Baryon and lepton number (non)conservation in supersymmetric theories
19939 pages
Published in:
- Phys.Lett.B 314 (1993) 336-344
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Abstract: (Elsevier)
We discuss the origin of baryon and lepton number (non-)conservation in supersymmetric versions of the standard model in which the Higgs mass term is generated via the vacuum expectation value of a singlet field and nucleon stability is guaranteed by a discrete symmetry. We determine the simplest examples satisfying the discrete anomaly cancellation conditions. With only one singlet field present anomaly cancellation can be achieved with nucleon conservation guaranteed at dimension 4 by a matter parity or a lepton parity (a symmetry that allows baryon number violating operators in the low energy lagrangian). If two singlet fields are present, a baryon parity (which allows lepton number violating terms) is also anomaly free. In some cases nucleon decay is further inhibited because all the dimension-five baryon number violating operators are forbidden eliminating the need for any small couplings. We show that such discrete symmetries may also allow a flavour subset of lepton number violating operators, allowing for primordial baryogenesis and non-standard SUSY phenomenology. A novel feature in the latter case is the simultaneous presence of both lepton and baryon number violating operators without disturbing the proton stability.- baryon number: violation
- lepton number: violation
- supersymmetry
- anomaly
- nucleon: stability
- symmetry: discrete
- quantum number
- gauge field theory: SU(3) x SU(2) x U(1)
- Higgs particle: mass generation
- mass generation: Higgs particle
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