Search results for "Anisotropy"

showing 10 items of 912 documents

Measurement of the azimuthal anisotropy for charged particle production insNN=2.76TeV lead-lead collisions with the ATLAS detector

2012

Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at root sNN = 2.76 TeV with the ATLAS detector at the LHC, based on an integrated luminosity of approximately 8 mu b(-1). This anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients v(n) denoting the magnitude of the anisotropy. Significant v(2)-v(6) values are obtained as a function of transverse momentum (0.5 = 3 are found to vary weakly with both eta and centrality, and their p(T) dependencies are found to follow an approximate scaling relation, v(n)(1/n)(p(T)) proportional …

PhysicsNuclear and High Energy PhysicsLuminosity (scattering theory)010308 nuclear & particles physicsElliptic flow01 natural sciencesCharged particleNuclear physicsDistribution (mathematics)FactorizationPseudorapidity0103 physical sciencesQuark–gluon plasmaNuclear Experiment010306 general physicsAnisotropyPhysical Review C
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Event-by-event distributions of azimuthal asymmetries in ultrarelativistic heavy-ion collisions

2012

Relativistic dissipative fluid dynamics is a common tool to describe the space-time evolution of the strongly interacting matter created in ultrarelativistic heavy-ion collisions. For a proper comparison to experimental data, fluid-dynamical calculations have to be performed on an event-by-event basis. Therefore, fluid dynamics should be able to reproduce, not only the event-averaged momentum anisotropies, $$, but also their distributions. In this paper, we investigate the event-by-event distributions of the initial-state and momentum anisotropies $\epsilon_n$ and $v_n$, and their correlations. We demonstrate that the event-by-event distributions of relative $v_n$ fluctuations are almost eq…

PhysicsNuclear and High Energy PhysicsNuclear Theoryta114FOS: Physical sciencesNuclear Theory (nucl-th)MomentumViscosityQuantum electrodynamicsQuark–gluon plasmaDissipative systemFluid dynamicsBoundary value problemAnisotropyEvent (particle physics)Physical Review C
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Improvement of cosmological neutrino mass bounds

2016

The most recent measurements of the temperature and low-multipole polarization anisotropies of the cosmic microwave background from the Planck satellite, when combined with galaxy clustering data f ...

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsCosmic microwave backgroundAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsPolarization (waves)01 natural sciencesGalaxysymbols.namesake0103 physical sciencessymbolsNeutrinoPlanckAnisotropyCluster analysis010303 astronomy & astrophysicsHubble's lawPhysical Review D
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Measuring the cosmological background of relativistic with the Wilkinson Microwave Anisotropy Probe

2003

We show that the first year results of the Wilkinson Microwave Anisotropy Probe (WMAP) constrain very efficiently the energy density in relativistic particles in the Universe. We derive new bounds on additional relativistic degrees of freedom expressed in terms of an excess in the effective number of light neutrinos $\ensuremath{\Delta}{N}_{\mathrm{eff}}.$ Within the flat \ensuremath{\Lambda}CDM scenario, the allowed range is $\ensuremath{\Delta}{N}_{\mathrm{eff}}l6$ (95% confidence level) using WMAP data only, or $\ensuremath{-}2.6l\ensuremath{\Delta}{N}_{\mathrm{eff}}l4$ with the prior ${H}_{0}=72\ifmmode\pm\else\textpm\fi{}8\mathrm{km}{\mathrm{s}}^{\ensuremath{-}1}{\mathrm{Mpc}}^{\ensure…

PhysicsNuclear and High Energy PhysicsParticle physicsCosmic microwave backgroundFísicaAstrophysics::Cosmology and Extragalactic AstrophysicsLambdaCMB cold spotRelativistic particleBig Bang nucleosynthesisObservational cosmologyNeutrinoAnisotropy
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Azimuthal anisotropy ofD-meson production in Pb-Pb collisions atsNN=2.76TeV

2014

The production of the prompt charmed mesons D0, D+, and D*+ relative to the reaction plane was measured in Pb-Pb collisions at a center-of-mass energy per nucleon-nucleon collision of √sNN=2.76TeV with the ALICE detector at the CERN Large Hadron Collider. D mesons were reconstructed via their hadronic decays at central rapidity in the transverse-momentum (p_T) interval 2–16 GeV/c. The azimuthal anisotropy is quantified in terms of the second coefficient v2 in a Fourier expansion of the D-meson azimuthal distribution and in terms of the nuclear modification factor R_AA, measured in the direction of the reaction plane and orthogonal to it. The v2 coefficient was measured with three different …

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderMeson010308 nuclear & particles physicsPlane (geometry)Hadron01 natural sciences7. Clean energyNuclear physicsYield (chemistry)0103 physical sciencesD mesonHigh Energy Physics::ExperimentRapidityNuclear Experiment010306 general physicsAnisotropyPhysical Review C
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Anisotropy of flow and the order of phase transition in relativistic heavy ion collisions

2005

Using a hydrodynamical model we study how the order of phase transition in the equation of state of strongly interacting matter affects single particle spectra, elliptic flow and higher order anisotropies in Au+Au collisions at RHIC (sqrt{s_NN}=200 GeV energy). We find that the single particle spectra are independent of the order of phase transition and that the fourth harmonic v_4(p_T) shows only a weak dependence in the p_T region where hydrodynamics is expected to work. The differential elliptic flow, v_2(p_T), of baryons shows the strongest dependence on equation of state. Surprisingly the closest fit to data was obtained when the equation of state had a strong first order phase transit…

PhysicsNuclear and High Energy PhysicsPhase transitionNuclear Theory010308 nuclear & particles physicsHadronElliptic flowFOS: Physical sciences7. Clean energy01 natural sciencesSpectral lineNuclear Theory (nucl-th)BaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum electrodynamics0103 physical sciencesFourth harmonicHeavy ionNuclear Experiment (nucl-ex)Nuclear Experiment010306 general physicsAnisotropyNuclear ExperimentNuclear Physics A
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Neutron yields from a thick 13C target irradiated by 30 MeV protons

2002

Abstract Total neutron yields resulting from the proton bombardment of a thick 13 C target have been measured for 30 MeV protons. Absolute intensities, angular distributions and energy spectra of neutrons have been obtained by the time-of-flight technique where the detectors provided continuous coverage from 0° to 120°. Resonances have been found, some of which can be attributed to known states in 14 N. A total yield of 0.022(3) n/p was observed with a slight angular anisotropy towards forward angles. The measured yields are compared to the neutron yields produced by using deuterons on thick 12 C and 9 Be targets.

PhysicsNuclear and High Energy PhysicsProtonNuclear TheoryTotal neutronSpectral lineDeuteriumYield (chemistry)NeutronIrradiationAtomic physicsAngular anisotropyNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Energy dependence of collective flow of neutrons and protons in197Au+197Au collisions

1994

We investigate the beam energy dependence of neutron and proton squeeze-out in collisions of197Au+197Au atE/A=400—800 MeV. The azimuthal anisotropy that describes the enhanced emission of mid-rapidity neutrons perpendicular to the reaction plane rises strongly with the transverse momentum of the neutrons. This dependence of the azimuthal anisotropy follows a universal curve — independent of beam energy — if the neutron momenta are measured in fractions of the projectile momentum per mass unit. Analogously, the kinetic energy spectra of mid-rapidity neutrons exhibit a universal behaviour as a function of the kinetic energy of the projectile.

PhysicsNuclear and High Energy PhysicsProtonProjectileAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryKinetic energyNeutron time-of-flight scatteringMomentumNuclear physicsNuclear fusionNeutronAtomic physicsNuclear ExperimentAnisotropyZeitschrift für Physik A Hadrons and Nuclei
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Azimuthal anisotropy ofπ0andηmesons in Au + Au collisions atsNN=200GeV

2013

The azimuthal anisotropy coefficients v2 and v4 of p 0 and. mesons are measured in Au + Au collisions at root s(NN) = 200 GeV as a function of transverse momentum p(T) (1-14 GeV/c) and centrality. The extracted v(2) coefficients are found to be consistent between the two meson species over the measured p(T) range. The ratio of v(4)/v(2)(2) for pi(0) mesons is found to be independent of p(T) for 1- 9 GeV/c, implying a lack of sensitivity of the ratio to the change of underlying physics with p(T). Furthermore, the ratio of v(4)/v(2)(2) is systematically larger in central collisions, which may reflect the combined effects of fluctuations in the initial collision geometry and finite viscosity i…

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Meson010308 nuclear & particles physicsElliptic flow01 natural sciencesNuclear physicsAzimuthViscosity0103 physical sciencesTransverse momentumHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsRelativistic Heavy Ion ColliderAnisotropyPhysical Review C
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Initial state anisotropies and their uncertainties in ultrarelativistic heavy-ion collisions from the Monte Carlo Glauber model

2011

In hydrodynamical modeling of heavy-ion collisions, the initial-state spatial anisotropies are translated into momentum anisotropies of the final-state particle distributions. Thus, understanding the origin of the initial-state anisotropies and their uncertainties is important before extracting specific QCD matter properties, such as viscosity, from the experimental data. In this work we review the wounded nucleon approach based on the Monte Carlo Glauber model, charting in particular the uncertainties arising from modeling of the nucleon-nucleon interactions between the colliding nucleon pairs and nucleon-nucleon correlations inside the colliding nuclei. We discuss the differences between …

PhysicsNuclear and High Energy PhysicsWork (thermodynamics)Nuclear Theoryta114010308 nuclear & particles physicsMonte Carlo methodNuclear TheoryFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)MomentumNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesQuark–gluon plasma010306 general physicsNucleonAnisotropyNuclear ExperimentGlauberQCD matterPhysical review C
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