Abstract

We consider a conformal complex singlet extension of the Standard Model with a Higgs portal interaction. The global $U(1)$ symmetry of the complex singlet can be either broken or unbroken and we study each scenario. In the unbroken case, the global $U(1)$ symmetry protects the complex singlet from decaying, leading to an ideal cold dark matter candidate with approximately 100 GeV mass along with a significant proportion of thermal relic dark matter abundance. In the broken case, we have developed a renormalization-scale optimization technique to significantly narrow the parameter space and in some situations, provide unique predictions for all the model's couplings and masses. We have found there exists a second Higgs boson with a mass of approximately $550\,\rm{GeV}$ that mixes with the known $125\,\rm{GeV}$ Higgs with a large mixing angle $\sin\theta\approx 0.47$ consistent with current experimental limits. The imaginary part of the complex singlet in the broken case could provide axion dark matter for a wide range of models. Upon including interactions of the complex scalar with an additional vector-like fermion, we explore the possibility of a diphoton excess in both the unbroken and the broken cases. In the unbroken case, the model can provide a natural explanation for diphoton excess if extra terms are introduced providing extra contributions to the singlet mass. In the broken case, we find a set of coupling solutions that yield a second Higgs boson of mass $720\,\rm{GeV}$ and an $830\,\rm{GeV}$ extra vector-like fermion $F$, which is able to address the $750\,\rm{GeV}$ LHC diphoton excess. We also provide criteria to determine the symmetry breaking pattern in both the Higgs and hidden sectors.

Highlights

  • Unbroken phaseS decay is protected by the U (1) global symmetry, making it an ideal cold dark matter candidate when yS is set to zero

  • We consider here two main scenarios depending on whether or not the global U(1) symmetry is spontaneously broken by a vacuum expectation value of the hidden-sector complex field

  • We have explored the possibility of diphoton excess in the unbroken case and find that a natural explanation of the diphoton excess can be provided only if extra terms are introduced in the singlet sector to increase the singlet mass

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Summary

Unbroken phase

S decay is protected by the U (1) global symmetry, making it an ideal cold dark matter candidate when yS is set to zero. This case may provide a natural explanation for the diphoton excess when yS is turned on since S will not mix with the Higgs and the decay channels of S to other SM particles are greatly suppressed. In the unbroken case, there is no mixing between the singlet and the Higgs field, thereby greatly suppressing the decay processes of the S to SM particles, in turn ideally satisfying the bounds in ref.

Broken phase
Findings
Summary

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