On vacuum structures of N = 2 LSUSY QED equivalent to N = 2 NLSUSY model
arXiv:0710.1680 · doi:10.1016/j.physletb.2007.11.036 10.1016/j.physletb.2007.12.043
Abstract
The vacuum structure of N = 2 linear supersymmetry (LSUSY) invariant QED, which is equivalent to N = 2 nonlinear supersymmetry (NLSUSY) model, is studied explicitly in two dimensional space-time (d = 2). Two different isometries SO(1,3) and SO(3,1) appear for the vacuum field configuration corresponding to the various parameter regions. Two different field configurations of SO(3,1) isometry describe the two different physical vacua, i.e. one breaks spontaneously both U(1) and SUSY and the other breaks spontaneously SUSY alone.
arXiv comment10 pages, correct form of the potential given as a footnote
References in corpus (7)
- Supersymmetric structure of spacetime and matter -superon-graviton model-
- New supersymmetry algebra on gravitational interaction of Nambu-Goldstone fermion
- On Linearization of N=1 Nonlinear Supersymmetry
- Linearizing N = 2 Nonlinear Supersymmetry
- On Origin of Mass and Supersymmetry
- On Yukawa and mass terms in nonlinear supersymmetry equivalent renormarizable theory
- New Einstein-Hilbert-type Action and Superon-Graviton Model(SGM) of Nature
Cited by in corpus (9)
- On Wess-Zumino gauge
- Systematics of linearization of N = 2 nonlinear SUSY in superfield formulation
- On N = 2 superfield for N = 2 vector supermultiplet in two dimensional spacetime
- Super Yang-Mills theory from nonlinear supersymmetry
- Nonlinear SUSY General Relativity Theory and Significances
- Particle astrophysics in nonlinear supersymmetric general relativity
- On gauge coupling constant in linearization of nonlinear supersymmetry
- On SUSY breaking from NL/L SUSY relation
- Low energy particle physics and cosmology of nonlinear supersymmetric general relativity