Abstract
We discuss the lower bound to the lightest Higgs boson ${H}_{1}$ in the minimal supersymmetric extension of the standard model with explicit $CP$ violation, and the phenomenology of the lightest relic neutralino in the same scenario. In particular, adopting the CPX benchmark scenario, we find that the combination of experimental constraints coming from LEP, thallium electric dipole moment measurements, quarkonium decays, and ${B}_{s}\ensuremath{\rightarrow}\ensuremath{\mu}\ensuremath{\mu}$ decay favors a region of the parameter space where the mass of ${H}_{1}$ is in the range $7\text{ }\text{ }\mathrm{GeV}\ensuremath{\lesssim}{M}_{{H}_{1}}\ensuremath{\lesssim}10\text{ }\text{ }\mathrm{GeV}$, while $3\ensuremath{\lesssim}\mathrm{tan}\ensuremath{\beta}\ensuremath{\lesssim}5$. Assuming a departure from the usual grand unified theory relation among gaugino masses ($|{M}_{1}|\ensuremath{\ll}|{M}_{2}|$), we find that through resonant annihilation to ${H}_{1}$ a neutralino as light as 2.9 GeV can be a viable dark matter candidate in this scenario. We call this the CPX light neutralino scenario and discuss its phenomenology showing that indirect dark matter searches are compatible with the present experimental constraints, as long as ${m}_{\ensuremath{\chi}}\ensuremath{\lesssim}{M}_{{H}_{1}}/2$. On the other hand, part of the range ${m}_{\ensuremath{\chi}}\ensuremath{\gtrsim}{M}_{{H}_{1}}/2$ which is allowed by cosmology is excluded by antiproton fluxes.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.