Abstract
In this paper we construct supersymmetric Pati-Salam (PS) models containing the minimal supersymmetric standard model and an invisible axion. The models include two discrete symmetries, ${\mathbb{Z}}_{4}^{R}\ifmmode\times\else\texttimes\fi{}{\mathbb{Z}}_{N}$, which maintain the quality of the accidental Peccei-Quinn (PQ) symmetry and thus the solution to the strong $CP$ problem. We require that the discrete anomaly conditions are satisfied for both ${\mathbb{Z}}_{4}^{R}\ifmmode\times\else\texttimes\fi{}{G}_{\mathrm{PS}}^{2}$ and ${\mathbb{Z}}_{N}\ifmmode\times\else\texttimes\fi{}{G}_{\mathrm{PS}}^{2}$. The vacuum expectation value of the PQ field spontaneously breaks all the discrete symmetries. R-parity is violated if any of the PQ field(s) has an odd charge under ${\mathbb{Z}}_{4}^{R}$. We present two explicit models which we refer to as a minimal model where R-parity violation is extremely suppressed, and a nonminimal model where R-parity violation is significant. In the latter model, the neutralino becomes unstable even if it is the lightest supersymmetric particle (LSP), and, in addition, there are new low-energy vectorlike states. In both examples, R-parity violation is sufficiently suppressed such that the proton is stable.
Highlights
The Peccei-Quinn (PQ) symmetry, Uð1ÞPQ, provides an attractive solution to the strong CP problem [1,2]
We aim to construct models in which the PQ symmetry arises as an accidental symmetry and its quality is ensured by the discrete symmetries
We introduce SUSY models based on the Pati-Salam gauge symmetry, which is broken down to the Standard Model (SM) at the grand unification theory (GUT) scale, and the discrete ZR4 and ZN symmetries
Summary
The Peccei-Quinn (PQ) symmetry, Uð1ÞPQ, provides an attractive solution to the strong CP problem [1,2]. We propose simple models with Pati-Salam (PS) gauge symmetry and non-anomalous discrete symmetries, ZR4 × ZN, where N is an integer. There can be R-parity violation (RPV) due to the spontaneous breaking of the ZR4 symmetry, if the PQ field carries odd R-charge. In this case we consider two viable scenarios of the unstable LSP. One is that the RPV effect is so suppressed that the lifetime of the LSP is much longer than the age of the universe In this case, the low-energy R-parity is accidental, but is high quality such that the LSP contributes to the DM. The sizes of coupling constants of operators in our examples are listed in Appendix B
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