Search results for " collisions"

showing 10 items of 516 documents

Nonresistive dissipative magnetohydrodynamics from the Boltzmann equation in the 14-moment approximation

2018

We derive the equations of motion of relativistic, non-resistive, second-order dissipative magnetohydrodynamics from the Boltzmann equation using the method of moments. We assume the fluid to be composed of a single type of point-like particles with vanishing dipole moment or spin, so that the fluid has vanishing magnetization and polarization. In a first approximation, we assume the fluid to be non-resistive, which allows to express the electric field in terms of the magnetic field. We derive equations of motion for the irreducible moments of the deviation of the single-particle distribution function from local thermodynamical equilibrium. We analyze the Navier-Stokes limit of these equati…

Nuclear TheoryTRANSIENT RELATIVISTIC THERMODYNAMICSFOS: Physical scienceshiukkasfysiikkaHEAVY-ION COLLISIONSmagneettikentätSystem of linear equations114 Physical sciences01 natural sciencesMAGNETIC-FIELDSBoltzmann equationNuclear Theory (nucl-th)HYDRODYNAMICSHigh Energy Physics - Phenomenology (hep-ph)FLUIDS0103 physical sciences010306 general physicsKINETIC-THEORYnestefysiikkaPhysicsta114010308 nuclear & particles physicsFluid Dynamics (physics.flu-dyn)Equations of motionPhysics - Fluid DynamicsBoltzmann equationMagnetic fieldnonresistivenessHigh Energy Physics - PhenomenologyDipoleDistribution functionClassical mechanicsDissipative systemMagnetohydrodynamicsmagnetohydrodynamicsPhysical Review D
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Production of π0 and η mesons in Cu+Au collisions at √sNN = 200 GeV

2018

Production of π0 and η mesons has been measured at midrapidity in Cu+Au collisions at √sNN = 200 GeV. Measurements were performed in π0 (η) → γ γ decay channel in the 1(2)-20 GeV/c transverse momentum range. A strong suppression is observed for π0 and η meson production at high transverse momentum in central Cu+Au collisions relative to the p + p results scaled by the number of nucleon-nucleon collisions. In central collisions the suppression is similar to Au + Au with comparable nuclear overlap. The η/π0 ratio measured as a function of transverse momentum is consistent with mT -scaling parametrization down to pT = 2 GeV/c, its asymptotic value is constant and consistent with Au + Au and p …

Nuclear Theoryeta mesonsHigh Energy Physics::ExperimentpionshiukkasfysiikkaNuclear Experimentrelativistic heavy-ion collisions
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Kaon femtoscopy in Pb-Pb collisions at √sNN = 2.76 TeV

2017

We present the results of three-dimensional femtoscopic analyses for charged and neutral kaons recorded by ALICE in Pb-Pb collisions at √ s NN = 2.76 TeV. Femtoscopy is used to measure the space-time characteristics of particle production from the effects of quantum statistics and final-state interactions in two-particle correlations. Kaon femtoscopy is an important supplement to that of pions because it allows one to distinguish between different model scenarios working equally well for pions. In particular, we compare the measured three-dimensional kaon radii with a purely hydrodynamical calculation and a model where the hydrodynamic phase is followed by a hadronic rescattering stage. The…

Nuclear TheoryfemtoscopyPb-Pb collisionsHigh Energy Physics::ExperimentkaonshiukkasfysiikkaNuclear Experiment
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Linearly polarized gluons and axial charge fluctuations in the glasma

2018

We calculate of the one- and two-point correlation functions of the energy density and the divergence of the Chern-Simons current in the nonequilibrium Glasma state formed in a high-energy nuclear collision. We show that the latter depends on the difference of the total and linearly polarized gluon transverse momentum distributions. Since the divergence of the Chern-Simons current provides the source of axial charge, we infer information about the statistical properties of axial charge production at early times. We further develop a simple phenomenological model to characterize axial charge distributions in terms of distributions of the energy density.

Nuclear Theoryquark-gluon plasmaField (physics)FLOWFOS: Physical sciencesparticle productionNon-equilibrium thermodynamicsHEAVY-ION COLLISIONS114 Physical sciences01 natural sciencesHYDRODYNAMICSNuclear Theory (nucl-th)hiukkasetHigh Energy Physics - Phenomenology (hep-ph)nuclear physicsCONDENSATE0103 physical sciencesPhenomenological modelFIELD010306 general physicsDivergence (statistics)plasmaPhysicsta114ionitkvarkit010308 nuclear & particles physicsLinear polarizationkvarkki-gluoniplasmaCharge densityCharge (physics)EVOLUTIONGluonHigh Energy Physics - PhenomenologyDENSITYQuantum electrodynamicsENERGY NUCLEAR COLLISIONSAtomic physicsydinfysiikkarelativistic heavy-ion collisionsPhysical Review
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Production of deuterons, tritons, 3He nuclei, and their antinuclei in pp collisions at √s = 0.9, 2.76, and 7 TeV

2018

Invariant differential yields of deuterons and antideuterons in p p collisions at √ s = 0.9, 2.76 and 7 TeV and the yields of tritons, 3 He nuclei, and their antinuclei at √ s = 7 TeV have been measured with the ALICE detector at the CERN Large Hadron Collider. The measurements cover a wide transverse momentum ( p T ) range in the rapidity interval | y | < 0.5 , extending both the energy and the p T reach of previous measurements up to 3 GeV/ c for A = 2 and 6 GeV/ c for A = 3 . The coalescence parameters of (anti)deuterons and 3 ¯¯¯¯ He nuclei exhibit an increasing trend with p T and are found to be compatible with measurements in p A collisions at low p T and lower energies. The integrate…

Nuclear and High Energy Physics3HeNuclear Theoryparticle productionHigh Energy Physics::ExperimenttritonsdeuteronsNuclear Experimentpp collisions
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Dielectron production in proton-proton and proton-lead collisions at √sNN=5.02TeV

2020

The first measurements of dielectron production at midrapidity (|ηe| &lt; 0.8) in proton–proton and proton–lead collisions at √sNN = 5.02 TeV at the LHC are presented. The dielectron cross section is measured with the ALICE detector as a function of the invariant mass mee and the pair transverse momentum pT, ee in the ranges mee &lt; 3.5 GeV/c2 and pT, ee &lt; 8 GeV/c, in both collision systems. In proton–proton collisions, the charm and beauty cross sections are determined at midrapidity from a fit to the data with two different event generators. This complements the existing dielectron measurements performed at √s = 7 and 13 TeV. The slope of the √s dependence of the three measurements is…

Nuclear and High Energy Physics:Kjerne- og elementærpartikkelfysikk: 431 [VDP]ProtonHadronNuclear Theorydielectrondielectron production01 natural sciences7. Clean energyNuclear physicshadron-ion interactionshadron-hadron collisions; dielectron production;Ionic Collisionsdielectron cross sectiondielectron nuclear modification factor0103 physical sciencesInvariant massDielectronCharm (quantum number)Dielectron; hadron-hadron interactions; hadron-ion interactionsPhysics::Atomic PhysicsIonic Collisions; Relativistic Heavy-ion Collisions; Quark-Gluon Plasma010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsLarge Hadron Collider010308 nuclear & particles physicsPhysicsVDP::Kjerne- og elementærpartikkelfysikk: 431hadron-hadron interactionNuclear matterhadron-hadron collisionsNATURAL SCIENCES. Physics.ALICE LHC proton-lead collisions proton-proton collisionsPRIRODNE ZNANOSTI. Fizika.:Nuclear and elementary particle physics: 431 [VDP]VDP::Nuclear and elementary particle physics: 431dielectron ; LHC ; dielectron cross section ; dielectron nuclear modification factorQuark–gluon plasmaQuark-Gluon PlasmaHigh Energy Physics::ExperimentLHChadron-hadron interactionsRelativistic Heavy-ion Collisions
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Azimuthally-differential pion femtoscopy relative to the third harmonic event plane in Pb–Pb collisions at √sNN = 2.76 TeV

2018

Azimuthally-differential femtoscopic measurements, being sensitive to spatio-temporal characteristics of the source as well as to the collective velocity fields at freeze out, provide very important information on the nature and dynamics of the system evolution. While the HBT radii oscillations relative to the second harmonic event plane measured recently reflect mostly the spatial geometry of the source, model studies have shown that the HBT radii oscillations relative to the third harmonic event plane are predominantly defined by the velocity fields. In this Letter, we present the first results on azimuthally-differential pion femtoscopy relative to the third harmonic event plane as a fun…

Nuclear and High Energy PhysicsAzimuthally-differential femtoscopic measurementsheavy-ion collisionshiukkasfysiikkaNuclear Experiment
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Status and perspectives of atomic physics research at GSI

2003

A short overview on the results of atomic physics research at the storage ring ESR is given followed by a presentation of the envisioned atomic physics program at the planned new GSI facility. The proposed new GSI facility will provide highest intensities of relativistic beams of both stable and unstable heavy nuclei - up to a Lorentz factor of 24. At those relativistic velocities, the energies of optical transitions, such as for lasers.. are boosted into the X-ray region and the high-charge state ions generate electric and magnetic fields of exceptional strength. Together with high beam intensities a range of important experiments can be anticipated, for example electronic transitions in r…

Nuclear and High Energy PhysicsCOLLISIONSElectronlaw.inventionNuclear physicssymbols.namesakestorage ringslawEXCITATIONLAMB SHIFTInstrumentationPhysicsSPECTROSCOPYQEDLaserMagnetic fieldLamb shiftLorentz factorrelativistic collisionsAtomic electron transitionsymbolsheavy-ion acceleratorAtomic physicsHYDROGENLIKEStorage ringExcitationNuclear Instruments & Methods in Physics Research Section B-Beam Interactions with Materials and Atoms
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Latest predictions from the EbyE NLO EKRT model

2019

We present the latest results from the NLO pQCD + saturation + viscous hydrodynamics (EbyE NLO EKRT) model. The parameters in the EKRT saturation model are fixed by the charged hadron multiplicity in the 0-5 \% 2.76 TeV Pb+Pb collisions. The $\sqrt{s}$, $A$ and centrality dependence of the initial particle production follows then from the QCD dynamics of the model. This allows us to predict the $\sqrt{s}$ and $A$ dependence of the particle production. We show that our results are in an excellent agreement with the low-$p_T$ data from 2.76 TeV and 5.02 TeV Pb+Pb collisions at the LHC as well as with the data from the 200 GeV Au+Au collisions at RHIC. In particular, we study the centrality de…

Nuclear and High Energy PhysicsCOLLISIONSMULTIPLICITIESNuclear TheoryHadronFOS: Physical scienceshiukkasfysiikka7. Clean energy01 natural sciences114 Physical sciencesdissipative fluid dynamicNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsTRANSVERSE ENERGIESNuclear ExperimentNuclear theoryMass numberQuantum chromodynamicsPhysicsLarge Hadron Colliderta114010308 nuclear & particles physicssaturationHigh Energy Physics::PhenomenologyMultiplicity (mathematics)heavy-ion collisionsCharged particleHigh Energy Physics - PhenomenologyHigh Energy Physics::Experimentperturbative QCD calculationsydinfysiikka
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Multiplicity fluctuations in hadronic final states from the decay of the Z0

1992

An analysis of the fluctuations in the phase space distribution of hadrons produced in the decay of 78829 Z0 has been carried out, using the method of factorial moments. The high statistics collected by the DELPHI experiment at LEP during 1990 allowed studies of the event sample both globally and in intervals of p(t) and multiplicity, and for different jet topologies and for single jets. A large contribution to the factorial moments of the one-dimensional data on rapidity with respect to the event axis comes from hard gluons. Details of factorial moments in two and three dimensions are presented. Influences of resonance decays have been studied by Monte Carlo simulation: one-dimensional fac…

Nuclear and High Energy PhysicsFactorialParticle physicsE+E ANNIHILATIONLUND MONTE-CARLOMonte Carlo methodPartonMULTIPARTICLE PRODUCTION01 natural sciences7. Clean energyJET FRAGMENTATIONNuclear physicsParticle decayRAPIDITY DISTRIBUTIONS0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]RapidityZ0010306 general physicsParton showerHIGH-ENERGY COLLISIONSQuantum chromodynamicsPhysics010308 nuclear & particles physicsLUND MONTE-CARLO; HIGH-ENERGY COLLISIONS; E+E ANNIHILATION; MULTIPARTICLE PRODUCTION; RAPIDITY DISTRIBUTIONS; INTERMITTENCY ANALYSIS; JET FRAGMENTATION; Z0; QCD; SIMULATIONQCDINTERMITTENCY ANALYSISGluonSIMULATIONHigh Energy Physics::ExperimentFísica nuclearParticle Physics - Experiment
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