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2021
DOI: 10.1007/jhep06(2021)183
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The forgotten channels: charged Higgs boson decays to a W± and a non-SM-like Higgs boson

Abstract: The presence of charged Higgs bosons is a generic prediction of multiplet extensions of the Standard Model (SM) Higgs sector. Focusing on the Two-Higgs-Doublet-Model (2HDM) with type I and lepton-specific Yukawa sectors, we discuss the charged Higgs boson collider phenomenology in the theoretically and experimentally viable parameter space. While almost all existing experimental searches at the LHC target the fermionic decays of charged Higgs bosons, we point out that the bosonic decay channels — especially th… Show more

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Cited by 33 publications
(21 citation statements)
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“…If it is off-shell, the charged lepton emerging from it might be soft (as already remarked upon), like in BP4-BP10. • For these BPs, the main production process of a charged Higgs boson is pp → H ± h, which cross section can be up to one order of magnitude larger than those of pp → H ± A and pp → H ± H ∓ , which are alternative discovery modes in this region of 2HDM Type-I parameter space [25][26][27]. Therefore, in the present analysis, we will focus on the W ± + 4γ signature stemming from the pp → H ± h production process only.…”
Section: Parameter Space Scansmentioning
confidence: 99%
“…If it is off-shell, the charged lepton emerging from it might be soft (as already remarked upon), like in BP4-BP10. • For these BPs, the main production process of a charged Higgs boson is pp → H ± h, which cross section can be up to one order of magnitude larger than those of pp → H ± A and pp → H ± H ∓ , which are alternative discovery modes in this region of 2HDM Type-I parameter space [25][26][27]. Therefore, in the present analysis, we will focus on the W ± + 4γ signature stemming from the pp → H ± h production process only.…”
Section: Parameter Space Scansmentioning
confidence: 99%
“…As discussed in the beginning of the section, the charged Higgs will be produced via Drell-Yan process: pp → W ± * → H ± H/A and and the subsequent bosonic decay of the Higgses yield a same sign trilepton signal (3 ± + E T ) in association with additional jets and/or leptons. We applied uniform K-factor of 1.35 [36] for the signal cross-section. For event generation, the type-I 2HDM model is implemented in FeynRules-2.3 [62] and both the signal and the background events are generated using MadGraph5-aMC@NLO-2.6.6 [63,64].…”
Section: Event Generation and Signal Selectionmentioning
confidence: 99%
“…For type-I or fermiophobic case, the H ± tb coupling is tan β suppressed, and for large tan β, the channel becomes irrelevant. On the other hand, the electroweak production of H ± [32][33][34][35][36] in association with a neutral (pseudo)scalar depends on the gauge coupling and dominates over the top associated production at large tan β. For type-I 2HDM, the electroweak production of a light charged Higgs can give rise to multi-photon or multi-boson final state [37][38][39][40][41][42][43].…”
mentioning
confidence: 99%
“…2 Some unconventional decay channels of the heavy H ± in the 2HDM have also been studied, such as H ± → W ± A [32], H ± → W ± γ [33], and H ± → t b [34][35][36]. 3 In Ref.…”
Section: Introductionmentioning
confidence: 99%