPS; SYMMETRY GROUPS
Optional Information
- Copyright
- Copyright (c) 2007 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.