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Heavy Higgs boson production and decay into top quarks at the LHC
High Energy Physics - Phenomenology · Submitted 24 Nov 2016
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim In our NLO calculation the QCD-Higgs interference is evaluated in the resonance region that provides the dominant part of the heavy Higgs-boson contributions.
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The abstract, sentence by sentence
In this contribution we report on the calculation of the next-to-leading order (NLO) QCD corrections to the hadro-production of heavy neutral Higgs bosons and their decay into top-quark pairs within the type-II two-Higgs-doublet extension of the standard model (SM). We take into account the contributions from resonant Higgs boson production, the non-resonant SM $t\bar{t}$ background as well as the interference of these two contributions. The NLO corrections to the signal and interference contributions are calculated by applying the heavy top-quark mass ($m_t$) limit including an effective rescaling. In our NLO calculation the QCD-Higgs interference is evaluated in the resonance region that provides the dominant part of the heavy Higgs-boson contributions. Evaluating representative $CP$-conserving and $CP$-violating parameter scenarios within the two-Higgs-doublet model (2HDM) we present results for different distributions and, in addition, for observables that depend on the top-quark spin.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In this contribution we report on the calculation of the next-to-leading order (NLO) QCD corrections to the hadro-production of heavy neutral Higgs bosons and their decay into top-quark pairs within the type-II two-Higgs-doublet extension of the standard model (SM). | contribution 1.00 | 0.95 | 0.11 | asserted 0.99 |
| s1 | We take into account the contributions from resonant Higgs boson production, the non-resonant SM $t\bar{t}$ background as well as the interference of these two contributions. | method 0.65 | 0.82 | 0.04 | asserted 0.99 |
| s2 | The NLO corrections to the signal and interference contributions are calculated by applying the heavy top-quark mass ($m_t$) limit including an effective rescaling. | method 1.00 | 0.93 | 0.05 | asserted 1.00 |
| s3 | In our NLO calculation the QCD-Higgs interference is evaluated in the resonance region that provides the dominant part of the heavy Higgs-boson contributions. | method 0.92 | 0.93 | 0.09 | asserted 1.00 |
| s4 | Evaluating representative $CP$-conserving and $CP$-violating parameter scenarios within the two-Higgs-doublet model (2HDM) we present results for different distributions and, in addition, for observables that depend on the top-quark spin. | result 0.51 | 0.94 | 0.12 | asserted 0.99 |
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The paper
Original abstract
In this contribution we report on the calculation of the next-to-leading order (NLO) QCD corrections to the hadro-production of heavy neutral Higgs bosons and their decay into top-quark pairs within the type-II two-Higgs-doublet extension of the standard model (SM). We take into account the contributions from resonant Higgs boson production, the non-resonant SM $t\bar{t}$ background as well as the interference of these two contributions. The NLO corrections to the signal and interference contributions are calculated by applying the heavy top-quark mass ($m_t$) limit including an effective rescaling. In our NLO calculation the QCD-Higgs interference is evaluated in the resonance region that provides the dominant part of the heavy Higgs-boson contributions. Evaluating representative $CP$-conserving and $CP$-violating parameter scenarios within the two-Higgs-doublet model (2HDM) we present results for different distributions and, in addition, for observables that depend on the top-quark spin.
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What this paper does with the arXiv papers it cites
Papers whose main result relates to this one's
States the same result 1 paper
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Using representative CP-conserving as well as CP-violating parameter scenarios phenomenological results are presented for different observables.
Heavy Higgs boson resonances and their decay into top quarks at the LHC · 0.82
What it cites · 7 sentences without a confident label
Cites as background 3 papers
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Now that the standard-model like Higgs boson has been experimentally [ref] established at the LHC, the ongoing and future investigation of the scalar sector—including the search for additional spin-zero bosons—remains one of the central research goals at the LHC.
Precise determination of the mass of the Higgs boson and tests of compatibility of its couplings with the standard model predictions using proton collisions at 7 and 8 TeV · Introduction · 0.92
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Now that the standard-model like Higgs boson has been experimentally [ref] established at the LHC, the ongoing and future investigation of the scalar sector—including the search for additional spin-zero bosons—remains one of the central research goals at the LHC.
Measurements of the Higgs boson production and decay rates and coupling strengths using $pp$ collision data at $\sqrt{s}=7$ and $8$ TeV in the ATLAS experiment · Introduction · 0.92
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Details of the 2HDM in general and type-II in particular can be found in the literature, e.g. [ref] .
Theory and phenomenology of two-Higgs-doublet models · Two-Higgs-doublet model scenarios · 1.00
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