Abstract

We study the implications of the LHC diphoton and Z+photon Higgs signals on the Higgs triplet model with Y=0. We discuss three different scenarios: (i) the observed boson is the light Higgs boson $h$; (ii) it is the heavy Higgs boson $H$; (iii) the observed signal is from the almost degenerate $h$ and $H$. We find that the inclusive Higgs diphoton rates in the first two scenarios can be enhanced or suppressed compared to the SM value, which can respectively fit the ATLAS and CMS diphoton data within $1\sigma$ range. The inclusive $ZZ^*$ rates are suppressed, which are outside $1\sigma$ range of ATLAS data and within $1\sigma$ range of CMS data. Meanwhile, another CP-even Higgs boson production rate can be suppressed enough not to be observed at the collider. For the third scenario, the Higgs diphoton rate is suppressed, which is outside $1\sigma$ range of ATLAS data, and the $ZZ^*$ rate equals to SM value approximately. In addition, we find that the two rates of $h\to \gamma\gamma$ and $h\to Z\gamma$ have the positive correlations for the three scenarios.

Highlights

  • We study the implications of the LHC diphoton and Z+photon Higgs signals on the Higgs triplet model with Y=0, which predicts two neutral CP-even Higgs bosons h, H and a pair of charged Higgs H±

  • The inclusive ZZ∗ rates are suppressed, which are outside 1σ range of ATLAS data and within 1σ range of CMS data

  • The Higgs diphoton rate is suppressed, which is outside 1σ range of ATLAS data, and the ZZ∗ rate equals to SM value approximately

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Summary

The Higgs diphoton and Zγ rates at the LHC

We take mh, mH , a2, b4 and vd, vt as the input parameters, which can determine the values of λ0, a1, mH±. The experimental data at the LEP gives the lower bound of the charged Higgs mass, mH± > 79.3 GeV [69, 70]. The cross sections and the decay widths of h(H) normalized to SM values can be given as σ ( gg → h(H) ) σSM ( gg → h(H) ). Compared to SM, in addition to the modified httand hW W couplings, the charged Higgs H± will alter the decays h → γγ and h → Zγ via the one-loop. The Higgs boson γγ, ZZ∗ and Zγ rates of HTM0 normalized to the SM values are respectively defined as. Where σ ( pp → h(H) ) is the total cross section of Higgs boson. We take code Hdecay to consider the relevant higher order QCD and electroweak corrections [71]

Scenario I
ATLAS 1σ
Scenario II
Scenario III
Conclusion
B The vacuum expectation values

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