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Discovering the constrained NMSSM with tau leptons at the LHC
High Energy Physics - Phenomenology · Submitted 3 Nov 2010
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim This dedicated analysis allows to improve on the results of generic supersymmetry searches for a large part of the parameter space of the cNMSSM.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
The constrained Next-to-Minimal Supersymmetric Standard Model (cNMSSM) with mSugra-like boundary conditions at the GUT scale implies a singlino-like LSP with a mass just a few GeV below a stau NLSP. Hence, most of the squark/gluino decay cascades contain two tau leptons. The gluino mass >~ 1.2 TeV is somewhat larger than the squark masses of >~ 1 TeV. We simulate signal and background events for such a scenario at the LHC, and propose cuts on the transverse momenta of two jets, the missing transverse energy and the transverse momentum of a hadronically decaying tau lepton. This dedicated analysis allows to improve on the results of generic supersymmetry searches for a large part of the parameter space of the cNMSSM. The distribution of the effective mass and the signal rate provide sensitivity to distinguish the cNMSSM from the constrained Minimal Supersymmetric Standard Model in the stau-coannihilation region.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The constrained Next-to-Minimal Supersymmetric Standard Model (cNMSSM) with mSugra-like boundary conditions at the GUT scale implies a singlino-like LSP with a mass just a few GeV below a stau NLSP. | background 0.95 | 0.14 | 0.09 | asserted 0.99 |
| s1 | Hence, most of the squark/gluino decay cascades contain two tau leptons. | background 0.43 | 0.26 | 0.07 | asserted 0.82 |
| s2 | The gluino mass >~ 1.2 TeV is somewhat larger than the squark masses of >~ 1 TeV. | result 0.54 | 0.29 | 0.04 | asserted 0.91 |
| s3 | We simulate signal and background events for such a scenario at the LHC, and propose cuts on the transverse momenta of two jets, the missing transverse energy and the transverse momentum of a hadronically decaying tau lepton. | method 0.89 | 0.93 | 0.08 | asserted 0.99 |
| s4 | This dedicated analysis allows to improve on the results of generic supersymmetry searches for a large part of the parameter space of the cNMSSM. | interpretation 0.41 | 0.78 | 0.49 | asserted 0.95 |
| s5 | The distribution of the effective mass and the signal rate provide sensitivity to distinguish the cNMSSM from the constrained Minimal Supersymmetric Standard Model in the stau-coannihilation region. | result 0.51 | 0.79 | 0.45 | asserted 0.89 |
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The paper
Original abstract
The constrained Next-to-Minimal Supersymmetric Standard Model (cNMSSM) with mSugra-like boundary conditions at the GUT scale implies a singlino-like LSP with a mass just a few GeV below a stau NLSP. Hence, most of the squark/gluino decay cascades contain two tau leptons. The gluino mass >~ 1.2 TeV is somewhat larger than the squark masses of >~ 1 TeV. We simulate signal and background events for such a scenario at the LHC, and propose cuts on the transverse momenta of two jets, the missing transverse energy and the transverse momentum of a hadronically decaying tau lepton. This dedicated analysis allows to improve on the results of generic supersymmetry searches for a large part of the parameter space of the cNMSSM. The distribution of the effective mass and the signal rate provide sensitivity to distinguish the cNMSSM from the constrained Minimal Supersymmetric Standard Model in the stau-coannihilation region.
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References
How the literature uses it
10 arXiv papers cite this in 15 sentences
Papers citing it · 8 sentences without a confident label
Cites it as support 1 paper
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In the 5-parameter and 4-parameter cNMSSM, the SM-like Higgs cannot get to 125 GeV under all the constraints including muon g-2 [ref] .
The semi-constrained NMSSM in light of muon g-2, LHC, and dark matter constraints · Introduction · 0.96
Cites it as background 6 papers
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Since simple models are usually more favoured, the fully constrained NMSSM (cNMSSM) [ref] and the semi-constrained NMSSM (scNMSSM) are also being studied [ref] .
The semi-constrained NMSSM in light of muon g-2, LHC, and dark matter constraints · Introduction · 0.94
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While in constrained models, congeneric parameters are assumed universal at the Grand Unified Theoretical (GUT) scale, leaving only four free parameters in the fully-constrained MSSM (CMSSM) and four or five in the fully-constrained NMSSM (CNMSSM) [ref] .
Higgs decay to light scalars in the semi-constrained NMSSM · Introduction · 0.94
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In the graceful and simple model of fully-constrained NMSSM (cNMSSM), all Higgs and sfermion masses are assumed to be unified at the Grand Unified theoretical (GUT) scale, thus only four parameters at GUT scale are left free [ref] .
A Novel Scenario in the Semi-constrained NMSSM · Introduction · 0.94
What it cites · 37 sentences without a confident label
Uses the method or tool of 10 papers
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Both the signal and the top quark background were generated by PYTHIA 6.4 [ref] , which was in charge of generation and phase-space decays.
PYTHIA 6.4 Physics and Manual · Simulation, signal and background rates · 1.00
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For the detector simulation we employed AcerDet [ref] .
AcerDET: a particle level fast simulation and recosntruction package for phenomenological studies on high pT physics at LHC · Simulation, signal and background rates · 1.00
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Their total production cross sections are obtained at NLO (QCD) from PROSPINO [ref] , and are also shown in Table [ref].
PROSPINO: A Program for the Production of Supersymmetric Particles in Next-to-leading Order QCD · The signal, backgrounds and cuts · 0.99
Uses data or values from 1 paper
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For their transverse momenta we require at least 30 GeV, which allows to assume an efficiency of $∼40%$ [ref] (and a $τ$-fake rate of jets of $∼1-2%$).
Expected Performance of the ATLAS Experiment - Detector, Trigger and Physics · The signal, backgrounds and cuts · 0.94
Compares with 1 paper
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Adding the tau identification to the analysis in the 4jtau analysis, a total background cross section of 61 fb after cuts obtained here is to be compared with 51 fb at NLO in [ref] .
Expected Performance of the ATLAS Experiment - Detector, Trigger and Physics · Simulation, signal and background rates · 1.00
Cites as background 19 papers
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It is well known that, within the cMSSM [ref] , a small value of $m_0$ would imply a stau ($τ_1$) LSP, which is not a reasonable candidate for the dark matter.
The Soft Supersymmetry-Breaking Lagrangian: Theory and Applications · Introduction · 0.81
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The NMSSM with a scale invariant superpotential $W$ [ref] differs from the MSSM through the replacement of the $μ$ term in $W_MSSM$ by the coupling to a gauge singlet superfield $S$ and a trilinear $S$ self-coupling:
The Next-to-Minimal Supersymmetric extension of the Standard Model reviewed · The spectrum of the cNMSSM · 0.99
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The NMSSM with a scale invariant superpotential $W$ [ref] differs from the MSSM through the replacement of the $μ$ term in $W_MSSM$ by the coupling to a gauge singlet superfield $S$ and a trilinear $S$ self-coupling:
The Next-to-Minimal Supersymmetric Standard Model · The spectrum of the cNMSSM · 0.99
Discussion
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