Abstract

The inert doublet model is a minimal dark matter model with strong theoretical motivations, where the stability of dark matter is usually achieved by imposing a $Z_2$ parity. We promote the $Z_2$ parity into a global $U(1)$ symmetry and study its phenomenological implications. There are two characteristic features of the model: both the CP-even and CP-odd neutral inert scalars, $h_1$ and $h_2$, become DM candidates; the number of model parameters is one less than that with $Z_2$ parity. We first analyze the constraints from LEP experiments, electroweak precision tests, theoretical stability, Higgs precision data, dark matter relic density, and direct detection experiments. It is found that if the model is required to explain at least 10% of the observed relic density, the theory is extremely limited such that the dark matter mass is about $70\;{\rm GeV}$ and the charged Higgs boson is not very heavy. Focusing on this narrow parameter space, we calculate the production cross sections of almost all the possible mono-$X$ and mono-$XX'$ processes at the LHC. The mono-$W\gamma$ process is shown to have high discovery potential with the help of the decay of the intermediate-mass charged Higgs boson into $W^\pm h_{1,2}$. A search strategy is designed to increase the potential discovery of the model for the mono-$W\gamma$ signal at both the HL-LHC and the FCC-hh. The optimal cut on $E_T^{\rm miss}/\sqrt{H_T}$ is suggested to maximize the signal significance, being about $0.76$ at the HL-LHC and about $7.5$ at the FCC-hh.

Highlights

  • One of the most convincing pieces of evidence that the standard model (SM) is not the final theory of particle physics is the observed dark matter (DM) in the Universe [1]

  • Focusing on the inert doublet model (IDM), we find that promoting the Z2 parity into a global Uð1Þ symmetry has two immediate consequences: (i) two neutral inert scalar bosons become DM particles; (ii) the number of model parameters is one less than that of the IDM with Z2 parity

  • The phenomenology of the IDM-Uð1Þ at the LHC is simple since the model contains only two neutral scalars (h1 and h2), which will play the role of missing energy, and the charged Higgs boson HÆ decaying into WÆðÃÞh1;2

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Summary

INTRODUCTION

One of the most convincing pieces of evidence that the standard model (SM) is not the final theory of particle physics is the observed dark matter (DM) in the Universe [1] Not knowing what it is yet, DM searches have been enthusiastically performed in three directions, direct detection, indirect detection, and its production at high energy colliders. With the result of the allowed (possibly very small) parameter space, we can assess all possible mono-X and mono-XpX0ffiffi luminosity LHC (HL-LHpCffiffi) at s [67] and the FCC-hh at s 1⁄4 100 processes at the high1⁄4 14 TeV with 3 ab−1 TeV and 30 ab−1 [68], and suggest a golden mode for this model.

BRIEF REVIEW OF THE IDM WITH A CONTINUOUS Uð1Þ SYMMETRY
THEORETICAL AND EXPERIMENTAL CONSTRAINTS
LEP experiments and electroweak precision data
Constraints from the theoretical stability and the Higgs precision data
DM relic density and direct DM detection
Production of the inert DM associated with gauge bosons at the LHC
WÆγEmT iss FINAL STATES AT THE LHC
CONCLUSIONS
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