2016/10/31 by S. Mohammad Moosavi Nejad, S. Abbaspour
Physics and Astronomy · #Boson #Hadron #Higgs boson #High-Energy Particle Collisions Research #Large Hadron Collider #Massless particle #Nuclear physics #Particle physics #Particle physics theoretical and experimental studies #Physics #Physics beyond the Standard Model #Quantum Chromodynamics and Particle Interactions #Quark #Top quark #hep-ph
paper · pdf · doi:10.1016/j.nuclphysb.2017.05.009
published as Nuclear Physics B921 (2017) 86-103 · 10 pages, 6 figures. arXiv admin note: text overlap with arXiv:1611.08017
openalex created_date 2016/12/08 · arxiv created 2016/12/13 · openalex publication_date 2017/05/24 · arxiv updated 2017/06/01 · openalex updated_date 2026/08/05
In recent years, searches for the light and heavy charged Higgs bosons have been done by the ATLAS and the CMS collaborations at the Large Hadron Collider (LHC) in proton–proton collision. Nevertheless, a definitive search is a program that still has to be carried out at the LHC. The experimental observation of charged Higgs bosons would indicate physics beyond the Standard Model. In the present work, we study the scaled-energy distribution of bottom-flavored mesons (B) inclusively produced in polarized top quark decays into a light charged Higgs boson and a massless bottom quark at next-to-leading order in the two-Higgs-doublet model; t(↑)→bH+→BH++X. This spin-dependent energy distribution is studied in a specific helicity coordinate system where the polarization vector of the top quark is measured with respect to the direction of the Higgs momentum. The study of these energy distributions could be considered as a new channel to search for the charged Higgs bosons at the LHC. For our numerical analysis and phenomenological predictions, we restrict ourselves to the unexcluded regions of the MSSM mH+−tanβ parameter space determined by the recent results of the CMS [13] and ATLAS [14] collaborations.