Supersymmetric field theory in twotime physics
Abstract
We construct N=1 supersymmetry in 4+2 dimensions compatible with the theoretical framework of 2T physics field theory and its gauge symmetries. The fields are arranged into 4+2dimensional chiral and vector supermultiplets, and their interactions are uniquely fixed by supersymmetry (SUSY) and 2Tphysics gauge symmetries. Many 3+1 spacetimes emerge from 4+2 by gauge fixing. Gauge degrees of freedom are eliminated as one comes down from 4+2 to 3+1 dimensions without any remnants of KaluzaKlein modes. In a special gauge, the remaining physical degrees of freedom, and their interactions, coincide with ordinary N=1 supersymmetric field theory in 3+1 dimensions. In this gauge, SUSY in 4+2 is interpreted as superconformal symmetry SU(2,21) in 3+1 dimensions. Furthermore, the underlying 4+2 structure imposes some interesting restrictions on the emergent 3+1 SUSY field theory, which could be considered as part of the predictions of 2Tphysics. One of these is the absence of the troublesome renormalizable CP violating F*F terms. This is good for curing the strong CP violation problem of QCD. An additional feature is that the superpotential is required to have no dimensionful parameters. To induce phase transitions, such as SUSY or electroweak symmetry breaking, a coupling to the dilaton is needed. This suggests amore »
 Authors:

 Department of Physics and Astronomy, University of Southern California, Los Angeles, California 900890484 (United States)
 Publication Date:
 OSTI Identifier:
 21027906
 Resource Type:
 Journal Article
 Journal Name:
 Physical Review. D, Particles Fields
 Additional Journal Information:
 Journal Volume: 76; Journal Issue: 10; Other Information: DOI: 10.1103/PhysRevD.76.105028; (c) 2007 The American Physical Society; Country of input: International Atomic Energy Agency (IAEA); Journal ID: ISSN 05562821
 Country of Publication:
 United States
 Language:
 English
 Subject:
 72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS; CHIRALITY; COUPLING; CP INVARIANCE; DEGREES OF FREEDOM; GAUGE INVARIANCE; KALUZAKLEIN THEORY; PHASE TRANSFORMATIONS; POTENTIALS; QUANTUM CHROMODYNAMICS; RENORMALIZATION; SPACETIME; STANDARD MODEL; SUPERGRAVITY; SUPERMULTIPLETS; SUPERSYMMETRY; SYMMETRY BREAKING; TWODIMENSIONAL CALCULATIONS
Citation Formats
Bars, Itzhak, and Kuo, YuehCheng. Supersymmetric field theory in twotime physics. United States: N. p., 2007.
Web. doi:10.1103/PHYSREVD.76.105028.
Bars, Itzhak, & Kuo, YuehCheng. Supersymmetric field theory in twotime physics. United States. https://doi.org/10.1103/PHYSREVD.76.105028
Bars, Itzhak, and Kuo, YuehCheng. Thu .
"Supersymmetric field theory in twotime physics". United States. https://doi.org/10.1103/PHYSREVD.76.105028.
@article{osti_21027906,
title = {Supersymmetric field theory in twotime physics},
author = {Bars, Itzhak and Kuo, YuehCheng},
abstractNote = {We construct N=1 supersymmetry in 4+2 dimensions compatible with the theoretical framework of 2T physics field theory and its gauge symmetries. The fields are arranged into 4+2dimensional chiral and vector supermultiplets, and their interactions are uniquely fixed by supersymmetry (SUSY) and 2Tphysics gauge symmetries. Many 3+1 spacetimes emerge from 4+2 by gauge fixing. Gauge degrees of freedom are eliminated as one comes down from 4+2 to 3+1 dimensions without any remnants of KaluzaKlein modes. In a special gauge, the remaining physical degrees of freedom, and their interactions, coincide with ordinary N=1 supersymmetric field theory in 3+1 dimensions. In this gauge, SUSY in 4+2 is interpreted as superconformal symmetry SU(2,21) in 3+1 dimensions. Furthermore, the underlying 4+2 structure imposes some interesting restrictions on the emergent 3+1 SUSY field theory, which could be considered as part of the predictions of 2Tphysics. One of these is the absence of the troublesome renormalizable CP violating F*F terms. This is good for curing the strong CP violation problem of QCD. An additional feature is that the superpotential is required to have no dimensionful parameters. To induce phase transitions, such as SUSY or electroweak symmetry breaking, a coupling to the dilaton is needed. This suggests a common origin of phase transitions that is driven by the vacuum value of the dilaton and needs to be understood in a cosmological scenario as part of a unified theory that includes the coupling of supergravity to matter. Another interesting aspect of the proposed theory is the possibility to utilize the inherent 2T gauge symmetry to explore dual versions of the N=1 theory in 3+1 dimensions, such as the minimal supersymmetric standard model (MSSM) and its duals. This is expected to reveal nonperturbative aspects of ordinary 1T field theory.},
doi = {10.1103/PHYSREVD.76.105028},
url = {https://www.osti.gov/biblio/21027906},
journal = {Physical Review. D, Particles Fields},
issn = {05562821},
number = 10,
volume = 76,
place = {United States},
year = {2007},
month = {11}
}