Search results for "Collision"

showing 10 items of 908 documents

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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Beam Energy Scan of Specific Heat Through Temperature Fluctuations in Heavy Ion Collisions

2016

Temperature fluctuations may have two distinct origins, first, quantum fluctuations that are initial state fluctuations, and second, thermodynamical fluctuations. We discuss a method of extracting the thermodynamic temperature from the mean transverse momentum of pions, by using controllable parameters such as centrality of the system, and range of the transverse momenta. Event-by-event fluctuations in global temperature over a large phase space provide the specific heat of the system. We present Beam Energy Scan of specific heat from data, AMPT and HRG model prediction. Experimental results from NA49, STAR, PHENIX, PHOBOS and ALICE are combined to obtain the specific heat as a function of …

Physicsthermodynamical fluctuationHistory010308 nuclear & particles physicsbeam energy scanheavy ion collisionsThermal fluctuationsThermodynamic temperature01 natural sciencesComputer Science ApplicationsEducationNuclear physicsTransverse planePionLattice (order)Phase space0103 physical sciences010306 general physicsNuclear ExperimentQuantum fluctuationEvent generator
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A Wind Tunnel Study of the Effects of Turbulence on the Growth of Cloud Drops by Collision and Coalescence

1999

A set of wind tunnel experiments was carried out to investigate the growth of single drops by collision coalescence with small droplets in laminar and turbulent flow. Analysis of the experiments shows that under otherwise similar conditions, there exists a tendency toward a faster drop growth under turbulence. The observed growth under laminar conditions agrees well with computed continuous growth of a collector drop using collision efficiencies reported in the literature.

Physics::Fluid DynamicsCoalescence (physics)PhysicsAtmospheric ScienceOpticsbusiness.industryTurbulenceDrop (liquid)Laminar flowMechanicsbusinessCollisionWind tunnelJournal of the Atmospheric Sciences
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"Table 3" of "Measurement of azimuthal anisotropy of muons from charm and bottom hadrons in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detec…

2020

Summary of results for charm and bottom muon v2 as a function of multiplicity. Uncertainties are statistical and systematic, respectively.

Physics::Fluid Dynamicsv213000.0Physics::Instrumentation and DetectorsP P --> HF muon + XHigh Energy Physics::ExperimentHF muonProton-Proton Collision
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"Table 41" of "Multiplicity dependence of K*(892)$^{0}$ and $\phi$(1020) production in pp collisions at $\sqrt{s}$ = 13 TeV"

2020

K$^{*0}$ transverse momentum integrated yield vs multiplicity - V0M multiplicity classes, average of particle and antiparticle

Physics::General PhysicsP P --> Kstar+XKstar13000.0Proton-Proton CollisionsSIGyieldResonanceV0M Multiplicity
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"Table 2" of "Multiplicity dependence of K*(892)$^{0}$ and $\phi$(1020) production in pp collisions at $\sqrt{s}$ = 13 TeV"

2020

K$^{*0}$ transverse momentum spectrum - V0M multiplicity class II, average of particle and antiparticle

Physics::General PhysicsP P --> Kstar+XKstar13000.0YieldsProton-Proton CollisionsComputer Science::Computational GeometrySIGResonanceV0M Multiplicity
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"Table 1" of "Multiplicity dependence of K*(892)$^{0}$ and $\phi$(1020) production in pp collisions at $\sqrt{s}$ = 13 TeV"

2020

K$^{*0}$ transverse momentum spectrum - V0M multiplicity class I, average of particle and antiparticle

Physics::General PhysicsP P --> Kstar+XKstar13000.0YieldsProton-Proton CollisionsHigh Energy Physics::ExperimentNuclear ExperimentSIGResonanceV0M Multiplicity
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"Table 4" of "Multiplicity dependence of K*(892)$^{0}$ and $\phi$(1020) production in pp collisions at $\sqrt{s}$ = 13 TeV"

2020

K$^{*0}$ transverse momentum spectrum - V0M multiplicity class IV+V, average of particle and antiparticle

Physics::General PhysicsP P --> Kstar+XKstar13000.0YieldsProton-Proton CollisionsSIGResonancePhysics::GeophysicsV0M Multiplicity
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"Table 6" of "Multiplicity dependence of K*(892)$^{0}$ and $\phi$(1020) production in pp collisions at $\sqrt{s}$ = 13 TeV"

2020

K$^{*0}$ transverse momentum spectrum - V0M multiplicity class VII, average of particle and antiparticle

Physics::General PhysicsP P --> Kstar+XKstar13000.0YieldsProton-Proton CollisionsSIGResonanceV0M Multiplicity
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"Table 9" of "Multiplicity dependence of K*(892)$^{0}$ and $\phi$(1020) production in pp collisions at $\sqrt{s}$ = 13 TeV"

2020

K$^{*0}$ transverse momentum spectrum - V0M multiplicity class X, average of particle and antiparticle

Physics::General PhysicsP P --> Kstar+XKstar13000.0YieldsProton-Proton CollisionsSIGResonanceV0M Multiplicity
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