Abstract

We show that in a multi-Higgs model in which one Higgs fits the LHC 125 GeV state, one or more of the other Higgs bosons can mediate DM-nucleon interactions with maximal DM isospin violation being possible for appropriate Higgs-quark couplings, independent of the nature of DM. We then consider the explicit example of a Type II two-Higgs-doublet model, identifying the h or H as the 125 GeV state while the H or h, respectively, mediates DM-nucleon interactions. Finally, we show that if a stable scalar, S, is added then it can be a viable light DM candidate with correct relic density while obeying all direct and indirect detection limits.

Highlights

  • Small SS branching ratio) while correct relic abundance can be achieved via relatively strong interactions of the H (h) with the S

  • II we briefly describe the current status of direct detection experiments and show how isospin-violating interactions of DM are possible in the Type II 2HDM context, independently of whether or not dark matter is a Higgs boson

  • Experimental results are typically translated into the event rate for the spin-independent cross section for DM scattering off a nucleon σDSIM−N as a function of DM mass

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Summary

Direct detection of Dark Matter and isospin-violation

DM is a compelling window to new physics and a primary means for its direct detection is via scattering off nucleons. Where H sums over the Higgs mediators contributing to the t-channel diagrams, CUH,D denote the H couplings to up-, down-type quarks, respectively, normalized to their SM values, while the ΛH are dimensionless parameters specifying the strengths of the H couplings to a pair of DM particles. Using Eq (2.2) and the Higgs-quark couplings CU , CD of Table 1, a given value of fn/fp requires: tan β. SM-like implies that tan β and sin α must lie within the broad central yellow band Combining this with the fn/fp ∼ −0.7 requirement leaves only a small region in each of the (tan β, sin α) parameter spaces, located near tan β ∼ 1 and sin α ∼ −0.7 (+0.7), implying CDH ∼ −CUH ∼ 1 (CUh ∼ −CDh ∼ 1) for the h125 (H125) scenario

The 2HDMS Dark-Matter Model
Collider bounds from direct searches for Higgs bosons
Dark matter direct detection
Dark matter indirect detection
Conclusions

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