Search results for "Heavy Ion"

showing 10 items of 314 documents

Collision centrality andτ0dependence of the emission of thermal photons from a fluctuating initial state in an ideal hydrodynamic calculation

2012

Fluctuations in the initial QCD matter density distribution are found to enhance the production of thermal photons significantly in the range $2\ensuremath{\leqslant}{p}_{T}\ensuremath{\leqslant}4$ GeV/$c$ compared to a smooth initial state averaged profile in ideal hydrodynamic calculation for $200A$ GeV Au+Au collisions at the Relativistic Heavy Ion Collider (RHIC) and $2.76A$ TeV Pb+Pb collisions at the Large Hadron Collider (LHC). The thermal emission of photons is strongly dependent on the initial temperature of the system where the presence of ``hot spots'' in the initial state translates into enhanced production of photons compared to a smooth profile. The effect of fluctuations in t…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsRange (particle radiation)Photon010308 nuclear & particles physicsPlasma01 natural sciencesSpectral lineNuclear physics0103 physical sciencesProduction (computer science)Atomic physicsNuclear Experiment010306 general physicsRelativistic Heavy Ion ColliderQCD matterPhysical Review C
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Neutral pion production with respect to centrality and reaction plane in Au+Au collisions atsNN=200GeV

2013

The PHENIX experiment has measured the production of pi(0)s in Au + Au collisions at root S-NN = 200 GeV. The new data offer a fourfold increase in recorded luminosity, providing higher precision and a larger reach in transverse momentum, p(T), to 20 GeV/c. The production ratio of eta/pi(0) is 0.46 +/- 0.01(stat) +/- 0.05(syst), constant with p(T) and collision centrality. The observed ratio is consistent with earlier measurements, as well as with the p + p and d + Au values. pi(0) are suppressed by a factor of 5, as in earlier findings. However, with the improved statistical precision a small but significant rise of the nuclear modification factor R-AA vs p(T), with a slope of 0.0106 +/-(0…

PhysicsQuantum chromodynamicsNuclear physicsNuclear and High Energy PhysicsAdS/CFT correspondenceParticle physicsPionLuminosity (scattering theory)Path lengthConformal field theoryPartonRelativistic Heavy Ion ColliderPhysical Review C
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Dilepton Emission from Dense Hadron Gas

1997

Using a Hagedorn resonance gas picture and quark-hadron duality we estimate the dilepton emission rate in the vicinity of the QCD deconfinement phase transition. The result is then used to calculate a dilepton spectrum in ultrarelativistic heavy ion collisions. We show that multibody contributions taken into account in the Hagedorn resonance gas approach provide an enhancement of the production rate of massive dileptons as compared to the previously considered sources.

PhysicsQuantum chromodynamicsParticle physicsPhase transitionPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeHadronNuclear TheoryHigh Energy Physics::PhenomenologyDuality (optimization)FOS: Physical sciencesResonance (particle physics)DeconfinementNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Heavy ionHigh Energy Physics::ExperimentNuclear ExperimentEngineering (miscellaneous)Production rate
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Measurement ofKS0andK*0inp+p,d+Au, and Cu + Cu collisions atsNN=200 GeV

2014

The PHENIX experiment at the Relativistic Heavy Ion Collider has performed a systematic study of K-S(0) and K*(0) meson production at midrapidity in p + p, d + Au, and Cu + Cu collisions at root s(NN) = 200 GeV. The K-S(0) and K*(0) mesons are reconstructed via their K-S(0) -> pi(0)(-> gamma gamma) pi(0)(-> gamma gamma) and K*(0) -> K-+/-pi(-/+) decay modes, respectively. The measured transverse-momentum spectra are used to determine the nuclear modification factor of K-S(0) and K*(0) mesons in d + Au and Cu + Cu collisions at different centralities. In the d + Au collisions, the nuclear modification factor of K-S(0) and K*(0) mesons is almost constant as a function of transverse momentum a…

PhysicsQuarkNuclear and High Energy PhysicsMesonNuclear TheoryStrangenessPhi mesonBaryonNuclear physicsDeuteriumHigh Energy Physics::ExperimentImpact parameterNuclear ExperimentRelativistic Heavy Ion ColliderPhysical Review C
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Nuclear Contact Times in Dissipative Heavy Ion Collsions Measured Via γ-Ray Spectroscopy

1987

Electron spectra have been measured for elastic and dissipative U + Au collisions at 8.6 MeV/u and analysed within a simple schematic model which describes γ-ray emission in the presence of a nuclear contact time and a total kinetic energy loss (TKEL). A nearly linear dependence of the mean nuclear contact time τ and TKEL was found, reaching τ = 1.1 * 10-21 s with a variance σ = ±0.4 * 10-21 s for a TKEL of (400 ± 50) MeV.

PhysicsSIMPLE (dark matter experiment)Contact timeDissipative systemHeavy ionSchematic modelAtomic physicsImpact parameterSpectroscopyKinetic energy
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Measurement of ϕ -meson production at forward rapidity in p+p collisions at s=510  GeV and its energy dependence from s=200  GeV to 7 TeV

2018

The PHENIX experiment at the Relativistic Heavy Ion Collider has measured the differential cross section of φ(1020)-meson production at forward rapidity in p+p collisions at s=510 GeV via the dimuon decay channel. The partial cross section in the rapidity and pT ranges 1.2

PhysicsScattering cross-sectionMeson production010308 nuclear & particles physicsNuclear TheoryStrangeness01 natural sciencesNuclear physics0103 physical sciencesQuark–gluon plasmaHigh Energy Physics::ExperimentRapidityNuclear Experiment010306 general physicsRelativistic Heavy Ion ColliderPhysical Review D
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Recent results on heavy-ion direct reactions of interest for 0νββ decay at INFN - LNS

2020

Abstract Neutrinoless double beta decay of nuclei, if observed, would have important implications on fundamental physics. In particular it would give access to the effective neutrino mass. In order to extract such information from 0νββ decay half-life measurements, the knowledge of the Nuclear Matrix Elements (NME) is of utmost importance. In this context the NUMEN and the NURE projects aim to extract information on the NME by measuring cross sections of Double Charge Exchange reactions in selected systems which are expected to spontaneously decay via 0νββ. In this work an overview of the experimental challenges that NUMEN is facing in order to perform the experiments with accelerated beams…

Physicsnucleus: semileptonic decayHistoryparticle: Majoranahiukkasfysiikkacross section: measured[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]charge exchangemagnetic spectrometerComputer Science ApplicationsEducationNuclear physicsdouble-beta decay: (0neutrino)Heavy ionupgradeneutrino: massenergy resolution: highydinfysiikkabeam: heavy ionexperimental resultsJournal of Physics: Conference Series
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Heavy Ion Sensitivity of 16/32-Gbit NAND-Flash and 4-Gbit DDR3 SDRAM

2012

16/32-Gbit NAND-Flash and 4-Gbit DDR3 SDRAM memories have been tested under heavy ion irradiation. At high LET, 25nm NAND-Flash show MBUs at normal incidence. Techniques for SEFI mitigation in DDR3 SDRAM are studied.

Physicsta114business.industryNAND gateDDR3 SDRAMHeavy ion irradiationFlash (photography)MBusGigabitElectronic engineeringOptoelectronicsHeavy ionbusinessSensitivity (electronics)
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SEU and MBU Angular Dependence of Samsung and Micron 8-Gbit SLC NAND-Flash Memories under Heavy-Ion Irradiation

2011

The angular dependence of the SEU and MBU cross sections of two 8-Gbit NAND-Flash memories, Samsung and Micron, is measured under Ar, Fe, and Kr irradiation. The omnidirectional sensitivity is calculated based on experimental results.

Physicsta114ta213business.industryElectrical engineeringNAND gateOptoelectronicsAngular dependenceIrradiationbusinessHeavy ion irradiationIon2011 IEEE Radiation Effects Data Workshop
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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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