Search results for "High Energy Physics::Phenomenology"

showing 10 items of 5791 documents

"Fig1" of "Medium modification of jet fragmentation in Au+Au collisions at sqrt(s_NN)=200 GeV measured in direct photon-hadron correlations"

2020

Direct photon-hadron pair per-trigger yields vs Delta-phi (Au+Au and p+p)

62.4-200.0DEUT AU --> CHARGED XHigh Energy Physics::PhenomenologyAU AU --> CHARGED XCU CU --> CHARGED XHigh Energy Physics::ExperimentNuclear Experiment
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Search for the neutral Higgs bosons of the Minimal Supersymmetric Standard Model in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

2013

A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7 TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb[superscript −1] to 4.8 fb[superscript −1]. Higgs boson decays into oppositely-charged muon or τ lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits ar…

7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Naturvetenskap[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]SUPERSYMMETRYQCBosonPhysicsLarge Hadron ColliderSettore FIS/01 - Fisica SperimentaleSupersymmetryATLASmedicine.anatomical_structureComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHiggs bosonLHCNatural SciencesParticle Physics - ExperimentParticle physicsNuclear and High Energy PhysicsCiências Naturais::Ciências Físicas530 PhysicsHiggs boson:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Nuclear physicsAtlas (anatomy)0103 physical sciencesmedicineddc:530High Energy Physics010306 general physicsCiencias ExactasHadron-Hadron scattering; Nuclear and High Energy PhysicsMuonScience & TechnologyHadron-Hadron ScatteringATLAS detector010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaHadron-Hadron scatteringHADRON-HADRON COLLISIONSExperimental High Energy PhysicsHigh Energy Physics::ExperimentMinimal Supersymmetric Standard ModelLepton
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"Table 31" of "Search for photonic signatures of gauge-mediated supersymmetry in 8 TeV $pp$ collisions with the ATLAS detector"

2015

The total NLO cross sections with uncertainties for the electroweak production GGM signal grid for the photon+j analysis.

8000.0Physics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyIntegrated Cross SectionSUSYCross SectionSIGStatistics::ComputationP P --> CHARGINO1 CHARGINO1 XP P --> NEUTRALINO2 NEUTRALINO2 XInclusiveP P --> CHARGINO1 NEUTRALINO2 XProton-Proton ScatteringHigh Energy Physics::ExperimentSupersymmetry
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"Table 34" of "Search for massive, long-lived particles using multitrack displaced vertices or displaced lepton pairs in pp collisions at $\sqrt{s}$ …

2015

Choice of signal region in the $m(\tilde{g})$-$c\tau$ plane for the split-SUSY models with gluino decays and neutralino masses in GeV as indicated. A value of 1 indicates that the DV+$E_T^{miss}$ channel provided the best expected constraint for that point, while a value of -1 indicates the DV+jets channel. A dash indicates where results were not calculated for a particular mass/lifetime combination.

8000.0Proton-Proton ScatteringHigh Energy Physics::PhenomenologyP P --> GLUINO GLUINOExclusiveHigh Energy Physics::Experiment
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"Table 42" of "Search for massive, long-lived particles using multitrack displaced vertices or displaced lepton pairs in pp collisions at $\sqrt{s}$ …

2015

Vertex mass distributions in data and one RPV SUSY signal model, for vertices with 0, 1 and $\geq$2 charged leptons in the dilepton $e^{\pm}\mu^{\mp}$ channel. The entries are the number of DVs in each bin, not normalized according to bin size. The signal model is for gluino pair production, with $\tilde{g}\to qq[\tilde{\chi}_1^0\to e\mu\nu/ee\nu]$ decays, $m(\tilde{g})$ = 1300 GeV, $m(\tilde{\chi}_1^0)$ = 50 GeV and $c\tau(\tilde{\chi}_1^0)$ = 30 mm.

8000.0Proton-Proton ScatteringHigh Energy Physics::PhenomenologyP P --> GLUINO GLUINOExclusiveHigh Energy Physics::ExperimentN
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"Table 43" of "Search for massive, long-lived particles using multitrack displaced vertices or displaced lepton pairs in pp collisions at $\sqrt{s}$ …

2015

Vertex mass distributions in data and one RPV SUSY signal model, for vertices with 0, 1 and $\geq$2 charged leptons in the dilepton $\mu^+\mu^-$ channel. The entries are the number of DVs in each bin, not normalized according to bin size. The signal model is for gluino pair production, with $\tilde{g}\to qq[\tilde{\chi}_1^0\to e\mu\nu/\mu\mu\nu]$ decays, $m(\tilde{g})$ = 1300 GeV, $m(\tilde{\chi}_1^0)$ = 50 GeV and $c\tau(\tilde{\chi}_1^0)$ = 30 mm.

8000.0Proton-Proton ScatteringHigh Energy Physics::PhenomenologyP P --> GLUINO GLUINOExclusiveHigh Energy Physics::ExperimentNComputer Science::Data Structures and Algorithms
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"Table 41" of "Search for massive, long-lived particles using multitrack displaced vertices or displaced lepton pairs in pp collisions at $\sqrt{s}$ …

2015

Vertex mass distributions in data and one RPV SUSY signal model, for vertices with 0, 1 and $\geq$2 charged leptons in the dilepton $e^+e^-$ channel. The entries are the number of DVs in each bin, not normalized according to bin size. The signal model is for gluino pair production, with $\tilde{g}\to qq[\tilde{\chi}_1^0\to e\mu\nu/ee\nu]$ decays, $m(\tilde{g})$ = 1300 GeV, $m(\tilde{\chi}_1^0)$ = 50 GeV and $c\tau(\tilde{\chi}_1^0)$ = 30 mm.

8000.0Proton-Proton ScatteringHigh Energy Physics::PhenomenologyP P --> GLUINO GLUINOExclusiveHigh Energy Physics::ExperimentNComputer Science::Data Structures and Algorithms
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"Table 3" of "Search for massive, long-lived particles using multitrack displaced vertices or displaced lepton pairs in pp collisions at $\sqrt{s}$ =…

2015

Vertex-level efficiency as a function of the vertex radial position for an RPV SUSY model of squark production with $\tilde{q}\to q[\tilde{\chi}_1^0\to\mu qb]$, where $m(\tilde{q}) = 700$ GeV, $m(\tilde{\chi}_1^0) = 494$ GeV and $c\tau(\tilde{\chi}_1^0)$ = 175 mm. The other SUSY model point in the figure is tabulated in http://hepdata.cedar.ac.uk/view/ins1362183/d1.

8000.0Proton-Proton ScatteringP P --> SQUARK SQUARKHigh Energy Physics::PhenomenologyEFFExclusiveHigh Energy Physics::ExperimentComputer Science::Data Structures and Algorithms
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"Table 3" of "Measurements of the charge asymmetry in top-quark pair production in the dilepton final state at $\sqrt{s}=8$ TeV with the ATLAS detect…

2017

The leptonic inclusive asymmetry in the fiducial volume.

8000.0Proton-Proton ScatteringP P --> top + antitopHigh Energy Physics::PhenomenologyAstrophysics::Instrumentation and Methods for AstrophysicsExclusiveTopTop ProductionHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsINCLUSIVE ASYMMETRY
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"Table 1" of "Measurement of electroweak parameters from Z decays into Fermion pairs"

1990

Hadronic cross section from the charged track selection trigger.

88.227-95.036E+ E- --> HADRONSE+ E- --> Z0E+ E- ScatteringNuclear TheoryHigh Energy Physics::PhenomenologyIntegrated Cross SectionExclusiveHigh Energy Physics::ExperimentCross SectionR measurementNuclear ExperimentSIG
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