Search results for "Proton"

showing 10 items of 5886 documents

Measurement of the electron charge asymmetry inpp¯→W+X→eν+Xdecays inpp¯collisions ats=1.96  TeV

2015

We present a measurement of the electron charge asymmetry in $p\bar{p}\rightarrow W+X \rightarrow e\nu +X$ events at a center-of-mass energy of 1.96 TeV, using data corresponding to 9.7~fb$^{-1}$ of integrated luminosity collected with the D0 detector at the Fermilab Tevatron Collider. The asymmetry is measured as a function of the electron pseudorapidity and is presented in five kinematic bins based on the electron transverse energy and the missing transverse energy in the event. The measured asymmetry is compared with next-to-leading-order predictions in perturbative quantum chromodynamics and provides accurate information for the determination of parton distribution functions of the prot…

PhysicsNuclear and High Energy PhysicsParticle physicsProtonmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatronPartonElectron7. Clean energyAsymmetryNuclear physicsDistribution functionPseudorapidityHigh Energy Physics::ExperimentNuclear Experimentmedia_commonLeptonPhysical Review D
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Spin asymmetriesA1and structure functionsg1of the proton and the deuteron from polarized high energy muon scattering

1998

We present the final results of the spin asymmetries A1 and the spin structure functions g1 of the proton and the deuteron in the kinematic range 0.0008<x<0.7 and 0.2<Q2<100 GeV2. For the determination of A1, in addition to the usual method which employs inclusive scattering events and includes a large radiative background at low x, we use a new method which minimizes the radiative background by selecting events with at least one hadron as well as a muon in the final state. We find that this hadron method gives smaller errors for x<0.02, so it is combined with the usual method to provide the optimal set of results.

PhysicsNuclear and High Energy PhysicsParticle physicsRange (particle radiation)MuonProtonScatteringHadronSpin structureNuclear physicsRadiative transferHigh Energy Physics::ExperimentNuclear ExperimentSpin-½Physical Review D
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Design and commissioning of the GSI pion beam

2002

We describe the design of the secondary pion beam-line installed at the SIS 18Tm synchrotron at GSI, Darmstadt, and discuss the commissioning results. The experiments were performed with proton and C-12 primary beams at several energies using beryllium production targets. Pion yields in a momentum range between 0.4 and 2.8 GeV/c were identified, At the highest primary beam energies of 3.5 GeV for proton and 2.0 A GeV for carbon ions, the latter beam produces the highest low-momentum pion yield while at momenta of 1.5 GeV/c the yields are comparable and at 2.8 GeV/c the proton beam is superior. A momentum resolution of around 0.5% is achieved and the time resolution (a) ranges from 100 to 15…

PhysicsNuclear and High Energy PhysicsParticle physicsRange (particle radiation)ProtonNuclear Theorychemistry.chemical_elementSynchrotronlaw.inventionNuclear physicsMomentumTime of flightPionchemistrylawPhysics::Accelerator PhysicsHigh Energy Physics::Experiment[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]BerylliumNuclear ExperimentInstrumentationBeam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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A trigger system for measurements of proton-induced rare hadronic reactions around Tp=400MeV

2008

Abstract We developed a trigger system for the measurement of proton-induced rare hadronic reactions around the beam kinetic energy T p = 400 MeV based on highly segmented trigger scintillation detectors and programmable logic modules. The trigger system was designed to enhance events with the negative-pion production by the difference of the curvatures of the particle tracks in a magnetic field. Since the production cross-section of the negative-pion by the proton-induced reactions was smaller by about 3 orders of magnitude than the total cross-section around the beam energy, we expected large reduction of the trigger rate by the negative-pion selection. The construction of the trigger sys…

PhysicsNuclear and High Energy PhysicsParticle physicsScintillationProtonOrders of magnitude (temperature)Nuclear TheoryDetectorHadronKinetic energyMagnetic fieldNuclear physicsPhysics::Accelerator PhysicsNuclear ExperimentInstrumentationBeam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Prospects for hypernuclear physics at Mainz: From KAOS@MAMI to PANDA@FAIR

2013

Abstract At the Mainz Microtron hypernuclei are produced by ( e , e ′ K ) reactions. A dedicated kaon spectrometer located at 0° with respect to the electron beam is used to detect kaons emitted in forward direction thus tagging events involving strangeness production. By measuring the momenta of pions from two body weak decays using high resolution magnetic spectrometers one gains direct access to the ground state masses of the produced hyperfragments. At FAIR the PANDA Collaboration intends to produce double-hypernuclei by numbers with an antiproton beam and study their high resolution γ -spectroscopy thus providing for the first time precise information on the level structure of these nu…

PhysicsNuclear and High Energy PhysicsParticle physicsSpectrometerNuclear TheoryStrangeness productionHypernucleusNuclear physicsPionAntiproton beamhypernuclei; weak decay; spectroscopyKAOSGround stateNuclear ExperimentMicrotron
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The Proton Spectrum in Neutron Beta Decay: Latest Results with the aSPECT Spectrometer

2009

Abstract The purpose of the neutron decay spectrometer aSPECT is to determine the antineutrino electron angular correlation coefficient a with high precision. Latest measurements with aSPECT were performed during April/May 2008 at the Institut Laue-Langevin in Grenoble, France. In this paper we give a report on the experiment and the status of the ongoing data analysis.

PhysicsNuclear and High Energy PhysicsParticle physicsSpectrometerProtonCabibbo–Kobayashi–Maskawa matrixSpectrum (functional analysis)ElectronBeta decayPhysics::GeophysicsNuclear physicsAngular correlationNeutronNuclear ExperimentNuclear Physics A
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Measurement of thepp¯→tt¯production cross section and the top quark mass ats=1.96  TeVin the all-hadronic decay mode

2007

We report the measurements of the t{bar t} production cross section and of the top quark mass using 1.02 fb{sup -1} of p{bar p} data collected with the CDF II detector at the Fermilab Tevatron. We select events with six or more jets on which a number of kinematical requirements are imposed by means of a neural network algorithm. At least one of these jets must be identified as initiated by a b-quark candidate by the reconstruction of a secondary vertex. The cross section is measured to be {sigma}{sub t{bar t}} = 8.3 {+-} 1.0(stat. ){sup +2.0}{sub -1.5}(syst.) {+-} 0.5(lumi.) pb, which is consistent with the standard model prediction. The top quark mass of 174.0 {+-} 2.2(stat.){+-}4.8(syst.)…

PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkMass distribution010308 nuclear & particles physicsHadronHigh Energy Physics::PhenomenologyTevatron01 natural sciencesParticle identificationStandard ModelNuclear physicsPair productionAntiproton0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)Invariant massFermilabNuclear Experiment010306 general physicsPhysical Review D
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Measurement of the top quark pair production cross section in thelepton+jetschannel in proton-antiproton collisions ats=1.96  TeV

2011

We present a measurement of the inclusive top quark pair production cross section in \ppbar collisions at (\sqrt{s}=1.96) TeV utilizing data corresponding to an integrated luminosity of \lumi\ collected with the D0 detector at the Fermilab Tevatron Collider. We consider final states containing one high-$p_{T}$ isolated electron or muon and at least two jets, and we perform three analyses: one exploiting specific kinematic features of \ttbar events, the second using $b$-jet identification, and the third using both techniques to separate \ttbar\ signal from background. In the third case, we determine simultaneously the $t\bar{t}$ cross section and the ratio of the production rates of $W$+heav…

PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatron01 natural sciences7. Clean energyNuclear physicsPair productionAntiproton0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)Fermilab010306 general physicsLeptonPhysical Review D
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Future experiments on hypernuclei and hyperatoms

2004

Abstract The possibility to produce double Λ nuclei in anti-proton nucleus collisions at anti-proton momenta close to the threshold for Ξ − Ξ + is explored. Combining a high-luminosity antiproton beam with a novel solid-state tracking system and a high-rate Ge-array, γ-spectroscopy of ΛΛ-hypernuclei will become feasible at the PANDA experiment of the future International Accelerator Facility at GSI.

PhysicsNuclear and High Energy PhysicsParticle physicsbusiness.industryNuclear TheoryTracking systemNuclear physicsmedicine.anatomical_structureAntiproton beamAntiprotonmedicinePhysics::Accelerator PhysicsNuclear ExperimentbusinessInstrumentationNucleusNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Measurement of the forward-backward asymmetry inΛb0andΛ¯b0baryon production inpp¯collisions ats=1.96TeV

2015

We measure the forward-backward asymmetry in the production of Lambda(0)(b) and (Lambda) over bar (0)(b) baryons as a function of rapidity in p (p) over bar collisions at root s = 1.96 TeV using 10.4 fb(-1) of data collected with the D0 detector at the Fermilab Tevatron collider. The asymmetry is determined by the preference of Lambda(0)(b) or (Lambda) over bar (0)(b) particles to be produced in the direction of the beam protons or antiprotons, respectively. The measured asymmetry integrated over rapidity y in the range 0.1 < vertical bar y vertical bar < 2.0 is A = 0.04 +/- 0.07(stat) +/- 0.02(syst).

PhysicsNuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatronLambdaAsymmetrylaw.inventionBaryonNuclear physicslawAntiprotonPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentRapidityNuclear ExperimentCollidermedia_commonBar (unit)Physical Review D
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