Supersymmetric $SU(2)_L\times SU(2)_R \times SU(4)_c$ and observable neutron-antineutron oscillation

Details Supersymmetric $SU(2)_L\times SU(2)_R \times SU(4)_c$ and observable neutron-antineutron oscillation Supersymmetric $SU(2)_L\times SU(2)_R \times SU(4)_c$ and observable neutron-antineutron oscillation

1998-02-21

arxiv.org/abs/hep-ph/9802388v1

Phys.Rev. D59 (1999) 055004

Physics

High Energy Physics

High Energy Physics - Phenomenology

4 pages; one figure; Preprint No. UMD-PP-98-94

Scientific paper

10.1103/PhysRevD.59.055004

We show that in a large class of supersymmetric $SU(2)_L\times SU(2)_R\times SU(4)_c$ models with the see-saw mechanism for neutrino masses and an R-parity conserving vacuum, there are diquark Higgs bosons with masses ($M_{qq}$) near the weak scale even though the scale of $SU(2)_R\times SU(4)_c$ symmetry breaking is around $10^{10}$ GeV. This happens because these masses ($M_{qq}$) arise out of higher dimensional operators needed to stabilize the charge conserving vacuum in the model. This feature has the interesting implication that the $\Delta B=2$ processes such as neutron-anti-neutron oscillation can have observable rates while at the same time yielding neutrino masses in the range of current interest.

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