Search results for "Heavy Ion"

showing 10 items of 314 documents

Momentum anisotropy effects for quarkonium in a weakly coupled quark-gluon plasma below the melting temperature

2017

In the early stages of heavy-ion collisions, the hot QCD matter expands more longitudinally than transversely. This imbalance causes the system to become rapidly colder in the longitudinal direction and a local momentum anisotropy appears. In this paper, we study the heavy-quarkonium spectrum in the presence of a small plasma anisotropy. We work in the framework of pNRQCD at finite temperature. We inspect arrangements of non-relativistic and thermal scales complementary to those considered in the literature. In particular, we consider temperatures larger and Debye masses smaller than the binding energy, which is a temperature range relevant for presently running LHC experiments. In this set…

High Energy Physics - Theoryheavy ion: scatteringNuclear Theoryhiukkasfysiikka01 natural sciences7. Clean energy[ PHYS.HTHE ] Physics [physics]/High Energy Physics - Theory [hep-th]High Energy Physics - Phenomenology (hep-ph)quarkonium: heavyquarkonium: mass spectrum[ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)AnisotropyNuclear Experiment[ PHYS.NUCL ] Physics [physics]/Nuclear Theory [nucl-th]quark gluon: plasmaQCD matterDebyeQuantum chromodynamicsPhysics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]quarkonium: momentumQuarkoniumHigh Energy Physics - PhenomenologyQuantum electrodynamicssymbolsquarkonium[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]FOS: Physical sciencesanisotropy[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]plasma: anisotropyNuclear Theory (nucl-th)Momentumsymbols.namesake0103 physical sciencesplasma: expansionparticle physicsquantum chromodynamics: perturbation theory010306 general physicsquantum chromodynamics: matterquantum chromodynamics: nonrelativisticta114effect: anisotropy010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPlasmamomentum: anisotropyquarkonium: dissociationHigh Energy Physics - Theory (hep-th)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Quark–gluon plasma[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Physical Review D
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Transverse momentum dependence of D-meson production in Pb-Pb collisions at √sNN = 2.76 TeV

2016

The production of prompt charmed mesons D0 , D+ and D∗+, and their antiparticles, was measured with the ALICE detector in Pb-Pb collisions at the centre-of-mass energy per nucleon pair, √ sNN, of 2.76 TeV. The production yields for rapidity |y| < 0.5 are presented as a function of transverse momentum, pT, in the interval 1–36 GeV/c for the centrality class 0–10% and in the interval 1–16 GeV/c for the centrality class 30–50%. The nuclear modification factor RAA was computed using a proton-proton reference at √ s = 2.76 TeV, based on measurements at √ s = 7 TeV and on theoretical calculations. A maximum suppression by a factor of 5–6 with respect to binary-scaled pp yields is observed for the…

High Energy Physics::ExperimentNuclear Experimentcharm physicsheavy ion experimentsquark gluon plasma
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Measurement of electrons from beauty-hadron decays in p-Pb collisions at √sNN = 5.02 TeV and Pb-Pb collisions at √sNN = 2.76 TeV

2017

The production of beauty hadrons was measured via semi-leptonic decays at mid-rapidity with the ALICE detector at the LHC in the transverse momentum interval 1<pT< 8 GeV/c in minimum-bias p-Pb collisions at √sNN=5.02 TeV and in 1.3 < pT< 8 GeV/c in the 20% most central Pb-Pb collisions at √sNN=2.76 TeV. The pp reference spectra at √sNN=5.02 TeV and √s=2.76 TeV, needed for the calculation of the nuclear modification factors RpPb and RPbPb, were obtained by a pQCD-driven scaling of the cross section of electrons from beauty-hadron decays measured at √s=7 TeV. In the pT interval 3 < pT< 8 GeV/c, a suppression of the yield of electrons from beauty-hadron decays is observed in Pb-Pb compared to …

High Energy Physics::ExperimenthiukkasfysiikkaNuclear Experimentheavy ion experiments
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Measurement of prompt D0, D+, D*+, and D+S production in p–Pb collisions at √sNN = 5.02 TeV

2019

The measurement of the production of prompt D0, D+, D*+, and D+S mesons in proton–lead (p–Pb) collisions at the centre-of-mass energy per nucleon pair of √sNN = 5.02 TeV, with an integrated luminosity of 292 ± 11 μb−1, are reported. Differential production cross sections are measured at mid-rapidity (−0.96 < ycms< 0.04) as a function of transverse momentum (pT) in the intervals 0 < pT< 36 GeV/c for D0, 1 < pT< 36 GeV/c for D+ and D*+, and 2 < pT< 24 GeV/c for D+ mesons. For each species, the nuclear modification factor RpPb is calculated as a function of pT using a proton-proton (pp) reference measured at the same collision energy. The results are compatible with unity in the whole pT range…

High Energy Physics::ExperimenthiukkasfysiikkaNuclear Experimentheavy ion experiments
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Elliptic flow of electrons from heavy-flavour hadron decays at mid-rapidity in Pb-Pb collisions at √sNN =2.76 TeV

2016

The elliptic flow of electrons from heavy-flavour hadron decays at mid-rapidity (|y| < 0.7) is measured in Pb–Pb collisions at √ sNN = 2.76 TeV with ALICE at the LHC. The particle azimuthal distribution with respect to the reaction plane can be parametrized with a Fourier expansion, where the second coefficient (v2) represents the elliptic flow. The v2 coefficient of inclusive electrons is measured in three centrality classes (0–10%, 10–20% and 20–40%) with the event plane and the scalar product methods in the transverse momentum (pT) intervals 0.5–13 GeV/c and 0.5–8 GeV/c, respectively. After subtracting the background, mainly from photon conversions and Dalitz decays of neutral mesons, a …

High Energy Physics::PhenomenologyHigh Energy Physics::ExperimentNuclear Experimentheavy ion experiments
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Measurement of Ds+ production and nuclear modification factor in Pb-Pb collisions at √sNN = 2.76 TeV

2016

The production of prompt D+ s mesons was measured for the first time in collisions of heavy nuclei with the ALICE detector at the LHC. The analysis was performed on a data sample of Pb-Pb collisions at a centre-of-mass energy per nucleon pair, √ sNN, of 2.76 TeV in two different centrality classes, namely 0–10% and 20–50%. D+ s mesons and their antiparticles were reconstructed at mid-rapidity from their hadronic decay channel D+ s → φπ+, with φ → K−K+, in the transverse momentum intervals 4 < pT < 12 GeV/c and 6 < pT < 12 GeV/c for the 0–10% and 20–50% centrality classes, respectively. The nuclear modification factor RAA was computed by comparing the pT-differential production yields in Pb-…

High Energy Physics::PhenomenologyNuclear TheoryHigh Energy Physics::ExperimentNuclear Experimenthadron-hadron scatteringheavy ion experimentsquark gluon plasma
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Neutron skin and centrality classification in high-energy heavy-ion collisions at the LHC

2015

The concept of centrality in high-energy nuclear collisions has recently become a subject of an active debate. In particular, the experimental methods to determine the centrality that have given reasonable results for many observables in high-energy lead-lead collisions at the LHC have led to surprising behaviour in the case of proton-lead collisions. In this letter, we discuss the possibility to calibrate the experimental determination of centrality by asymmetries caused by mutually different spatial distributions of protons and neutrons inside the nuclei --- a well-known phenomenon in nuclear physics known as the neutron-skin effect.

High energyParticle physicsNuclear and High Energy PhysicsNuclear TheoryFLOWNuclear TheoryFOS: Physical sciences114 Physical sciencesHigh Energy Physics - ExperimentNuclear physicsNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)lead–lead collisionsDISTRIBUTIONSNeutronNuclear Experiment (nucl-ex)proton–lead collisionsNuclear ExperimentNuclear ExperimentPhysicsANISOTROPYLarge Hadron Colliderta114TRANSVERSE-MOMENTUMObservablecentralityneutron-skin effectlcsh:QC1-999High Energy Physics - PhenomenologyTransverse momentumTEVHeavy ionExperimental methodsCentralitylcsh:PhysicsPhysics Letters B
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Gluon correlations in the glasma

2010

The physics of the initial conditions of heavy ion collisions is dominated by the nonlinear gluonic interactions of QCD. These lead to the concepts of parton saturation and the Color Glass Condensate (CGC). We discuss recent progress in calculating multi-gluon correlations in this framework, prompted by the observation that these correlations are in fact easier to compute in a dense system (nucleus-nucleus) than a dilute one (proton-proton).

HistoryParticle physicsPhysics and Astronomy (miscellaneous)Nuclear TheoryHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesParton01 natural sciencesEducationColor-glass condensateNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNuclear Experiment010306 general physicsNuclear theoryQuantum chromodynamicsPhysicsta114010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyComputer Science ApplicationsGluonHigh Energy Physics - PhenomenologyNonlinear systemHigh Energy Physics::ExperimentHeavy ionSaturation (chemistry)Journal of Physics: Conference Series
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Recent results on heavy-ion induced reactions of interest for neutrinoless double beta decay at INFN-LNS

2019

Abstract The NUMEN project aims at accessing experimentally driven information on Nuclear Matrix Elements (NME) involved in the half-life of the neutrinoless double beta decay (0νββ). In this view measurements of Heavy Ion (HI) induced Double Charge Exchange (DCE) reaction cross sections are performed with high-accuracy. In particular, the (18O,18Ne) and (20Ne,20O) reactions are used as tools for β+β+ and β-β- decays, respectively. In the experiments, performed at INFN - Laboratory Nazionali del Sud (LNS) in Catania, the beams are accelerated by the Superconducting Cyclotron (CS) and the reaction ejectiles are detected the MAGNEX magnetic spectrometer. The measured cross sections are challe…

Historyexperimental methodsheavy ion: scatteringQC1-999heavy ion: charge exchange[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]hiukkasfysiikka7. Clean energy01 natural sciencesEducationNuclear physicsdouble-beta decay: (0neutrino)Double beta decay0103 physical sciencesneutrino: mass010306 general physicsnucleus: semileptonic decayPhysics010308 nuclear & particles physicsPhysicsparticle: MajoranaNuclear structurecross section: measuredSpecial classmagnetic spectrometercharge exchangedetector: upgradeneon: nuclideComputer Science Applicationsheavy ion induced double charge exchange reactionsneutrino: MajoranaHeavy ionenergy resolution: highydinfysiikkaCharge exchangeexperimental resultsEPJ Web of Conferences
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Recent results on Heavy-Ion induced reactions of interest for 0νββ decay

2019

An updated overview of recent results on Heavy-Ion induced reactions of interest for neutrinoless double beta decay is reported in the framework of the NUMEN project. The NUMEN idea is to study heavy-ion induced Double Charge Exchange (DCE) reactions with the aim to get information on the nuclear matrix elements for neutrinoless double beta (0νββ) decay. Moreover, to infer the neutrino average masses from the possible measurement of the half- life of 0νββ decay, the knowledge of the nuclear matrix elements is a crucial aspect. Uma visão geral atualizada dos resultados recentes sobre reações induzidas por íons pesados ​​de interesse para o decaimento beta duplo sem neutrinos é relatada na es…

Historymeasurement methodsnuclear matrix elements[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]heavy-ion induced Double Charge Exchange; nuclear matrix elements; neutrinoless double beta decay01 natural sciencesneutrinoless double beta decayEducationNuclear physicsoxygen: nuclidedouble-beta decay: (0neutrino)Double beta decay0103 physical sciencesBeta (velocity)neutrino: mass010306 general physicsNuclear ExperimentPhysicsnucleus: semileptonic decayMeasurement methodoperator: transition010308 nuclear & particles physicsHigh Energy Physics::Phenomenologyparticle: Majoranacharge exchangemagnetic spectrometerBeta decayheavy ionComputer Science Applicationsneon: nuclideheavy-ion induced Double Charge ExchangeHeavy ionHigh Energy Physics::ExperimentNeutrinoCharge exchange
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