<p>In the type-I two-Higgs-doublet model, the pseudoscalar <i>A</i> can act as a long-lived particle (LLP) for sufficiently large values of tan <i>β</i>. At the LHC, the <i>A</i> particles are predominantly produced in pairs through <i>pp</i> → <i>W</i><sup>∗</sup>/<i>Z</i><sup>∗</sup> → <i>H</i><sup><i>±</i></sup>/<i>H A</i>, with subsequent decays <i>H</i><sup>±</sup>/<i>H</i> → <i>W</i><sup>±</sup>/<i>Z A</i>. For the mass range of our interest, 10 GeV ≲ <i>m</i><sub><i>A</i></sub> ≲ 100 GeV, the pseudoscalar <i>A</i> typically decays into a pair of bottom quarks after traveling a macroscopic distance from its production point, giving rise to displaced-vertex (DV) signatures inside the inner detector. We perform Monte Carlo simulations of signal events with DVs plus jets, and assess the discovery prospects of <i>A</i> as an LLP at the ATLAS and CMS experiments. Our findings show that a substantial portion of the parameter space with <i>m</i><sub><i>A</i></sub> &gt; 10 GeV has already been excluded by LHC Run-2 data, while the high-luminosity LHC will be able to probe broader regions.</p>

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Probing a long-lived pseudoscalar in type-I 2HDM with displaced vertices and jets at the LHC

  • Lei Wang,
  • Zeren Simon Wang,
  • Haotian Xu

摘要

In the type-I two-Higgs-doublet model, the pseudoscalar A can act as a long-lived particle (LLP) for sufficiently large values of tan β. At the LHC, the A particles are predominantly produced in pairs through ppW/ZH±/H A, with subsequent decays H±/HW±/Z A. For the mass range of our interest, 10 GeV ≲ mA ≲ 100 GeV, the pseudoscalar A typically decays into a pair of bottom quarks after traveling a macroscopic distance from its production point, giving rise to displaced-vertex (DV) signatures inside the inner detector. We perform Monte Carlo simulations of signal events with DVs plus jets, and assess the discovery prospects of A as an LLP at the ATLAS and CMS experiments. Our findings show that a substantial portion of the parameter space with mA > 10 GeV has already been excluded by LHC Run-2 data, while the high-luminosity LHC will be able to probe broader regions.