Abstract
We propose an extension of the Standard Model gauge symmetry by the gauge group $U(1)_{T3R}$ in order to address the Yukawa coupling hierarchy between the third generation fermions and the first two generation fermions of the SM. We assume that only the right-handed fermions of the first two generations are charged under the $U(1)_{T3R}$. In addition to the new dark gauge boson, we have a dark scalar particle whose vacuum expectation value (vev) breaks the $U(1)_{T3R}$ symmetry down to $Z_2$ symmetry and also explains the hierarchy problem. A vev of $\cal O$(GeV) is required to explain the mass parameters of the light flavor sector naturally. The dark matter (DM) particle arising from the model naturally has mass in the $\mathcal {O}$(1-100) MeV range. The model satisfies all the current constraints. We discuss the various prospects of the direct detection of the dark matter. We get both elastic and inelastic spin independent DM-nucleon scattering. The dark matter obtains the correct thermal relic density by annihilation.
Highlights
In recent years, the central motivation for dark matter direct detection, indirect detection, and collider search strategies has been the WIMP miracle [1]
The WIMP miracle is the statement that a stable particle with a mass of Oð100–1000Þ GeV, annihilating to Standard Model particles with an Oð1Þ coupling, would have a thermal relic density which is consistent with cosmological dark matter
The mass parameters of the charged Standard Model fermions in the two lightest generations all lie in the Oð1–100Þ MeV range, and if dark matter arises from new physics associated with a light flavor, it will naturally lie at that scale
Summary
The central motivation for dark matter direct detection, indirect detection, and collider search strategies has been the WIMP miracle [1]. The mass parameters of the charged Standard Model fermions in the two lightest generations all lie in the Oð1–100Þ MeV range, and if dark matter arises from new physics associated with a light flavor, it will naturally lie at that scale. As expected, all gauge anomalies cancel if the SM fields charged under Uð1ÞT3R consist of a full right-handed generation, including an up-type quark, down-type quark, charged lepton, and a neutrino. This model is anomaly-free if either one or two generations couples to Uð1ÞT3R. If they are not kinematically allowed, A0 → νAνA will dominate. (iii) νs: νs → νAγγ (mediated by an off-shell φ0) will dominate
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