Resonant heavy Higgs searches at the HL-LHC

Abstract In this work, we show the importance of searches for heavy resonant scalars (H) and pseudoscalars (A). Taking cue from the present searches, we make projections for searches in an extended scalar sector at the high luminosity run of the Large Hadron Collider. We study the three most relevan...

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Main Authors: Amit Adhikary, Shankha Banerjee, Rahool Kumar Barman, Biplob Bhattacherjee
Format: Article
Language:English
Published: SpringerOpen 2019-09-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP09(2019)068
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spelling doaj-c624c74d8c3049df98be1ee9c94e7b2d2020-11-25T03:37:44ZengSpringerOpenJournal of High Energy Physics1029-84792019-09-012019916710.1007/JHEP09(2019)068Resonant heavy Higgs searches at the HL-LHCAmit Adhikary0Shankha Banerjee1Rahool Kumar Barman2Biplob Bhattacherjee3Centre for High Energy Physics, Indian Institute of ScienceInstitute for Particle Physics Phenomenology, Department of Physics, Durham UniversityCentre for High Energy Physics, Indian Institute of ScienceCentre for High Energy Physics, Indian Institute of ScienceAbstract In this work, we show the importance of searches for heavy resonant scalars (H) and pseudoscalars (A). Taking cue from the present searches, we make projections for searches in an extended scalar sector at the high luminosity run of the Large Hadron Collider. We study the three most relevant search channels, i.e., H → hh, H/A → t t ¯ $$ \overline{t} $$ and bbH/A. Upon studying multifarious final states for the resonant double Higgs production, we find that the b b ¯ $$ \overline{b} $$ γγ (σ(pp → H → hh) ∈ [81.27, 14.45] fb for m H ∈ [300, 600] GeV at 95% C.L.) and b b ¯ $$ \overline{b} $$ b b ¯ $$ \overline{b} $$ ([5.4, 2.5] fb for m H ∈ [800, 1000] GeV at 95% C.L.) channels are the most constraining. For the b b ¯ $$ \overline{b} $$ H channel, we can exclude σ(pp → b b ¯ $$ \overline{b} $$ H) ∈ [22.2, 3.7] fb for m H ∈ [300, 500] GeV. Finally, we consider the phenomenological Minimal Supersymmetric Standard Model as an example and impose various present constraints and our future direct search-limits and obtain strong constraints on the m A − tan β parameter space, where m A and tan β are respectively the mass of the pseudoscalar and the ratio of the vacuum expectation values of the two Higgs doublets. Assuming that the heavy Higgs boson decays only to Standard Model (SM) states, we find that the H → hh → b b ¯ $$ \overline{b} $$ γγ (H → t t ¯ $$ \overline{t} $$ ) channel excludes tan β as low as 4 (m A ∈ [400,800]GeV) at 95% CL. This weakens up to ∼ 5.5 when the b b ¯ $$ \overline{b} $$ H channel dominates. Upon allowing for non-SM decay modes, the limits weaken.http://link.springer.com/article/10.1007/JHEP09(2019)068Beyond Standard ModelHiggs PhysicsSupersymmetric Standard Model
collection DOAJ
language English
format Article
sources DOAJ
author Amit Adhikary
Shankha Banerjee
Rahool Kumar Barman
Biplob Bhattacherjee
spellingShingle Amit Adhikary
Shankha Banerjee
Rahool Kumar Barman
Biplob Bhattacherjee
Resonant heavy Higgs searches at the HL-LHC
Journal of High Energy Physics
Beyond Standard Model
Higgs Physics
Supersymmetric Standard Model
author_facet Amit Adhikary
Shankha Banerjee
Rahool Kumar Barman
Biplob Bhattacherjee
author_sort Amit Adhikary
title Resonant heavy Higgs searches at the HL-LHC
title_short Resonant heavy Higgs searches at the HL-LHC
title_full Resonant heavy Higgs searches at the HL-LHC
title_fullStr Resonant heavy Higgs searches at the HL-LHC
title_full_unstemmed Resonant heavy Higgs searches at the HL-LHC
title_sort resonant heavy higgs searches at the hl-lhc
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2019-09-01
description Abstract In this work, we show the importance of searches for heavy resonant scalars (H) and pseudoscalars (A). Taking cue from the present searches, we make projections for searches in an extended scalar sector at the high luminosity run of the Large Hadron Collider. We study the three most relevant search channels, i.e., H → hh, H/A → t t ¯ $$ \overline{t} $$ and bbH/A. Upon studying multifarious final states for the resonant double Higgs production, we find that the b b ¯ $$ \overline{b} $$ γγ (σ(pp → H → hh) ∈ [81.27, 14.45] fb for m H ∈ [300, 600] GeV at 95% C.L.) and b b ¯ $$ \overline{b} $$ b b ¯ $$ \overline{b} $$ ([5.4, 2.5] fb for m H ∈ [800, 1000] GeV at 95% C.L.) channels are the most constraining. For the b b ¯ $$ \overline{b} $$ H channel, we can exclude σ(pp → b b ¯ $$ \overline{b} $$ H) ∈ [22.2, 3.7] fb for m H ∈ [300, 500] GeV. Finally, we consider the phenomenological Minimal Supersymmetric Standard Model as an example and impose various present constraints and our future direct search-limits and obtain strong constraints on the m A − tan β parameter space, where m A and tan β are respectively the mass of the pseudoscalar and the ratio of the vacuum expectation values of the two Higgs doublets. Assuming that the heavy Higgs boson decays only to Standard Model (SM) states, we find that the H → hh → b b ¯ $$ \overline{b} $$ γγ (H → t t ¯ $$ \overline{t} $$ ) channel excludes tan β as low as 4 (m A ∈ [400,800]GeV) at 95% CL. This weakens up to ∼ 5.5 when the b b ¯ $$ \overline{b} $$ H channel dominates. Upon allowing for non-SM decay modes, the limits weaken.
topic Beyond Standard Model
Higgs Physics
Supersymmetric Standard Model
url http://link.springer.com/article/10.1007/JHEP09(2019)068
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AT shankhabanerjee resonantheavyhiggssearchesatthehllhc
AT rahoolkumarbarman resonantheavyhiggssearchesatthehllhc
AT biplobbhattacherjee resonantheavyhiggssearchesatthehllhc
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