Triply charged Higgs bosons at a 100 TeV pp collider
Abstract In this work, we study the potential of searching for triply charged Higgs boson originating from a complex Higgs quadruplet in the final state with at least three same-sign leptons. A detailed collider analysis of the SM backgrounds and signals is performed at a 100 TeV pp collider for the...
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Format: | Article |
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SpringerOpen
2021-01-01
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Series: | European Physical Journal C: Particles and Fields |
Online Access: | https://doi.org/10.1140/epjc/s10052-021-08844-z |
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author | Junxing Pan Jung-Hsin Chen Xiao-Gang He Gang Li Jhih-Ying Su |
author_facet | Junxing Pan Jung-Hsin Chen Xiao-Gang He Gang Li Jhih-Ying Su |
author_sort | Junxing Pan |
collection | DOAJ |
description | Abstract In this work, we study the potential of searching for triply charged Higgs boson originating from a complex Higgs quadruplet in the final state with at least three same-sign leptons. A detailed collider analysis of the SM backgrounds and signals is performed at a 100 TeV pp collider for the triply charged Higgs boson mass below 1 TeV and the Higgs quadruplet vacuum expectation value $$v_\Delta $$ v Δ ranging from $$1.5\times 10^{-9}~\text {GeV}$$ 1.5 × 10 - 9 GeV to $$1.3~\text {GeV}$$ 1.3 GeV and the mass splitting $$\Delta m$$ Δ m between the nearby states of the Higgs quadruplet satisfying $$|\Delta m|\lesssim 30~\text {GeV}$$ | Δ m | ≲ 30 GeV . About $$100~\text {fb}^{-1}$$ 100 fb - 1 of data are required at most for $$5\sigma $$ 5 σ discovery. We also revisit the sensitivity at the Large Hadron Collider (LHC) and find that $$5\sigma $$ 5 σ discovery of the triply charged Higgs boson below 1 TeV can be reached for a relatively small $$v_\Delta $$ v Δ . For example, if $$v_\Delta =10^{-6}~\text {GeV}$$ v Δ = 10 - 6 GeV and $$\Delta m=0$$ Δ m = 0 , the integrated luminosity of $$330~\text {fb}^{-1}$$ 330 fb - 1 is needed. But for a relatively large $$v_\Delta $$ v Δ , i.e., $$v_\Delta \gtrsim 10^{-3}~\text {GeV}$$ v Δ ≳ 10 - 3 GeV , the triply charged Higgs boson above about 800 GeV cannot be discovered even in the high-luminosity LHC era. For $$\Delta m>0$$ Δ m > 0 , the cascade decays are open and the sensitivity can be improved depending on the value of $$v_\Delta $$ v Δ . |
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issn | 1434-6044 1434-6052 |
language | English |
last_indexed | 2024-12-20T02:06:22Z |
publishDate | 2021-01-01 |
publisher | SpringerOpen |
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series | European Physical Journal C: Particles and Fields |
spelling | doaj.art-1a47e88f3436415489f9ae41d13c84b32022-12-21T19:57:11ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522021-01-0181112110.1140/epjc/s10052-021-08844-zTriply charged Higgs bosons at a 100 TeV pp colliderJunxing Pan0Jung-Hsin Chen1Xiao-Gang He2Gang Li3Jhih-Ying Su4School of Physics and Information Engineering, Shanxi Normal UniversityDepartment of Physics, National Taiwan UniversitySchool of Physics and Information Engineering, Shanxi Normal UniversityDepartment of Physics, National Taiwan UniversityDepartment of Physics, National Taiwan UniversityAbstract In this work, we study the potential of searching for triply charged Higgs boson originating from a complex Higgs quadruplet in the final state with at least three same-sign leptons. A detailed collider analysis of the SM backgrounds and signals is performed at a 100 TeV pp collider for the triply charged Higgs boson mass below 1 TeV and the Higgs quadruplet vacuum expectation value $$v_\Delta $$ v Δ ranging from $$1.5\times 10^{-9}~\text {GeV}$$ 1.5 × 10 - 9 GeV to $$1.3~\text {GeV}$$ 1.3 GeV and the mass splitting $$\Delta m$$ Δ m between the nearby states of the Higgs quadruplet satisfying $$|\Delta m|\lesssim 30~\text {GeV}$$ | Δ m | ≲ 30 GeV . About $$100~\text {fb}^{-1}$$ 100 fb - 1 of data are required at most for $$5\sigma $$ 5 σ discovery. We also revisit the sensitivity at the Large Hadron Collider (LHC) and find that $$5\sigma $$ 5 σ discovery of the triply charged Higgs boson below 1 TeV can be reached for a relatively small $$v_\Delta $$ v Δ . For example, if $$v_\Delta =10^{-6}~\text {GeV}$$ v Δ = 10 - 6 GeV and $$\Delta m=0$$ Δ m = 0 , the integrated luminosity of $$330~\text {fb}^{-1}$$ 330 fb - 1 is needed. But for a relatively large $$v_\Delta $$ v Δ , i.e., $$v_\Delta \gtrsim 10^{-3}~\text {GeV}$$ v Δ ≳ 10 - 3 GeV , the triply charged Higgs boson above about 800 GeV cannot be discovered even in the high-luminosity LHC era. For $$\Delta m>0$$ Δ m > 0 , the cascade decays are open and the sensitivity can be improved depending on the value of $$v_\Delta $$ v Δ .https://doi.org/10.1140/epjc/s10052-021-08844-z |
spellingShingle | Junxing Pan Jung-Hsin Chen Xiao-Gang He Gang Li Jhih-Ying Su Triply charged Higgs bosons at a 100 TeV pp collider European Physical Journal C: Particles and Fields |
title | Triply charged Higgs bosons at a 100 TeV pp collider |
title_full | Triply charged Higgs bosons at a 100 TeV pp collider |
title_fullStr | Triply charged Higgs bosons at a 100 TeV pp collider |
title_full_unstemmed | Triply charged Higgs bosons at a 100 TeV pp collider |
title_short | Triply charged Higgs bosons at a 100 TeV pp collider |
title_sort | triply charged higgs bosons at a 100 tev pp collider |
url | https://doi.org/10.1140/epjc/s10052-021-08844-z |
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