Higgs interference effects in top-quark pair production in the 1HSM

A bstract We present a next-to-leading-order (NLO) study of the process pp ( → { h 1 , h 2 }) → t t ¯ + X in the 1-Higgs-singlet extension of the Standard Model with an additional heavy Higgs boson h 2 that mixes with the light Higgs boson h 1 . This process is subject to large interference effects...

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Published inThe journal of high energy physics Vol. 2024; no. 8; pp. 112 - 30
Main Authors Banfi, Andrea, Kauer, Nikolas, Lind, Alexander, Lindert, Jonas M., Wood, Ryan
Format Journal Article
LanguageEnglish
Published Berlin/Heidelberg Springer Berlin Heidelberg 14.08.2024
Springer Nature B.V
Springer
SpringerOpen
Subjects
Classical and Quantum Gravitation
Elementary Particles
Higgs bosons
Higgs Production
High Energy Physics - Experiment
High Energy Physics - Phenomenology
Higher-Order Perturbative Calculations
Large Hadron Collider
Multi-Higgs Models
Pair production
Physics
Physics and Astronomy
Quantum chromodynamics
Quantum Field Theories
Quantum Field Theory
Quantum Physics
Quarks
Regular Article - Theoretical Physics
Relativity Theory
Resonance
Standard model (particle physics)
String Theory
Higgs Production
Multi-Higgs Models
Higher-Order Perturbative Calculations
numerical calculations
new physics
upgrade
quantum chromodynamics
mass
infrared
dip
CERN LHC Coll
pair production
benchmark
structure
heavy
1
top
background
effect
Higgs particle
GeV
higher-order
interference
correction
stability
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Abstract A bstract We present a next-to-leading-order (NLO) study of the process pp ( → { h 1 , h 2 }) → t t ¯ + X in the 1-Higgs-singlet extension of the Standard Model with an additional heavy Higgs boson h 2 that mixes with the light Higgs boson h 1 . This process is subject to large interference effects between loop-induced Higgs-mediated amplitudes and the QCD continuum background which tend to overcompensate any resonance contributions. A reliable modelling of the resulting top-pair invariant mass shapes requires the inclusion of higher-order QCD corrections, which are presented here. The computation of these NLO corrections is exact in all contributions but in the class of non-factorisable two-loop diagrams which are included in an approximate way such that all infrared singular limits are preserved. We present numerical results for several benchmark points with heavy Higgs masses in the range 700–3000 GeV considering the production of stable top quarks. We find that the interference effects dominate the BSM signal yielding sharp dip structures instead of resonance peaks. The significance and excludability of the BSM effect is explored for the LHC Run 2, Run 3 and HL-LHC.
AbstractList Abstract We present a next-to-leading-order (NLO) study of the process pp (→ {h 1, h 2}) → t t ¯ $$ t\overline{t} $$ + X in the 1-Higgs-singlet extension of the Standard Model with an additional heavy Higgs boson h 2 that mixes with the light Higgs boson h 1. This process is subject to large interference effects between loop-induced Higgs-mediated amplitudes and the QCD continuum background which tend to overcompensate any resonance contributions. A reliable modelling of the resulting top-pair invariant mass shapes requires the inclusion of higher-order QCD corrections, which are presented here. The computation of these NLO corrections is exact in all contributions but in the class of non-factorisable two-loop diagrams which are included in an approximate way such that all infrared singular limits are preserved. We present numerical results for several benchmark points with heavy Higgs masses in the range 700–3000 GeV considering the production of stable top quarks. We find that the interference effects dominate the BSM signal yielding sharp dip structures instead of resonance peaks. The significance and excludability of the BSM effect is explored for the LHC Run 2, Run 3 and HL-LHC.
We present a next-to-leading-order (NLO) study of the process $pp \; ( \to \{ h_1, h_2 \}) \to t\bar{t} + X$ in the 1-Higgs-singlet extension of the Standard Model with an additional heavy Higgs boson $h_2$ that mixes with the light Higgs boson $h_1$. This process is subject to large interference effects between loop-induced Higgs-mediated amplitudes and the QCD continuum background which tend to overcompensate any resonance contributions. A reliable modelling of the resulting top-pair invariant mass shapes requires the inclusion of higher-order QCD corrections, which are presented here. The computation of these NLO corrections is exact in all contributions but in the class of non-factorisable two-loop diagrams which are included in an approximate way such that all infrared singular limits are preserved. We present numerical results for several benchmark points with heavy Higgs masses in the range $700$--$3000$ GeV considering the production of stable top quarks. We find that the interference effects dominate the BSM signal yielding sharp dip structures instead of resonance peaks. The significance and excludability of the BSM effect is explored for the LHC Run 2, Run 3 and HL-LHC.
We present a next-to-leading-order (NLO) study of the process pp (→ {h1, h2}) →tt¯ + X in the 1-Higgs-singlet extension of the Standard Model with an additional heavy Higgs boson h2 that mixes with the light Higgs boson h1. This process is subject to large interference effects between loop-induced Higgs-mediated amplitudes and the QCD continuum background which tend to overcompensate any resonance contributions. A reliable modelling of the resulting top-pair invariant mass shapes requires the inclusion of higher-order QCD corrections, which are presented here. The computation of these NLO corrections is exact in all contributions but in the class of non-factorisable two-loop diagrams which are included in an approximate way such that all infrared singular limits are preserved. We present numerical results for several benchmark points with heavy Higgs masses in the range 700–3000 GeV considering the production of stable top quarks. We find that the interference effects dominate the BSM signal yielding sharp dip structures instead of resonance peaks. The significance and excludability of the BSM effect is explored for the LHC Run 2, Run 3 and HL-LHC.
We present a next-to-leading-order (NLO) study of the process pp ( → { h 1 , h 2 }) → $$ t\overline{t} $$ t t ¯ + X in the 1-Higgs-singlet extension of the Standard Model with an additional heavy Higgs boson h 2 that mixes with the light Higgs boson h 1 . This process is subject to large interference effects between loop-induced Higgs-mediated amplitudes and the QCD continuum background which tend to overcompensate any resonance contributions. A reliable modelling of the resulting top-pair invariant mass shapes requires the inclusion of higher-order QCD corrections, which are presented here. The computation of these NLO corrections is exact in all contributions but in the class of non-factorisable two-loop diagrams which are included in an approximate way such that all infrared singular limits are preserved. We present numerical results for several benchmark points with heavy Higgs masses in the range 700–3000 GeV considering the production of stable top quarks. We find that the interference effects dominate the BSM signal yielding sharp dip structures instead of resonance peaks. The significance and excludability of the BSM effect is explored for the LHC Run 2, Run 3 and HL-LHC.
A bstract We present a next-to-leading-order (NLO) study of the process pp ( → { h 1 , h 2 }) → t t ¯ + X in the 1-Higgs-singlet extension of the Standard Model with an additional heavy Higgs boson h 2 that mixes with the light Higgs boson h 1 . This process is subject to large interference effects between loop-induced Higgs-mediated amplitudes and the QCD continuum background which tend to overcompensate any resonance contributions. A reliable modelling of the resulting top-pair invariant mass shapes requires the inclusion of higher-order QCD corrections, which are presented here. The computation of these NLO corrections is exact in all contributions but in the class of non-factorisable two-loop diagrams which are included in an approximate way such that all infrared singular limits are preserved. We present numerical results for several benchmark points with heavy Higgs masses in the range 700–3000 GeV considering the production of stable top quarks. We find that the interference effects dominate the BSM signal yielding sharp dip structures instead of resonance peaks. The significance and excludability of the BSM effect is explored for the LHC Run 2, Run 3 and HL-LHC.
ArticleNumber 112
Author Banfi, Andrea
Lind, Alexander
Kauer, Nikolas
Lindert, Jonas M.
Wood, Ryan
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  surname: Wood
  fullname: Wood, Ryan
  organization: Department of Physics and Astronomy, University of Sussex
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Issue 8
Keywords Higgs Production
Multi-Higgs Models
Higher-Order Perturbative Calculations
numerical calculations
new physics
upgrade
quantum chromodynamics
mass
infrared
dip
CERN LHC Coll
pair production
benchmark
structure
heavy
1
top
background
effect
Higgs particle
GeV
higher-order
interference
correction
stability
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Snippet A bstract We present a next-to-leading-order (NLO) study of the process pp ( → { h 1 , h 2 }) → t t ¯ + X in the 1-Higgs-singlet extension of the Standard...
We present a next-to-leading-order (NLO) study of the process pp ( → { h 1 , h 2 }) → $$ t\overline{t} $$ t t ¯ + X in the 1-Higgs-singlet extension of the...
We present a next-to-leading-order (NLO) study of the process pp (→ {h1, h2}) →tt¯ + X in the 1-Higgs-singlet extension of the Standard Model with an...
We present a next-to-leading-order (NLO) study of the process $pp \; ( \to \{ h_1, h_2 \}) \to t\bar{t} + X$ in the 1-Higgs-singlet extension of the Standard...
Abstract We present a next-to-leading-order (NLO) study of the process pp (→ {h 1, h 2}) → t t ¯ $$ t\overline{t} $$ + X in the 1-Higgs-singlet extension of...
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SubjectTerms Classical and Quantum Gravitation
Elementary Particles
Higgs bosons
Higgs Production
High Energy Physics - Experiment
High Energy Physics - Phenomenology
Higher-Order Perturbative Calculations
Large Hadron Collider
Multi-Higgs Models
Pair production
Physics
Physics and Astronomy
Quantum chromodynamics
Quantum Field Theories
Quantum Field Theory
Quantum Physics
Quarks
Regular Article - Theoretical Physics
Relativity Theory
Resonance
Standard model (particle physics)
String Theory
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Title Higgs interference effects in top-quark pair production in the 1HSM
URI https://link.springer.com/article/10.1007/JHEP08(2024)112
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