Search results for "Transverse plane"

showing 10 items of 285 documents

Measurement of the transverse polarization ofΛandΛ¯hyperons produced in proton-proton collisions ats=7  TeVusing the ATLAS detector

2015

The transverse polarization of Λ and Λ¯ hyperons produced in proton-proton collisions at a center-of-mass energy of 7 TeV is measured. The analysis uses 760  μb−1 of minimum bias data collected by the ATLAS detector at the LHC in the year 2010. The measured transverse polarization averaged over Feynman xF from 5×10−5 to 0.01 and transverse momentum pT from 0.8 to 15 GeV is −0.010±0.005(stat)±0.004(syst) for Λ and 0.002±0.006(stat)±0.004(syst) for Λ¯. It is also measured as a function of xF and pT, but no significant dependence on these variables is observed. Prior to this measurement, the polarization was measured at fixed-target experiments with center-of-mass energies up to about 40 GeV. …

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderExtrapolationHyperonParticle acceleratorPolarization (waves)7. Clean energylaw.inventionNuclear physicssymbols.namesakeTransverse planelawsymbolsFeynman diagramHigh Energy Physics::ExperimentNuclear ExperimentPhysical Review D
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Transverse energy from minijets in ultrarelativistic nuclear collisions: a next-to-leading order analysis

2000

We compute in next-to-leading order (NLO) perturbative QCD the amount of transverse energy produced into a rapidity region $\Delta Y$ of a nuclear collision from partons created in the few-GeV subcollisions. The NLO formulation assumes collinear factorization and is based on the subtraction method. We first study the results as a function of the minimum transverse momentum scale and define and determine the associated $K$-factors. The dependence of the NLO results on the scale choice and on the size of $\Delta Y$ is also studied. The calculations are performed for GRV94 and CTEQ5 sets of parton distributions. Also the effect of nuclear shadowing to the NLO results is investigated. The main …

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderNuclear Theory010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPerturbative QCDFOS: Physical sciencesParton01 natural sciencesNuclear physicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyTransverse planeHigh Energy Physics - Phenomenology (hep-ph)Factorization0103 physical sciencesQuark–gluon plasmaRapidityHigh Energy Physics::Experiment010306 general physicsNuclear Experiment
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Transverse momenta of partons and dimuons in QCD

1978

Abstract Intrinsic (primordial) transverse momenta of quarks and gluons are calculated as well as those arising from recoil (bremsstrahlung) effects, using only the well-known parton distributions as input. The intrinsic kT's lie typically in the range of 150–250 MeV. Recent approaches using heuristic integro-differential equations for kT distributions of partons are shown to disagree with the results obtained by rigorous QCD calculations. The transverse momenta of dimuon pairs produced in pp → μ+μ− + X at the ISR can be solely explained by dynamical recoil effects, i.e., q q →(μ + μ − ) g and gq →(μ + μ − ) q , and no significant intrinsic transverse parton momenta are required. These dimu…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsRange (particle radiation)Large Hadron ColliderNuclear TheoryBremsstrahlungPartonNuclear physicsTransverse planeRecoilQuark–gluon plasmaHigh Energy Physics::ExperimentNuclear ExperimentNuclear Physics B
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Measurement of Dijet Azimuthal Decorrelations inppCollisions ats=7  TeV

2011

Azimuthal decorrelations between the two central jets with the largest transverse momenta are sensitive to the dynamics of events with multiple jets. We present a measurement of the normalized differential cross section based on the full data set ( integral Ldt = 36 pb(-1)) acquired by the ATLAS detector during the 2010 root s = 7 TeV proton-proton run of the LHC. The measured distributions include jets with transverse momenta up to 1.3 TeV, probing perturbative QCD in a high-energy regime.

PhysicsQuantum chromodynamicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaHadronGeneral Physics and AstronomyPerturbative QCDElementary particle01 natural sciencesNuclear physicsTransverse planemedicine.anatomical_structureAtlas (anatomy)0103 physical sciencesmedicineHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsNucleonPhysical Review Letters
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Measurement of Dijet Azimuthal Decorrelations at Central Rapidities inpp¯Collisions ats=1.96  TeV

2005

Correlations in the azimuthal angle between the two largest transverse momentum jets have been measured using the D0 detector in p (p) over bar collisions at a center-of-mass energy root s=1.96 TeV. The analysis is based on an inclusive dijet event sample in the central rapidity region corresponding to an integrated luminosity of 150 pb(-1). Azimuthal correlations are stronger at larger transverse momenta. These are well described in perturbative QCD at next-to-leading order in the strong coupling constant, except at large azimuthal differences where contributions with low transverse momentum are significant.

PhysicsQuantum chromodynamicsParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsGeneral Physics and AstronomyPerturbative QCD01 natural sciencesAzimuthMomentumNuclear physicsTransverse plane0103 physical sciencesHigh Energy Physics::ExperimentRapidityNuclear Experiment010306 general physicsEvent (particle physics)Physical Review Letters
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Hadron azimuthal distributions and transverse spin asymmetries in DIS of leptons off transversely polarized targets from SMC

1999

Abstract Azimuthal distributions of hadrons (mainly π + and π − ) produced in DIS off transversely polarized targets (proton and deuteron) are studied for the first time in SMC. From these azimuthal distributions, transverse single-spin asymmetries are derived. According to Collins (‘Collins effect’), the azimuthal distribution of the leading hadron might exhibit an symmetry which originates from the transverse polarization of the final quark.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::PhenomenologyHadronPolarization (waves)Atomic and Molecular Physics and OpticsNuclear physicsAzimuthTransverse planeDeuteriumHigh Energy Physics::ExperimentNuclear ExperimentLeptonNuclear Physics B - Proceedings Supplements
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Transverse spin asymmetries in p ↑ p → π± + X and lp ↑ → l′ + π± + X

2000

Abstract While transverse spin effects have been studied in hadronic interactions since a few decades, investigations with leptonic probes have started very recently. Azimuthal distributions of hadrons (mainly π + and π − ) produced in DIS off transversely polarized targets (proton and deuteron) are studied for the first time in SMC. According to Collins (‘Collins effect’), the azimuthal distribution of the leading hadron might exhibit an asymmetry which originates from the transverse polarization of the final quark.

PhysicsQuarkNuclear and High Energy Physicsmedia_common.quotation_subjectNuclear TheoryHigh Energy Physics::PhenomenologyHadronPolarization (waves)AsymmetryNuclear physicsTransverse planeAngular distributionDeuteriumHigh Energy Physics::ExperimentNuclear Experimentmedia_commonNuclear Physics A
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Lattice study of the Boer-Mulders transverse momentum distribution in the pion

2013

The Boer-Mulders transverse momentum-dependent parton distribution (TMD) characterizes polarized quark transverse momentum in an unpolarized hadron. Techniques previously developed for lattice calculations of nucleon TMDs are applied to the pion. These techniques are based on the evaluation of matrix elements of quark bilocal operators containing a staple-shaped Wilson connection. Results for the Boer-Mulders transverse momentum shift in the pion, obtained at a pion mass of $m_{\pi} = 518\, \mbox{MeV} $, are presented and compared to corresponding results in the nucleon.

PhysicsQuarkParticle physicsHigh Energy Physics::LatticeHadronHigh Energy Physics::PhenomenologyNuclear TheoryHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesPartonHigh Energy Physics - PhenomenologyTransverse planeHigh Energy Physics - LatticePionHigh Energy Physics - Phenomenology (hep-ph)Lattice (order)Transverse momentumHigh Energy Physics::ExperimentNucleonNuclear Experiment
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Spin structures of the pion and nucleon

2012

We present recent studies on the transverse spin densities of the pion and nucleon within the framework of the chiral quark-(soliton) model, based on the calculation of the electromagnetic and tensor form factors of the pion and the nucleon. The results for the transverse spin densities of the quark inside a pion are in good agreement with the recent lattice data, while those of the nucleon show similar features to the lattice results. We also present the first results of the transverse spin densities of the strange quark inside a nucleon.

PhysicsQuarkStrange quarkParticle physicsHigh Energy Physics::LatticePhysicsQC1-999High Energy Physics::PhenomenologyNuclear TheoryNuclear physicsTransverse planePionLattice (order)Tensor formHigh Energy Physics::ExperimentNucleonNuclear ExperimentEPJ Web of Conferences
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The Influence of Flow on the Jet Quenching Power in Heavy-Ion Collisions

2005

The flow pattern and evolution of the medium created in ultrarelativistic heavy ion collisions can have significant influence on the energy loss of hard partons traversing the medium. We demonstrate that within a range of assumptions for longitudinal and transverse flow which are all compatible with the measured hadronic single particle distributions, the quenching power of the medium can vary within almost a factor five. Thus, the choice of the medium evolution is one of the biggest uncertainties in jet quenching calculations and needs to be addressed with some care.

PhysicsQuenchingNuclear and High Energy PhysicsRange (particle radiation)Particle physicsFlow (psychology)HadronFOS: Physical sciencesGeneral Physics and AstronomyPartonNuclear physicsHigh Energy Physics - PhenomenologyTransverse planeHigh Energy Physics - Phenomenology (hep-ph)ParticleNuclear ExperimentJet quenchingActa Physica Hungarica A) Heavy Ion Physics
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