<p>In this article, we examine the Standard Model extended by a <i>Y</i> = 0 real Higgs triplet, the ∆SM. It contains a <i>CP</i>-even neutral Higgs (∆<sup>0</sup>) and two charged Higgs bosons (∆<sup><i>±</i></sup>), which are quasi-degenerate in mass. We first study the theoretical constraints from vacuum stability and perturbative unitarity and then calculate the Higgs decays, including the loop-induced modes such as di-photons (<i>γγ</i>) and <i>Zγ</i>. In the limit of a small mixing between the SM Higgs and ∆<sup>0</sup>, the latter decays dominantly to <i>WW</i> and can have a sizable branching ratio to di-photon. The model predicts a positive definite shift in the <i>W</i> mass, which is compatible with the current global electroweak fit. At the Large Hadron Collider, it leads to a (<i>i</i>) stau-like signature from <i>pp</i> → ∆<sup>+</sup>∆<sup><i>−</i></sup> → <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_25877_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="59" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msup> <mi>τ</mi> <mo>+</mo> </msup> <msup> <mi>τ</mi> <mo>−</mo> </msup> <mi>ν</mi> <mover accent="true"> <mi>ν</mi> <mo stretchy="true">¯</mo> </mover> </math></EquationSource> <EquationSource Format="TEX">\( {\tau}^{+}{\tau}^{-}\nu \overline{\nu} \)</EquationSource> </InlineEquation>, (<i>ii</i>) multi-lepton final states from <i>pp</i> → <i>γ</i><sup>*</sup> → ∆<sup>+</sup>∆<sup><i>−</i></sup> → <i>W</i><sup>+</sup><i>W</i><sup><i>−</i></sup><i>ZZ</i> and <i>pp</i> → <i>W</i><sup>*</sup> → ∆<sup><i>±</i></sup>∆<sup>0</sup> → <i>W</i><sup><i>±</i></sup><i>ZW</i><sup>+</sup><i>W</i><sup><i>−</i></sup> as well as (<i>iii</i>) associated di-photon production from <i>pp</i> → <i>W</i><sup>*</sup> → ∆<sup><i>±</i></sup>(∆<sup>0</sup> → <i>γγ</i>). Concerning (<i>i</i>), the reinterpretation of the recent supersymmetric tau partner search by ATLAS and CMS excludes <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_25877_Article_IEq2.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="35" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msub> <mi>m</mi> <msup> <mtext>∆</mtext> <mo>±</mo> </msup> </msub> </math></EquationSource> <EquationSource Format="TEX">\( {m}_{\Delta ^{\pm }} \)</EquationSource> </InlineEquation> <i>&lt;</i> 110 GeV at 95% CL. From (<i>ii</i>), some of the signal regions of multi-lepton searches lead to bounds close to the predicted cross-section, but electroweak scale masses are still allowed. For (<i>iii</i>), the recast of the associated di-photon searches by ATLAS and a combined log-likelihood fit of signal and background to data find that out of the 25 signal regions, 10 provide relevant limits on Br(∆<sup>0</sup> → <i>γγ</i>) at the per cent level. Interestingly, 6 signal regions show weaker than expected limits at around 152 GeV, leading to a preference for a non-zero di-photon branching ratio of about (0.7<i>±</i>0.2)%.</p>

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Anatomy of the real Higgs triplet model

  • Saiyad Ashanujjaman,
  • Sumit Banik,
  • Guglielmo Coloretti,
  • Andreas Crivellin,
  • Siddharth P. Maharathy,
  • Bruce Mellado

摘要

In this article, we examine the Standard Model extended by a Y = 0 real Higgs triplet, the ∆SM. It contains a CP-even neutral Higgs (∆0) and two charged Higgs bosons (∆±), which are quasi-degenerate in mass. We first study the theoretical constraints from vacuum stability and perturbative unitarity and then calculate the Higgs decays, including the loop-induced modes such as di-photons (γγ) and . In the limit of a small mixing between the SM Higgs and ∆0, the latter decays dominantly to WW and can have a sizable branching ratio to di-photon. The model predicts a positive definite shift in the W mass, which is compatible with the current global electroweak fit. At the Large Hadron Collider, it leads to a (i) stau-like signature from pp → ∆+ τ + τ ν ν ¯ \( {\tau}^{+}{\tau}^{-}\nu \overline{\nu} \) , (ii) multi-lepton final states from ppγ* → ∆+W+WZZ and ppW* → ∆±0W±ZW+W as well as (iii) associated di-photon production from ppW* → ∆±(∆0γγ). Concerning (i), the reinterpretation of the recent supersymmetric tau partner search by ATLAS and CMS excludes m ± \( {m}_{\Delta ^{\pm }} \) < 110 GeV at 95% CL. From (ii), some of the signal regions of multi-lepton searches lead to bounds close to the predicted cross-section, but electroweak scale masses are still allowed. For (iii), the recast of the associated di-photon searches by ATLAS and a combined log-likelihood fit of signal and background to data find that out of the 25 signal regions, 10 provide relevant limits on Br(∆0γγ) at the per cent level. Interestingly, 6 signal regions show weaker than expected limits at around 152 GeV, leading to a preference for a non-zero di-photon branching ratio of about (0.7±0.2)%.