Observability of light charged Higgs decay to muon in top quark pair events at LHC

The European Physical Journal C - In this paper the charged Higgs signal through the decay to a pair of muon and neutrino (H ±→μν) is analyzed. The analysis attempts to...     

Bounds on a top quark with charged Higgs decay

If the top quark decays to a charged Higgs boson t→bH⁺, semileptonic decay signatures are suppressed and the mass bounds set by the UA1 top search are evaded. However the charged Higgs decay mode H⁺→τ⁺ν_τ gives a missing-ϱ_T signature; depending on the decay branching fraction and using the UA1 limits on new physics contributions to missing-ϱ_T, we set bounds on the top mass in this scenario. We also evaluate the feasibility of seeking visible-τ-jet signals for top at a pp̄ collider.     

Higgs boson bremsstrahlung in top quark decay

In top quark decay a neutral Higgs boson may be emitted in bremsstrahlung from the top quark or from the W-boson. We evaluate the branching fraction for this hitherto overlooked t→H⁰bW⁺ decay mode, where the W⁺ can be virtual or real. It has the standard model values of 0.02%, 0.2%, 0.8% for m_t=50, 100, 200 GeVand m_H=10 GeV.     

Heavy top quark decay into a charged Higgs scalar and a photon (gluon)

We consider the decay of a heavy top quark into a charged Higgs scalar and a hard photon (gluon)tH ⁺ b(g). We give the general result for fermions of arbitrary mass. Our results for the differential decay rate for these two processes are remarkably simple. The radiation amplitude zero (RAZ) factorization is explicit but there is no RAZ for these processes because of the presence of opposite-sign charges. We obtain a branching ratio of 0.063% for bH⁺ and 5.6% for bH⁺g. Thus both decays should be relatively easy to see at the SSC.     

The hadronic tau decay signature of a heavy charged Higgs boson at LHC

The hadronic tau decay channel offers by far the best signature for heavy charged Higgs boson search at the LHC in the large tanβ region. By exploiting the distinct polarization of the tau and its large transverse mass, along with the accompanying missing–p_T, one can probe for a charged Higgs boson up to a mass of about 600 GeV in an essentially background-free environment. The transverse mass distribution of the tau jet also provides a fairly unambiguous estimate of the charged Higgs boson mass.     

Observability of Charged Higgs Contribution in t-channel Single Top at LHC

In this paper, the charged Higgs contribution in t-channel single top production is studied. The production process is a t-channel single top event with charged Higgs exchange. Therefore the signal is similar with Standard Model single top production in terms of the final state. In the first step, the signal cross section is calculated and compared to the other main production processes which are used for a heavy charged Higgs search at LHC, i.e., \(pp\rightarrow t\bar {b}H^{-}\) and \(pp\rightarrow H^{+} \rightarrow t\bar {b}\). In the next step, an event generation and analysis is applied on signal and background events, in order to estimate the signal significance. The signal cross section is typically smaller than the associated production (\(t\bar {b}H^{-}\)) and resonance production (\(t\bar {b}\)) by a factor of 10^?3 and ranges from 10 f b to 1 f b for charged Higgs mass from 200 to 500 GeV at tanβ = 50. Due to the small cross section of signal events and large SM background, the signal significance is small even after a dedicated kinematic analysis and selection of events, however, tanβ values above 120 can be excluded at an integrated luminosity of 3000 f b ^?1.     

Trilepton+top signal from chargino-neutralino decays of MSSM charged Higgs bosons at the LHC

We perform for the Large Hadron Collider (LHC) a detailed study of charged Higgs boson production via the top-bottom quark associated mode followed by decays into a chargino and a neutralino, with masses and couplings as given by the general minimal supersymmetric standard model (MSSM). We focus our attention on the region of parameter space with and intermediate values of , where identification of via decays into standard model (SM) particles has proven to be ineffective. Modelling the CMS detector, we find that a signature consisting of three hard leptons accompanied by a hadronically reconstructed top quark plus substantial missing transverse energy, which may result from decays, can be made viable over a large variety of initially overwhelming SM and MSSM backgrounds, provided MSSM input parameters are favourable: notably, small and light sleptons are important prerequisites. We quantify these statements by performing a fairly extensive scan of the parameter space, including realistic hadron-level simulations, and delineate some potential discovery regions.Received: 16 April 2003, Revised: 23 June 2003, Published online: 29 August 2003S. Moretti: Formerly at: Theory Division, CERN, 1211 Geneva 23, Switzerland and Institute for Particle Physics Phenomenology, University of Durham, Durham DH1 3LE, UK     

CP asymmetries in top quark pair production and decay: contributions from neutral Higgs boson and gluino exchange

Zeitschrift für Physik C Particles and Fields - For $$e^ + e^ - \to \bar tt$$ with subsequent semileptonic $$\bar t$$ and nonleptonic $$\bar t$$ decay and vice versa we investigate a few...     

Yukawa corrections to the charged Higgs boson production in association with the top quark at hadron colliders

We calculate the Yukawa corrections of order to charged Higgs boson production in association with a top quark at the Tevatron and the LHC. The corrections are not very sensitive to the mass of the charged Higgs boson and can exceed for low values of , where the contribution of the top quark is large, and high values of where the contribution of the bottom quark becomes large. These Yukawa corrections could be significant for charged Higgs boson searches based on this production process, particularly at the LHC where the cross section is relatively large. Received: 12 October 1999 / Revised version: 3 December 1999 / Published online: 6 April 2000     

Production of charged Higgs bosons at LHC in light-quark annihilation

The CMS potential (at LHC) for seeking the production of a charged Higgs boson is investigated for large values of tan β (between 20 and 50) and a relatively light charged Higgs boson M _H = 200–400 GeV). A simple parametrization is proposed for the

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distributions of signal and background events. The possibility of measuring the mass of the charged Higgs boson and tan β is investigated.

     

Ways to detect a light Higgs boson at the LHC

We summarize the possible processes which may be used to search for a Higgs boson, of mass in the range 114-130 GeV, at the LHC. We discuss, in detail, two processes with rapidity gaps: exclusive Higgs production with tagged outgoing protons and production by Weak Boson Fusion, in each case taking as the signal. We make an extensive study of all possible backgrounds, and discuss the relevant experimental issues. We emphasize the special features of these signals, and of their background processes, and show that they could play an important role in identifying a light Higgs boson at the LHC. Received: 5 July 2002 / Published online: 30 August 2002