Search results for " Collider"

showing 10 items of 1415 documents

Top-quark pair production cross-section measurements with the ATLAS detector

2019

Measurements of the inclusive and differential top-quark pair production cross sections in proton-proton collisions with the ATLAS detector at the Large Hadron Collider at center-of-mass energies of 8 TeV and 13 TeV are presented. The inclusive measurements reach high precision and are compared to the best available theoretical calculations. Differential measurements of the kinematic properties of the top-quark production are also discussed. These measurements, including results using boosted tops, probe our understanding of top-quark pair production in the TeV regime.

PhysicsTop quarkParticle physicsLarge Hadron ColliderNuclear TheoryHigh Energy Physics::PhenomenologyKinematicsTOPSCross section (physics)Pair productionPhysics::Atomic and Molecular ClustersPhysics::Accelerator PhysicsProduction (computer science)High Energy Physics::ExperimentDifferential (mathematics)Particle Physics - Experiment
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Constraints on four-fermion interactions from the tt¯ charge asymmetry at hadron colliders

2016

The charge asymmetry in top quark production at hadron colliders is sensitive to beyond-the-Standard-Model four-fermion interactions. In this study we compare the sensitivity of $$t\bar{t}$$ cross-section and charge asymmetry measurements to effective operators describing four-fermion interactions and study the limits on the validity of this approach. A fit to a combination of Tevatron and LHC measurements yields stringent limits on the linear combinations $$C_1$$ and $$C_2$$ of the four-fermion effective operators.

PhysicsTop quarkParticle physicsLarge Hadron ColliderPhysics and Astronomy (miscellaneous)010308 nuclear & particles physicsmedia_common.quotation_subjectPhysics beyond the Standard ModelHigh Energy Physics::LatticeHadronHigh Energy Physics::PhenomenologyTevatronCharge (physics)01 natural sciencesAsymmetryFour-fermion interactionsNuclear physics0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsEngineering (miscellaneous)media_commonEuropean Physical Journal C
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Measurement of top quark pair differential cross sections in the dilepton channel in pp collisions at s=7 and 8 TeV with ATLAS

2016

Measurements of normalized differential cross-sections of top quark pair ($t\bar t$) production are presented as a function of the mass, the transverse momentum and the rapidity of the $t\bar t$ system in proton-proton collisions at center-of-mass energies of $\sqrt{s}$ = 7 TeV and 8 TeV. The dataset corresponds to an integrated luminosity of 4.6 fb$^{-1}$ at 7 TeV and 20.2 fb$^{-1}$ at 8 TeV, recorded with the ATLAS detector at the Large Hadron Collider. Events with top quark pair signatures are selected in the dilepton final state, requiring exactly two charged leptons and at least two jets with at least one of the jets identified as likely to contain a $b$-hadron. The measured distributi…

PhysicsTop quarkParticle physicsLuminosity (scattering theory)Large Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyMonte Carlo methodParton7. Clean energy01 natural sciencesNuclear physicsmedicine.anatomical_structureAtlas (anatomy)0103 physical sciencesmedicineHigh Energy Physics::ExperimentRapidityNuclear Experiment010306 general physicsLeptonPhysical Review D
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Measurement of the tt¯Z and tt¯W cross sections in proton-proton collisions at s=13  TeV with the ATLAS detector

2019

A measurement of the associated production of a top-quark pair (tt) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1 fb-1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The ttZ and ttW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are σttZ=0.95±0.08stat±0.10syst…

PhysicsTop quarkParticle physicsMuonLarge Hadron Collider010308 nuclear & particles physicsElectron01 natural sciencesVertex (geometry)Vector boson0103 physical sciencesEffective field theoryHigh Energy Physics::Experiment010306 general physicsLeptonPhysical Review D
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The RICH counter in the CERN hyperon beam experiment

1992

Abstract The hyperon beam experiment WA89 at the CERN-SPS uses a ring imaging Cherenkov counter (RICH) for identification of secondaries from ∑ − N reactions. Cherenkov photons are generated in a 5 m long radiator volume filled with nitrogen at atmospheric pressure and detected in drift chambers. The drift chambers cover an active surface of 1.6 × 0.75 m 2 , with a maximum drift path of 41 cm. Photoelectrons are counted on 1280 wires with a pitch of 2.54 mm, equipped with multihit TDCs. The counting gas is ethane saturated with TMAE at 30°C. The counter was operated in two beam periods in 1990 and 1991. The spatial resolution of the chambers is better than 2 mm and under normal running cond…

PhysicsWire chamberNuclear and High Energy PhysicsPhotonLarge Hadron ColliderAtmospheric pressurePhysics::Instrumentation and DetectorsHyperonPhotoelectric effectCharged particleParticle detectorNuclear physicsVolume (thermodynamics)Measuring instrumentHigh Energy Physics::ExperimentDetectors and Experimental TechniquesAtomic physicsInstrumentationCherenkov radiationBeam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Approximate NNLO predictions for the stop-pair production cross section at the LHC

2013

If the minimal supersymmetric standard model at scales of around 1 TeV is realized in nature, the total top-squark pair production cross section should be measurable at the CERN Large Hadron Collider. In this work we present precise predictions for this observable, which are based upon approximate NNLO formulas obtained using soft-collinear effective theory methods.

PhysicsWork (thermodynamics)Particle physicsNuclear and High Energy PhysicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesObservableQCD Phenomenology01 natural sciences3. Good healthHigh Energy Physics - PhenomenologyCross section (physics)High Energy Physics - Phenomenology (hep-ph)Pair productionSupersymmetry PhenomenologyQCD Phenomenology; Supersymmetry Phenomenology0103 physical sciencesEffective field theoryHigh Energy Physics::Experiment010306 general physicsMinimal Supersymmetric Standard Model
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ISOLTRAP Mass Measurements for Weak-Interaction Studies

2005

International audience; The conserved-vector-current (CVC) hypothesis of the weak interaction and the unitarity of the Cabibbo-Kobayashi-Maskawa (CKM) matrix are two fundamental postulates of the Standard Model. While existing data on CVC supports vector current conservation, the unitarity test of the CKM matrix currently fails by more than two standard deviations. High-precision mass measurements performed with the ISOLTRAP experiment at ISOLDE/CERN provide crucial input for these fundamental studies by greatly improving our knowledge of the decay energy of super-allowed beta decays. Recent results of mass measurements on the beta emitters 18Ne, 22Mg, 34Ar, and 74Rb as pertaining to weak-i…

Physicselementary particle weak interactionsParticle physicsLarge Hadron ColliderUnitarity010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::Phenomenology12.15.Hh 23.40.Bw 11.40.HaWeak interaction[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesISOLTRAPStandard ModelNuclear physicsMatrix (mathematics)Decay energy0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsbeta-decay
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Direct search for light gluinos

1999

We present the results for a direct search for light gluinos through the appearance of $\eta\rightarrow 3\pi^{0}$ with high transverse momentum in the vacuum tank of the NA48 experiment at CERN. We find one event within a lifetime range of $10^{-9}-10^{-3}$s and another one between $10^{-10}-10^{-9}$s. Both events are consistent with the expected background from neutrons in the beam, produced by 450 GeV protons impinging on the Be targets, which interact with the residual air in the tank. From these data we give limits on the production of the hypothetical $g\widetilde{g}$ bound state, the $R^0$ hadron, and its $R^0\rightarrow\eta\widetilde{\gamma}$ decay in the $R^0$ mass range between 1 a…

PhysicsgluinoNuclear and High Energy PhysicsParticle physicsGluinoRange (particle radiation)Large Hadron ColliderHadronNA48 experimentSupersymmetrysupersymmetry gluinoNuclear physicsBound stateHigh Energy Physics::ExperimentNeutronsupersymmetryNuclear ExperimentParticle Physics - Experiment
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Measurement of the quadratic slope parameter in the K-L -> 3 pi(0) decay Dalitz plot

2001

A value of (-6.1 +- 0.9_{stat} +- 0.5_{syst})*10^{-3} is obtained for the quadratic slope parameter h in the K_L -> 3\pi^0 decay Dalitz plot at the NA48 experiment at the CERN SPS. The result is based on 14.7*10^6 fully reconstructed K_L -> 3\pi^0 -> 6\gamma decays. This is the most precise measurement of any of the Dalitz plot slope parameters in the charged and neutral kaon decays so far.

Physicsneutral kaonParticle physicsNuclear and High Energy PhysicsLarge Hadron Collidermesoni K; decadimenti; Dalitz plotdecadimentiDalitz plotkaon decay; neutral kaon; dalitz plotslope parametersNA48 experimentDalitz plotValue (computer science)KaonsKaons; Dalitz plot; slope parameterskaon decayHigh Energy Physics - Experimentmesoni KClassical mechanicsQuadratic equationK->3-PI
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Thermalization in the initial stage of heavy ion collisions

2017

The high density non-abelian matter produced in heavy ion collisions is extremely anisotropic. Prethermal dynamics for the anisotropic and weakly coupled matter is discussed. Thermalization is realized with the effective kinetic theory in the leading order accuracy of the weakly coupled expansion. With the initial condition from color glass condensate, hydrodynamization time for the LHC energies is realized to be about 1 fm/c, while the thermalization happens much later than the hydrodynamization. peerReviewed

PhysicsthermalizationLarge Hadron Colliderta114010308 nuclear & particles physicsPhysicsQC1-999heavy ion collisionsHigh density01 natural sciences7. Clean energyColor-glass condensateNuclear physicsThermalisationChemical physics0103 physical sciencesKinetic theory of gasescolor glass condensatehydrodynamizationInitial value problemHeavy ion010306 general physicsAnisotropyQuark Confinement and the Hadron Spectrum
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