Geometric Hierarchy
May, 198234 pages
Part of Proceedings, Third Workshop on Grand Unification : Chapel Hill, North Carolina, April 15-17, 1982
Published in:
- Nucl.Phys.B 219 (1983) 479,
- Prog.Phys. 6 (1982)
Contribution to:
- Published: 1983
Report number:
- LA-UR-82-1282
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Abstract: (Elsevier)
We present one approach for solving the gauge hierarchy problem in a grand unified supersymmetric theory. Supersymmetry is broken at a scale of order 10 12 GeV. Both the grand scale (∼10 19 GeV) and the weak scale are generated via radiative corrections. The main phenomenological features of the model are: (i) the proton decays into K 0 μ + and K + ν μ and the neutron decays into K 0 ν μ ; (ii) the strong GP problem is solved with an invisible axion; (iii) the superpartners of quarks, leptons, gauge and Higgs bosons have masses ∼ 50–100 GeV; and (iv) the lightest superpartner is stable.- GAUGE FIELD THEORY: HIERARCHY PROBLEM
- GRAND UNIFIED THEORY: SU(5)
- SPONTANEOUS SYMMETRY BREAKING
- P: SEMILEPTONIC DECAY
- SEMILEPTONIC DECAY: P
- N: SEMILEPTONIC DECAY
- SEMILEPTONIC DECAY: N
- CP: violation
- POSTULATED PARTICLE: AXION
- FERMION: MASS
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