Search results for "Pair Production"

showing 10 items of 431 documents

"Table 3" of "Measurement of W^+W^- production in pp collisions at sqrt{s}=7 TeV with the ATLAS detector and limits on anomalous WWZ and WWgamma coup…

2014

The measured total cross section (combined). The first systematic (sys) error is the combined systematic uncertainty excluding that of the luminosity. The second (sys) error is the uncertainty on the luminosity.

Astrophysics::High Energy Astrophysical PhenomenaIntegrated Cross SectionW pair Production7000.0Astrophysics::Cosmology and Extragalactic AstrophysicsCross SectionSIGInclusiveProton-Proton ScatteringP P --> W+ W- XHigh Energy Physics::ExperimentNuclear ExperimentW ProductionAstrophysics::Galaxy Astrophysics
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Search for Baryonic Decays of \psi(3770) and \psi(4040)

2013

By analyzing data samples of 2.9 fb^{-1} collected at \sqrt s=3.773 GeV, 482 pb^{-1} collected at \sqrt s=4.009 GeV and 67 pb^{-1} collected at \sqrt s=3.542, 3.554, 3.561, 3.600 and 3.650 GeV with the BESIII detector at the BEPCII storage ring, we search for \psi(3770) and \psi(4040) decay to baryonic final states, including \Lambda\bar\Lambda\pi^+\pi^-, \Lambda \bar\Lambda\pi^0, \Lambda\bar\Lambda\eta, \Sigma^+ \bar\Sigma^-, \Sigma^0 \bar\Sigma^0, \Xi^-\bar\Xi^+ and \Xi^0\bar\Xi^0 decays. None are observed, and upper limits are set at the 90% confidence level.

BEShadronic decay [psi(4040)]pair production [hyperon]hadronic decay [psi(3770)]High Energy Physics::PhenomenologyBeijing Storannihilation [electron positron]High Energy Physics - Experiment3.542-4.009 GeV-cmsddc:530High Energy Physics::Experimentbranching ratioNuclear Experimentpsi mesonsexperimental results
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Search for a fermiophobic Higgs at LEP 2

2001

Higgs bosons predicted by the fermiophobic scenario within Two Higgs Doublets Models were searched for in the data collected by the DELPHI detector at centre-of-mass energies between 189 GeV and 202 GeV, corresponding to a total integrated luminosity of 380 pb^{-1}. No signal was found and confidence limits were derived in the framework of possible extensions of the Standard Model Higgs sector.

BOSONSNuclear and High Energy PhysicsParticle physicsENERGIESQUARK PAIR PRODUCTION; CARLO PROGRAM KORALZ; MONTE-CARLO; BHABHA SCATTERING; SUPERSYMMETRY; PHOTONS; PHYSICS; BOSONS; ANNIHILATION; ENERGIESFOS: Physical sciencesPHOTONS01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentHiggs sectorStandard ModelPHYSICSHigh Energy Physics - Experiment (hep-ex)BHABHA SCATTERINGCARLO PROGRAM KORALZMONTE-CARLO0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsANNIHILATIONSUPERSYMMETRYBosonDELPHIPhysicsLuminosity (scattering theory)010308 nuclear & particles physicsDetectorHigh Energy Physics::PhenomenologyQUARK PAIR PRODUCTIONLARGE ELECTRON POSITRON COLLIDERPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIHiggs bosonPARTICLE PHYSICSFísica nuclearHigh Energy Physics::ExperimentParticle Physics - Experiment
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Top-quark pair + 1-jet production at next-to-leading order QCD

2008

Top-quark pair production with an additional jet is an important signal and background process at the LHC. We present the next-to-leading order QCD calculation for this process and show results for integrated as well as differential cross sections.

Background processQuantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsTop quarkLarge Hadron ColliderHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyOrder (ring theory)FOS: Physical sciencesJet (particle physics)Atomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyPair productionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentDifferential (infinitesimal)
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"Table 12" of "Search for pair production of higgsinos in final states with at least three $b$-tagged jets in $\sqrt{s} = 13$ TeV $pp$ collisions usi…

2018

Particle-level acceptance for the high-mass discovery signal regions SR-4b-meff1-A-disc and SR-3b-meff3-A, shown as a function of higgsino mass. The acceptance is defined as the fraction of signal events passing the particle-level event selection that emulates the detector-level selection. The acceptance calculation considers only those signal events where both higgsinos decay to Higgs bosons that subsequently both decay to b-quarks.

Beauty13000.0Proton-Proton ScatteringHiggs pair ProductionP P --> HIGGSINO HIGGSINO X --> HIGGS HIGGS NEUTRALINO NEUTRALINO X --> BQ BQBAR BQ BQBAR XHigh Energy Physics::PhenomenologySUSYHigh Energy Physics::ExperimentHiggsinoSupersymmetrySIGHiggs
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"Table 10" of "Search for pair production of higgsinos in final states with at least three $b$-tagged jets in $\sqrt{s} = 13$ TeV $pp$ collisions usi…

2018

Particle-level acceptance for the low-mass discovery signal regions low-SR-MET0-meff440 and low-SR-MET150-meff440, shown as a function of higgsino mass. The acceptance is defined as the fraction of signal events passing the particle-level event selection that emulates the detector-level selection. The acceptance calculation considers only those signal events where both higgsinos decay to Higgs bosons that subsequently both decay to b-quarks.

Beauty13000.0Proton-Proton ScatteringHiggs pair ProductionP P --> HIGGSINO HIGGSINO X --> HIGGS HIGGS NEUTRALINO NEUTRALINO X --> BQ BQBAR BQ BQBAR XHigh Energy Physics::PhenomenologySUSYHigh Energy Physics::ExperimentHiggsinoSupersymmetrySIGHiggs
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"Table 16" of "Search for pair production of higgsinos in final states with at least three $b$-tagged jets in $\sqrt{s} = 13$ TeV $pp$ collisions usi…

2018

Cutflow for low-mass analysis for each signal mass point.

Beauty13000.0Proton-Proton ScatteringHiggs pair ProductionP P --> HIGGSINO HIGGSINO X --> HIGGS HIGGS NEUTRALINO NEUTRALINO X --> BQ BQBAR BQ BQBAR XSUSYHiggsinoSupersymmetrySIGHiggs
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"Table 6" of "Search for pair production of higgsinos in final states with at least three $b$-tagged jets in $\sqrt{s} = 13$ TeV $pp$ collisions usin…

2018

The observed and expected 95% upper limits on the total pair production cross section for degenerate higgsinos as a function of m(higgsino) for the high-mass search. Only the high-mass analysis results are used in this figure.

Beauty13000.0Proton-Proton ScatteringHiggs pair ProductionP P --> HIGGSINO HIGGSINO X --> HIGGS HIGGS NEUTRALINO NEUTRALINO X --> BQ BQBAR BQ BQBAR XSUSYHiggsinoSupersymmetrySIGHiggs
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"Table 3" of "Search for pair production of higgsinos in final states with at least three $b$-tagged jets in $\sqrt{s} = 13$ TeV $pp$ collisions usin…

2018

Exclusion limits on higgsino pair production. The results of the low-mass analysis are used below m(higgsino) = 300 GeV, while those of the high-mass analysis are used above. The figure shows the observed and expected 95% upper limits on the higgsino pair production cross-section as a function of m(higgsino).

Beauty13000.0Proton-Proton ScatteringHiggs pair ProductionP P --> HIGGSINO HIGGSINO X --> HIGGS HIGGS NEUTRALINO NEUTRALINO X --> BQ BQBAR BQ BQBAR XSUSYHiggsinoSupersymmetrySIGHiggs
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"Table 15" of "Search for pair production of higgsinos in final states with at least three $b$-tagged jets in $\sqrt{s} = 13$ TeV $pp$ collisions usi…

2018

Example cutflow for SR-4b-meff1-A-disc.

Beauty13000.0Proton-Proton ScatteringHiggs pair ProductionP P --> HIGGSINO HIGGSINO X --> HIGGS HIGGS NEUTRALINO NEUTRALINO X --> BQ BQBAR BQ BQBAR XSUSYHiggsinoSupersymmetrySIGHiggs
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