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
Summary
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.
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