Search results for "Collider"

showing 10 items of 1690 documents

Search for single top quarks in the tau + jets channel using 4.8 fb−1 of pp¯ collision data

2010

We present the first direct search for single top quark production using tau leptons. The search is based on 4.8 fb$^{-1}$ of integrated luminosity collected in $p\bar{p}$ collisions at $\sqrt{s}$=1.96 TeV with the D0 detector at the Fermilab Tevatron Collider. We select events with a final state including an isolated tau lepton, missing transverse energy, two or three jets, one or two of them $b$ tagged. We use a multivariate technique to discriminate signal from background. The number of events observed in data in this final state is consistent with the signal plus background expectation. We set in the tau+jets channel an upper limit on the single top quark cross section of \TauLimObs pb …

QuarkPhysicsNuclear and High Energy PhysicsTop quarkParticle physicsMuon010308 nuclear & particles physicsTevatron01 natural scienceslaw.inventionNuclear physicslaw0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)Fermilab010306 general physicsColliderLeptonPhysics Letters B
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Observation of top-quark pair production in association with a photon and measurement of thett¯γproduction cross section inppcollisions ats=7TeV usin…

2015

A search is performed for top-quark pairs (t (t) over bar) produced together with a photon (gamma) with transverse energy greater than 20 GeV using a sample of t (t) over bar candidate events in final states with jets, missing transverse momentum, and one isolated electron or muon. The data set used corresponds to an integrated luminosity of 4.59 fb(-1) of proton-proton collisions at a center-of-mass energy of 7 TeV recorded by the ATLAS detector at the CERN Large Hadron Collider. In total, 140 and 222 t (t) over bar gamma candidate events are observed in the electron and muon channels, to be compared to the expectation of 79 +/- 26 and 120 +/- 39 non-t (t) over bar gamma background events,…

QuarkPhysicsNuclear and High Energy PhysicsTop quarkParticle physicsMuonLarge Hadron ColliderBranching fractionHigh Energy Physics::PhenomenologyParton7. Clean energyNuclear physicsPair productionHigh Energy Physics::ExperimentLeptonPhysical Review D
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Search for the neutral current top quark decayt→Zcusing the ratio ofZ-boson+4  jetstoW-boson+4  jetsproduction

2009

We have used the Collider Detector at Fermilab (CDF II) to search for the flavor-changing neutral-current (FCNC) top quark decay t {yields} Zc using a technique employing ratios of W and Z production, measured in p{bar p} data corresponding to an integrated luminosity of 1.52 fb{sup -1}. The analysis uses a comparison of two decay chains, p{bar p} {yields} t{bar t} {yields} WbWb {yields} {ell}{nu}bjjb and p{bar p} {yields} t{bar t} {yields} ZcWb {yields} {ell}{ell}cjjb, to cancel systematic uncertainties in acceptance, efficiency, and luminosity. We validate the modeling of acceptance and efficiency for lepton identification over the multi-year dataset using another ratio of W and Z product…

QuarkPhysicsNuclear and High Energy PhysicsTop quarkParticle physicsNeutral current010308 nuclear & particles physicsBranching fractionHigh Energy Physics::Phenomenology7. Clean energy01 natural sciencesStandard ModelNuclear physicsParticle decay0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)010306 general physicsCollider Detector at FermilabPhysical Review D
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Three-Loop Quark Jet Function.

2018

We calculate the massless quark jet function to three-loop order. The quark jet function is a universal ingredient in SCET factorization for many collider and decay processes with quark initiated final state jets. Our three-loop result contributes to the resummation for observables probing the invariant mass of final state quark jets at primed next-to-next-to-next-to-leading-logarithmic accuracy. It represents the first complete three-loop result for a factorization ingredient describing collinear radiation. Furthermore it constitutes a major component of the N-jettiness subtraction method at next-to-next-to-next-to-leading order accuracy, which eventually may enable the calculation of full…

QuarkPhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyObservableJet (particle physics)01 natural scienceslaw.inventionMassless particleFactorizationlaw0103 physical sciencesInvariant massHigh Energy Physics::ExperimentResummation010306 general physicsColliderPhysical review letters
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Search for the Production of Scalar Bottom Quarks inpp¯Collisions ats=1.96  TeV

2010

We report on a search for direct scalar bottom quark (sbottom) pair production in pp collisions at {radical}(s)=1.96 TeV, in events with large missing transverse energy and two jets of hadrons in the final state, where at least one of the jets is required to be identified as originating from a b quark. The study uses a collider detector at Fermilab Run II data sample corresponding to 2.65 fb{sup -1} of integrated luminosity. The data are in agreement with the standard model. In an R-parity conserving minimal supersymmetric scenario, and assuming that the sbottom decays exclusively into a bottom quark and a neutralino, 95% confidence-level upper limits on the sbottom pair production cross se…

QuarkPhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHadronGeneral Physics and AstronomySupersymmetry7. Clean energy01 natural sciencesBottom quarkNuclear physicsPair production0103 physical sciencesNeutralinoGrand Unified TheoryHigh Energy Physics::Experiment010306 general physicsCollider Detector at FermilabPhysical Review Letters
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Search for Charged Higgs Bosons Decaying into Top and Bottom Quarks in pp Collisions

2009

Made available in DSpace on 2022-04-28T20:54:02Z (GMT). No. of bitstreams: 0 Previous issue date: 2009-05-14 We describe a search for production of a charged Higgs boson, qq̄′→H+, reconstructed in the tb̄ final state in the mass range 180≤MH+≤300GeV. The search was undertaken at the Fermilab Tevatron collider with a center-of-mass energy s=1.96TeV and uses 0.9fb-1 of data collected with the D0 detector. We find no evidence for charged Higgs boson production and set upper limits on the production cross section in the types I, II, and III two-Higgs-doublet models (2HDMs). An excluded region in the (MH+, tanβ) plane for type I 2HDM is presented. © 2009 The American Physical Society. Universida…

QuarkPhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronGeneral Physics and AstronomyType (model theory)01 natural scienceslaw.inventionlaw0103 physical sciencesHiggs bosonProduction (computer science)High Energy Physics::ExperimentFermilab010306 general physicsColliderBoson
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Resummed jet rates for heavy quark production in e+e– annihilation

2004

Expressions for Sudakov form factors for heavy quarks are presented. They are used to construct resummed jet rates in electron-positron annihilation. Predictions are given for production of bottom quarks at LEP and top quarks at the Linear Collider.

QuarkPhysicsParticle physicsAnnihilationPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeElectron–positron annihilationNuclear TheoryHigh Energy Physics::PhenomenologyFísicaJet (particle physics)law.inventionlawPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentColliderEngineering (miscellaneous)The European Physical Journal C
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EPPS16 – First nuclear PDFs to include LHC data

2017

We present results of our recent EPPS16 global analysis of NLO nuclear parton distribution functions (nPDFs). For the first time, dijet and heavy gauge boson production data from LHC proton–lead collisions have been included in a global fit. Especially, the CMS dijets play an important role in constraining the nuclear effects in gluon distributions. With the inclusion of also neutrino–nucleus deeply-inelastic scattering and pion–nucleus Drell–Yan data and a proper treatment of isospin-corrected data, we were able to free the flavor dependence of the valence and sea quark nuclear modifications for the first time. This gives us less biased, yet larger, flavor by flavor uncertainty estimates. …

QuarkPhysicsParticle physicsGauge bosonLarge Hadron ColliderHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyDrell–Yan processPartonGluonFactorizationHigh Energy Physics::ExperimentNuclear ExperimentBosonProceedings of The European Physical Society Conference on High Energy Physics — PoS(EPS-HEP2017)
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Search for Gluino-Mediated Bottom Squark Production inpp¯Collisions ats=1.96  TeV

2009

We report on a search for the supersymmetric partner of the bottom quark produced from gluino decays in data from 2.5 fb{sup -1} of integrated luminosity collected by the Collider Detector at Fermilab at {radical}s = 1.96 TeV. Candidate events are selected requiring two or more jets and large missing transverse energy. At least two of the jets are required to be tagged as originating from a b quark to enhance the sensitivity. The results are in good agreement with the prediction of the standard model processes, giving no evidence for gluino decay to sbottom quarks. This result constrains the gluino-pair-production cross section to be less than 40 fb at 95% credibility level for a gluino mas…

QuarkPhysicsParticle physicsGluino010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyGeneral Physics and AstronomySuperpartnerSupersymmetry01 natural sciences7. Clean energyBottom quarkStandard ModelNuclear physicsParticle decay0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsCollider Detector at FermilabPhysical Review Letters
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Search for New Phenomena intt¯Events with Large Missing Transverse Momentum in Proton-Proton Collisions ats=7  TeVwith the ATLAS Detector

2012

A search for new phenomena in tt events with large missing transverse momentum in proton-proton collisions at a center-of-mass energy of 7 TeV is presented. The measurement is based on 1.04  fb-1 of data collected with the ATLAS detector at the LHC. Contributions to this final state may arise from a number of standard model extensions. The results are interpreted in terms of a model where new top-quark partners are pair produced and each decay to an on-shell top (or antitop) quark and a long-lived undetected neutral particle. The data are found to be consistent with standard model expectations. A limit at 95% confidence level is set excluding a cross section times branching ratio of 1.1 pb …

QuarkPhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsAtlas detectorBranching fractionGeneral Physics and AstronomySupersymmetry01 natural sciencesNuclear physics0103 physical sciencesTransverse momentumFourth generationHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsNeutral particlePhysical Review Letters
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