Search results for "Heavy-ion"

showing 10 items of 119 documents

Centrality dependence of multiplicity, transverse energy, and elliptic flow from hydrodynamics

2001

The centrality dependence of the charged multiplicity, transverse energy, and elliptic flow coefficient is studied in a hydrodynamic model, using a variety of different initializations which model the initial energy or entropy production process as a hard or soft process, respectively. While the charged multiplicity depends strongly on the chosen initialization, the p_t-integrated elliptic flow for charged particles as a function of charged particle multiplicity and the p_t-differential elliptic flow for charged particles in minimum bias events turn out to be almost independent of the initial energy density profile.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryEntropy productionPhysicsElliptic flowFOS: Physical sciencesInitializationRelativistic heavy-ion collisions Elliptic flow Hydrodynamic modelCharged particleNuclear Theory (nucl-th)High Energy Physics - PhenomenologyTransverse planeHigh Energy Physics - Phenomenology (hep-ph)Quantum electrodynamicsEnergy densityMultiplicity (chemistry)Centrality
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The 48Ca+181Ta reaction: Cross section studies and investigation of neutron-deficient 86 ≤ Z ≤ 93 isotopes

2019

© 2019 Fusion-evaporation reactions with the doubly magic projectile 48 Ca were used to access neutron-deficient nuclei around neptunium at the velocity filter SHIP, and investigated using the COMPASS decay spectroscopy station. With the use of digital electronics, several isotopes produced via neutron, proton, and α evaporation channels were identified by establishing correlated α-decay chains with short-lived sub-μs members. Data are given on decay chains stemming from 225,226 Np, 225 U, and 222,223 Pa. New information on the isotopes 225,226 Np and 222 Pa was obtained. Production cross sections of nuclei in the region using a variety of projectiles are discussed. The measured production …

PhysicsNuclear and High Energy PhysicsProtonIsotope010308 nuclear & particles physicsProjectileNeptuniumNuclear Theorychemistry.chemical_elementDigital electronics for nuclear spectroscopy[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesNuclear physicschemistry0103 physical sciencesAlpha decayNeutronAlpha decayDecay chainHeavy-ion induced fusionNuclear Experiment010306 general physicsSpectroscopyNuclear Physics A
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The large-area micro-channel plate entrance detector of the heavy-ion magnetic spectrometer PRISMA

2005

This paper describes the entrance detector of the magnetic spectrometer PRISMA recently installed at Legnaro. The detector is based on rectangular (80 x 100 mm(2)) Micro-Channel Plates (MCP). It provides a fast time signal and its position-sensitive anode allows to extract the X and Y information. It exploits an electrostatic field for the acceleration of secondary electrons from a thin Carbon foil (similar or equal to 20 mu g/cm(2)) onto the MCP assembly. The electrons are guided by a parallel magnetic field. Good performances were obtained in the laboratory tests. The detector is presently installed at the entrance of PRISMA and gives resolutions <= 400 ps in time, and 1 mm in both X and …

PhysicsNuclear and High Energy PhysicsSpectrometerbusiness.industryDetectordetectors for heavy ions ; micro-channel plates ; magnetic spectrometers ; low-energy heavy-ion reactionsParticle detectorSecondary electronsCharged particleMagnetic fieldNuclear physicsOpticsElectric fieldMicrochannel plate detectorbusinessInstrumentation
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Carbon fragmentation measurements and validation of the GEANT4 nuclear reaction models for hadrontherapy

2012

Nuclear fragmentation measurements are necessary when using heavy-ion beams in hadrontherapy to predict the effects of the ion nuclear interactions within the human body. Moreover, they are also fundamental to validate and improve the Monte Carlo codes for their use in planning tumor treatments. Nowadays, a very limited set of carbon fragmentation cross sections are being measured, and in particular, to our knowledge, no double-differential fragmentation cross sections at intermediate energies are available in the literature. In this work, we have measured the double-differential cross sections and the angular distributions of the secondary fragments produced in the (12)C fragmentation at 6…

PhysicsNuclear reactionRadiological and Ultrasound TechnologyHEAVY-ION REACTIONS; BEAM TRANSPORT; THERAPY;Monte Carlo methodBinary numberHeavy Ion RadiotherapyTHERAPYCarbonSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)IonNuclear physicsMolecular dynamicsFragmentation (mass spectrometry)CascadeHEAVY-ION REACTIONSHumansRadiology Nuclear Medicine and imagingNuclear ExperimentQuantumMonte Carlo MethodBEAM TRANSPORT
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Evolution of initial stage fluctuations in the glasma

2021

We perform a calculation of the one- and two-point correlation functions of energy density and axial charge deposited in the glasma in the initial stage of a heavy ion collision at finite proper time. We do this by describing the initial stage of heavy ion collisions in terms of freely evolving classical fields whose dynamics obey the linearized Yang-Mills equations. Our approach allows us to systematically resum the contributions of high momentum modes that would make a power series expansion in proper time divergent. We evaluate the field correlators in the McLerran-Venugopalan model using the glasma graph approximation, but our approach for the time dependence can be applied to a general…

PhysicsPower seriesquark-gluon plasmaField (physics)Nuclear Theory010308 nuclear & particles physicskvarkki-gluoniplasmaPhase (waves)FOS: Physical sciencesCharge (physics)Function (mathematics)Collision01 natural sciences114 Physical sciencesNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)nuclear physics0103 physical sciencesGraph (abstract data type)Proper timeStatistical physicsydinfysiikka010306 general physicsrelativistic heavy-ion collisions
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Search for elements 119 and 120

2020

A search for production of the superheavy elements with atomic numbers 119 and 120 was performed in the 50Ti+249Bk and 50Ti+249Cf fusion-evaporation reactions, respectively, at the gas-filled recoil separator TASCA at GSI Darmstadt, Germany. Over four months of irradiation, the 249Bk target partially decayed into 249Cf, which allowed for a simultaneous search for both elements. Neither was detected at cross-section sensitivity levels of 65 and 200 fb for the 50Ti+249Bk and 50Ti+249Cf reactions, respectively, at a midtarget beam energy of Elab=281.5 MeV. The nonobservation of elements 119 and 120 is discussed within the concept of fusion-evaporation reactions including various theoretical pr…

Physicselement 119010308 nuclear & particles physicselement 120Superheavy Elements01 natural sciencesIsland of stabilityRecoil separatorNuclear physicssuperheavy elementsProduction cross sectionSubatomic Physics0103 physical sciences540 Chemistry570 Life sciences; biologylow and intermediate energy heavy-ion reactionsAtomic numberIrradiationSensitivity (control systems)ydinfysiikka010306 general physicsBeam energyPhysical Review C
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Use of a running coupling in the NLO calculation of forward hadron production

2018

We address and solve a puzzle raised by a recent calculation [1] of the cross-section for particle production in proton-nucleus collisions to next-to-leading order: the numerical results show an un- reasonably large dependence upon the choice of a prescription for the QCD running coupling, which spoils the predictive power of the calculation. Specifically, the results obtained with a prescription formulated in the transverse coordinate space differ by one to two orders of magnitude from those obtained with a prescription in momentum space. We show that this discrepancy is an artefact of the interplay between the asymptotic freedom of QCD and the Fourier transform from coordinate space to mo…

Position and momentum spaceQCD EVOLUTION01 natural sciencesAsymptotic freedomquantum chromodynamics: correctionhard scatteringHigh Energy Physics - Phenomenology (hep-ph)coupling constant: energy dependencestrong interaction: coupling constantEQUATIONkvanttifysiikkaComputingMilieux_MISCELLANEOUSPhysicsQuantum chromodynamicsQUARKhigher-order: 1nuclear physicssddc:12.39.StHigh Energy Physics - Phenomenology12.38.Bxsymbolsydinfysiikkahadron: forward productionFOS: Physical sciences114 Physical sciencesRENORMALIZATION-GROUP12.38.Cysymbols.namesakeCross section (physics)Theoretical physicsquantum chromodynamics0103 physical sciencessirontarelativistic heavy-ion collisionCoordinate spacenumerical calculations010306 general physicsp nucleus: scatteringcorrection: higher-orderCouplingta114010308 nuclear & particles physics25.75.-qCOLOR GLASS CONDENSATENONLINEAR GLUON EVOLUTIONRenormalization groupFourier transformasymptotic freedom[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph][ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Physical Review D
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Measurement of visible cross sections in proton-lead collisions at √sNN= 5.02 TeV in van der Meer scans with the ALICE detector

2014

In 2013, the Large Hadron Collider provided proton-lead and lead-proton collisions at the center-of-mass energy per nucleon pair $\sqrt{s_{\rm{NN}}}=5.02$ TeV. Van der Meer scans were performed for both configurations of colliding beams, and the cross section was measured for two reference processes, based on particle detection by the T0 and V0 detectors, with pseudo-rapidity coverage $4.6<\eta< 4.9$, $-3.3<\eta<-3.0$ and $2.8<\eta< 5.1$, $-3.7<\eta<-1.7$, respectively. Given the asymmetric detector acceptance, the cross section was measured separately for the two configurations. The measured visible cross sections are used to calculate the integrated luminosity of the proton-lead and lead-…

ProtonNuclear Theorylarge detector systems for particle and astroparticle physicsLarge detector systems for particle and astroparticle physics; Particle tracking detec- tors; Heavy-ion detectors01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Particle tracking detectorsparticle tracking detectors[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Neutron detectionNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentInstrumentationMathematical PhysicsPhysicsLarge Hadron ColliderLuminosity (scattering theory)PhysicsDetectorLuminosity measurement3. Good healthPRIRODNE ZNANOSTI. Fizika.Large detector systems for particle and astroparticle physics Particle tracking detec- torNucleonParticle Physics - ExperimentLarge detector systems for particle and astroparticle physics ; Particle tracking detectors ; Heavy-ion detectorsParticle physicsParticle tracking detec- torsInstrumentationHeavy-ion detectorsFOS: Physical sciencesLarge detector systems for particle and astroparticle physics; Particle tracking detectors; Heavy-ion detectors[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear physicsCross section (physics)p-Pb collisions at the LHC0103 physical sciencesNuclear Physics - Experiment010306 general physics010308 nuclear & particles physicsLarge detector systems for particle and astroparticle physicsALICE experimentLarge detector systems for particle and astroparticle physics Particle tracking detec- tors; Heavy-ion detectorsNATURAL SCIENCES. Physics.heavy-ion detectorsInstrumentation; Mathematical PhysicsPhysics::Accelerator PhysicsHigh Energy Physics::Experiment
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D mesic nuclei

2010

The energies and widths of several D-0 meson bound states for different nuclei are obtained using a D-meson selfenergy in the nuclear medium, which is evaluated in a selfconsistent manner using techniques of unitarized coupled-channel theory. The kernel of the meson-baryon interaction is based on a model that treats heavy pseudoscalar and heavy vector mesons on equal footing, as required by heavy quark symmetry. We find D-0 bound states in all studied nuclei, from C-12 up to Pb-208. The inclusion of vector mesons is the keystone for obtaining an attractive D-nucleus interaction that leads to the existence of D-0-nucleus bound states, as compared to previous studies based on SU(4) flavor sym…

QuarkNuclear reactionNuclear and High Energy PhysicsParticle physicsCharmNuclear TheoryMesonHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesHEAVY-ION COLLISIONS01 natural sciences7. Clean energyBOUND-STATESHigh Energy Physics - ExperimentNuclear Theory (nucl-th)Nuclear physicsENERGYHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)ANTIPROTON ANNIHILATION0103 physical sciencesBound stateHeavy quark effective theorySCATTERINGNuclear Experiment (nucl-ex)Basso continuoNuclear Experiment010306 general physicsNuclear ExperimentSUPPRESSIONPhysicsPIONIC ATOMS010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyFísicaCHIRAL DYNAMICSHeavy quark symmetryETAPseudoscalarHigh Energy Physics - PhenomenologyMesic nucleiPhysics Letters B
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Predictions for multiplicities and flow harmonics in 5.44 TeV Xe+Xe collisions at the CERN Large Hadron Collider

2018

We present the next-to-leading-order event-by-event EKRT model predictions for the centrality dependence of the charged hadron multiplicity in the pseudorapidity interval $|\eta|\le 0.5$, and for the centrality dependence of the charged hadron flow harmonics $v_n\{2\}$ obtained from 2-particle cumulants, in $\sqrt{s_{NN}}=5.44$ TeV Xe+Xe collisions at the CERN Large Hadron Collider. Our prediction for the 0-5 \% central charged multiplicity is $dN_{\rm ch}/d\eta =1218\pm 46$. We also predict $v_n\{2\}$ in Xe+Xe collisions to increase more slowly from central towards peripheral collisions than those in a Pb+Pb system. We find that at $10 \dots 50$\% centralities $v_2\{2\}$ is smaller and $v_…

QuarkParticle physicsNuclear TheoryHadronFOS: Physical scienceshiukkasfysiikka01 natural sciences114 Physical sciencesNuclear physicsENERGYNuclear Theory (nucl-th)GLUON DISTRIBUTION-FUNCTIONSHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBAYESIAN-ANALYSISRapidityNUCLEAR COLLISIONS010306 general physicsNuclear ExperimentPhysicscollective flowta114010308 nuclear & particles physicsparticle and resonance productionHigh Energy Physics::PhenomenologyHIGH-DENSITY QCDQUARKMultiplicity (mathematics)Nuclear matterHigh Energy Physics - PhenomenologyPseudorapidityHigh Energy Physics::ExperimentImpact parameterhydrodynamic modelsCentralityrelativistic heavy-ion collisions
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