Search results for "elliptic flow"

showing 10 items of 111 documents

Thermal photon v3 at LHC from fluctuating initial conditions

2014

Abstract We calculate the triangular flow parameter v 3 of thermal photons for 0–40% central collisions of Pb nuclei at LHC using an event-by-event hydrodynamic model with fluctuating initial conditions. Thermal photon v 3 with respect to the participant plane angle is found to be positive and significant compared to the elliptic flow parameter v 2 of thermal photons. In addition, photon v 3 as a function of p T shows similar qualitative nature to photon v 2 in the region 1 p T 6 GeV / c . We argue that while v 3 originates from ϵ 3 deformations of the initial state density distribution, fast buildup of radial flow due to fluctuations is the main driving mechanism for the observed large val…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderPhotonDistribution (mathematics)Flow (mathematics)Plane (geometry)ThermalElliptic flowFunction (mathematics)Atomic physicsNuclear Physics A
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Hydrodynamic simulation of elliptic flow

1999

We use a hydrodynamic model to study the space-time evolution transverse to the beam direction in ultrarelativistic heavy-ion collisions with nonzero impact parameters. We focus on the influence of early pressure on the development of radial and elliptic flow. We show that at high energies elliptic flow is generated only during the initial stages of the expansion while radial flow continues to grow until freeze-out. Quantitative comparisons with SPS data from semiperipheral Pb+Pb collisions suggest the applicability of hydrodynamical concepts already $\approx$ 1 fm/c after impact.

PhysicsNuclear and High Energy PhysicsNuclear TheoryElliptic flowFOS: Physical sciencesMechanicsNuclear Theory (nucl-th)Transverse planeNuclear Physics - TheoryBeam directionRadial flowDevelopment (differential geometry)Focus (optics)Nuclear Experiment
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Evolution of fluctuations in the initial state of heavy-ion collisions from RHIC to LHC

2019

Fluctuations in the initial state of heavy-ion collisions are larger at RHIC energy than at LHC energy. This fact can be inferred from recent measurements of the fluctuations of the particle multiplicities and of elliptic flow performed at the two different energies. We show that an analytical description of the initial energy-density field and its fluctuations motivated by the color glass condensate (CGC) effective theory predicts and quantitatively captures the measured energy evolution of these observables. The crucial feature is that fluctuations in the CGC scale like the inverse of the saturation scale of the nuclei.

heavy ion: scatteringScale (ratio)Field (physics)Nuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]FOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesColor-glass condensateHigh Energy Physics - ExperimentNuclear physicsNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective field theory[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment (nucl-ex)010306 general physicsinitial stateNuclear ExperimentNuclear ExperimentBrookhaven RHIC CollPhysicsLarge Hadron Collider010308 nuclear & particles physicsfluctuationelliptic flowparticle: multiplicityElliptic flowObservableHigh Energy Physics - PhenomenologyCERN LHC Coll[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]color glass condensateParticlescale: saturation
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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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Energy loss in a fluctuating hydrodynamical background

2011

Recently it has become apparent that event-by-event fluctuations in the initial state of hydrodynamical modelling of ultrarelativistic heavy-ion collisions are crucial in order to understand the full centrality dependence of the elliptic flow coefficient v_2. In particular, in central collisions the density fluctuations play a major role in generating the spatial eccentricity in the initial state. This raises the question to what degree high P_T physics, in particular leading-parton energy loss, which takes place in the background of an evolving medium, is sensitive to the presence of the event-by-event density fluctuations in the background. In this work, we report results for the effects …

PhysicsNuclear and High Energy PhysicsParticle physicsta114Degree (graph theory)010308 nuclear & particles physicsPlane (geometry)Elliptic flowOrder (ring theory)FOS: Physical sciences01 natural sciencesNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesRadiative transfer010306 general physicsRelativistic Heavy Ion ColliderEccentricity (mathematics)Nuclear ExperimentEvent (particle physics)
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Elliptic flow from event-by-event hydrodynamics with fluctuating initial state

2011

We develop an event-by-event ideal hydrodynamical framework where initial state density fluctuations are present and where we use a similar flow-analysis method as in the experiments to make a one-to-one $v_2$ comparison with the measured data. Our studies also show that the participant plane is quite a good approximation for the event plane.

PhysicsNuclear and High Energy PhysicsIdeal (set theory)Nuclear Theoryta114010308 nuclear & particles physicsPlane (geometry)Event (relativity)Elliptic flowFOS: Physical sciencesState (functional analysis)01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)State density0103 physical sciencesStatistical physics010306 general physicsNuclear theory
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Measurement of the (anti-)3He elliptic flow in Pb–Pb collisions at sNN=5.02TeV

2020

The elliptic flow ( v 2 ) of (anti-) 3He is measured in Pb–Pb collisions at s NN = 5.02 TeV in the transverse-momentum ( p T ) range of 2–6 GeV/c for the centrality classes 0–20%, 20–40%, and 40–60% using the event-plane method. This measurement is compared to that of pions, kaons, and protons at the same center-of-mass energy. A clear mass ordering is observed at low p T , as expected from relativistic hydrodynamics. The violation of the scaling of v 2 with the number of constituent quarks at low p T , already observed for identified hadrons and deuterons at LHC energies, is confirmed also for (anti-) 3He. The elliptic flow of (anti-) 3He is underestimated by the Blast-Wave model and overe…

PhysicsQuarkNuclear and High Energy Physics010308 nuclear & particles physicsNuclear TheoryElliptic flowHadron01 natural sciencesNuclear physicsPionHelium-30103 physical sciencesNeutronNuclear Experiment010306 general physicsNucleonScalingPhysics Letters B
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Measurement of deuteron spectra and elliptic flow in Pb–Pb collisions at √sNN = 2.76 TeV at the LHC

2017

The transverse momentum (pT) spectra and elliptic flow coefficient (v2) of deuterons and anti-deuterons at mid-rapidity (|y| 1.8 GeV/c within the experimental uncertainties. The measurement of the coalescence parameter B2 is performed, showing a pT dependence in contrast with the simplest coalescence model, which fails to reproduce also the measured v2 coefficient. In addition, the coalescence parameter B2 and the elliptic flow coefficient in the 20–40% centrality interval are compared with the AMPT model which is able, in its version without string melting, to reproduce the measured v2(pT) and the B2(pT) trend. peerReviewed

Physics and Astronomy (miscellaneous)Pb–Pb collisionselliptic flowdeuteron spectraNuclear ExperimentEngineering (miscellaneous)
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J/ψElliptic Flow in Pb-Pb Collisions atsNN=2.76  TeV

2013

We report on the first measurement of inclusive J/psi elliptic flow v(2) in heavy-ion collisions at the LHC. The measurement is performed with the ALICE detector in Pb-Pb collisions at root s(NN) = 2.76 TeV in the rapidity range 2.5 < y < 4.0. The dependence of the J/psi v(2) on the collision centrality and on the J/psi transverse momentum is studied in the range 0 <= p(T) < 10 GeV/c. For semicentral Pb-Pb collisions at root s(NN) = 2.76 TeV, an indication of nonzero v(2) is observed with a largest measured value of v(2) = 0.116 +/-0.046(stat) +/- 0.029(syst) for J/psi in the transverse momentum range 2 <= p(T) < 4 GeV/c. The elliptic flow measurement complements the previously reported ALI…

PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsElliptic flowGeneral Physics and AstronomyModification factor01 natural sciencesDeconfinementCharm quarkNuclear physics0103 physical sciencesQuark–gluon plasmaTransverse momentumHigh Energy Physics::ExperimentRapidityNuclear Experiment010306 general physicsPhysical Review Letters
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Correlated gluonic hot spots meet symmetric cumulants data at LHC energies

2019

We present a systematic study on the influence of spatial correlations between the proton constituents, in our case gluonic hot spots, their size and their number on the symmetric cumulant SC(2, 3), at the eccentricity level, within a Monte Carlo Glauber framework [1]. When modeling the proton as composed by 3 gluonic hot spots, the most common assumption in the literature, we find that the inclusion of spatial correlations is indispensable to reproduce the negative sign of SC(2, 3) in the highest centrality bins as dictated by data. Further, the subtle interplay between the different scales of the problem is discussed. To conclude, the possibility of feeding a 2+1D viscous hydrodynamic sim…

COLLISIONSNuclear and High Energy PhysicsParticle physicsNuclear TheoryFLOWMonte Carlo methodFOS: Physical sciencesSmall systemshiukkasfysiikka114 Physical sciences01 natural sciences7. Clean energyHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)correlations0103 physical sciencesEntropy (information theory)ddc:530initial state010306 general physicsCumulantPhysicsLarge Hadron Colliderta114010308 nuclear & particles physicselliptic flowElliptic flowhot spotsHigh Energy Physics - Phenomenologysmall systemsSubstructureGlauberNuclear Physics A
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