Search results for "fluid"

showing 10 items of 5513 documents

Measurement of jet suppression in central Pb–Pb collisions at sNN=2.76 TeV

2015

The transverse momentum(p(T)) spectrum and nuclear modification factor (R-AA) of reconstructed jets in 0-10% and 10-30% central Pb-Pb collisions at root s(NN) = 2.76 TeV were measured. Jets were reconstructed using the anti-k(T) jet algorithm with a resolution parameter of R = 0.2 from charged and neutral particles, utilizing the ALICE tracking detectors and Electromagnetic Calorimeter (EMCal). The jet p(T) spectra are reported in the pseudorapidity interval of \eta(jet)\ 5 GeV/c to suppress jets constructed from the combinatorial background in Pb-Pb collisions. The leading charged particle requirement applied to jet spectra both in pp and Pb-Pb collisions had a negligible effect on the R-A…

PhysicsNuclear and High Energy PhysicsParticle physicsJet (fluid)Large Hadron ColliderAstrophysics::High Energy Astrophysical PhenomenaSpectral lineCharged particleNuclear physicsPseudorapidityHigh Energy Physics::ExperimentRapidityNuclear ExperimentJet quenchingNeutral particlePhysics Letters B
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Azimuthal decorrelations and multiple parton interactions inγ+2jet andγ+3jet events inpp¯collisions ats=1.96  TeV

2011

Samples of inclusive photon+2 jet and photon+3 jet events collected by the D0 experiment with an integrated luminosity of about 1fb^-1 in ppbar collisions at sqrt{s}=1.96 TeV are used to measure cross sections as a function of the angle in the plane transverse to the beam direction between the transverse momentum (pT) of the photon+leading jet system (jets are ordered in pT) and pT of the other jet for photon+2 jet, or pT sum of the two other jets for photon+3 jet events. The results are compared to different models of multiple parton interactions (MPI) in the PYTHIA and SHERPA Monte Carlo (MC) generators. The data indicate a contribution from events with double parton (DP) interactions and…

PhysicsNuclear and High Energy PhysicsParticle physicsJet (fluid)Luminosity (scattering theory)Photon010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaMonte Carlo methodPartonHERA7. Clean energy01 natural scienceslaw.inventionNuclear physicsTransverse planelaw0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsColliderPhysical Review D
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Double parton interactions inγ+3jet andγ+b/cjet+2jet events inpp¯collisions ats=1.96 TeV

2014

We determine the fraction of events with double parton (DP) Scattering in a single p (p) over bar collisions at root s = 1.96 TeV in gamma + 3 jet and gamma + b/c jet + 2 jet events collected with the D0 detector and corresponding to an integrated luminosity of about 8.7 fb(-1). The DP fractions and effective cross sections (sigma(eff)) are measured for both event samples using the same kinematic selections. The measured DP fractions range from 0.21 to 0.17, with effective cross sections in the gamma + 3 jet and gamma + b/cjet + 2 jet samples of sigma(incl)(eff) = 12.7 +/- 0.2(stat) +/- 1.3(syst) mb and sigma(HF)(eff) = 14.6 +/- 0.6(stat) +/- 3.2(syst) mb, respectively.

PhysicsNuclear and High Energy PhysicsParticle physicsJet (fluid)Luminosity (scattering theory)PhotonScatteringAstrophysics::High Energy Astrophysical PhenomenaSigmaPartonNuclear physicsHigh Energy Physics::ExperimentNuclear ExperimentBar (unit)Physical Review D
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Neutrino masses and mixing: 2008 status

2009

We review the current status (as of the end of 2008) of neutrino mass and mixing determinations, focusing on the hints of θ 13 > 0 , recently emerged in our global analysis.

PhysicsNuclear and High Energy PhysicsParticle physicsSolar neutrinoMeasurements of neutrino speedCurrent (fluid)Solar neutrino problemNeutrinoNeutrino oscillationAtomic and Molecular Physics and OpticsMixing (physics)Nuclear Physics B - Proceedings Supplements
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Entropy development in ideal relativistic fluid dynamics with the Bag Model equation of state

2010

We consider an idealized situation where the Quark-Gluon Plasma (QGP) is described by a perfect, (3 + 1)-dimensional fluid dynamic model starting from an initial state and expanding until a final state where freeze-out and/or hadronization takes place. We study the entropy production with attention to effects of (i) numerical viscosity, (ii) late stages of flow where the Bag Constant and the partonic pressure are becoming similar, (iii) and the consequences of final freeze-out and constituent quark matter formation.

PhysicsNuclear and High Energy PhysicsPhase transitionNuclear TheoryEntropy productionHigh Energy Physics::PhenomenologyNuclear TheoryFOS: Physical sciencesConstituent quarkHadronizationNuclear Theory (nucl-th)Strange matterQuantum electrodynamicsQuark–gluon plasmaFluid dynamicsHigh Energy Physics::ExperimentNuclear ExperimentEntropy (arrow of time)Mathematical physics
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Zeroing in on the initial state — tomography using bulk, jets and photons

2014

One of the unsolved problems in the current 'standard model' of heavy ion physics is the apparent rapid thermalization of QCD matter in the pre-equilibrium stage. While it is challenging to probe this mechanism directly, there are now several observables available which allow tomographic imaging of the initial state geometry, which is expected to carry remnant information of the equilibration mechanism. On the fluid dynamics side, scaled fluctuations in the momentum space anisotropy parameters v_n image the initial eccentricity fluctuations epsilon_n almost directly with only a weak dependence on the details of the fluid dynamical evolution. From a different direction, due to the strong non…

PhysicsNuclear and High Energy PhysicsPhotonta114Nuclear TheoryFOS: Physical sciencesObservablePosition and momentum spaceComputational physicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)ThermalisationQuantum mechanicsQuark–gluon plasmaFluid dynamicsJet quenchingQCD matterNuclear Physics A
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Isothermal flow of helium II through plane slits

1972

Measurements are reported on the isothermal, gravitational flow of liquid He II through narrow plane slits. The employed superleak consists of ring-shaped Hostaphan foils packed in layers. The distance between the foils is varied by pressure. The performance of the measurements and the observance of the isothermal conditions are described. The velocity of the superfluid component of He II is calculated in dependence on the width of the slits, the temperature and the hydrostatic pressure. Especially the critical velocity is considered.

PhysicsNuclear and High Energy PhysicsPlane (geometry)business.industryHydrostatic pressureIsothermal flowchemistry.chemical_elementMechanicsCritical ionization velocityIsothermal processSuperfluidityOpticschemistryFluid dynamicsbusinessHeliumZeitschrift für Physik A Hadrons and nuclei
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Superfluid properties of the inner crust of neutron stars

2011

We investigated the superfluid properties of the inner crust of neutron stars, solving the Hartree-Fock-Bogoliubov equations in spherical Wigner-Seitz cells. Using realistic two-body interactions in the pairing channel, we studied in detail the Cooper-pair and the pairing-field spatial properties, together with the effect of the proton clusters on the neutron pairing gap. Calculations with effective pairing interactions are also presented, showing significant discrepancies with the results obtained with realistic pairing forces. At variance with recent studies on finite nuclei, the neutron coherence length is found to depend on the strength of the pairing interaction, even inside the nucleu…

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsNuclear Theory01 natural sciencesCoherence lengthBaryonSuperfluidityNeutron starPairing0103 physical sciencesNuclear forceNeutronAtomic physics010306 general physicsPhysical Review C
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Focusing ions by viscous drag and weak electric fields in an ion guide

1991

Abstract A new special ion guide has one or more grids at low electric potential in the space between nozzle and skimmer. Viscous drag caused by helium flow is used together with weak electric fields for focusing ions through the skimmer. A typical yield through the skimmer is 75% of that through the nozzle. The focusing device is called a “squeezer”. Most properties of the “squeezer ion guide” are similar to those of an ordinary ion guide. Because the kinetic energies are only of the order of 10 eV, however, problems caused by ion scattering are greatly reduced as compared to ordinary ion guides.

PhysicsNuclear and High Energy PhysicsScatteringNozzlechemistry.chemical_elementIonPhysics::Fluid DynamicschemistryPhysics::Plasma PhysicsDragElectric fieldSkimmer (machine)Electric potentialAtomic physicsInstrumentationHeliumNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Wavelet analysis of experimental results for coupled structural–hydraulic behavior of the EURISOL target mock-up

2009

During test runs of the The European Isotope Separation On-Line (EURISOL) target mock-up performed in December 2008, data were recorded for strain gages and for acceleration sensors. In this paper, the applicability of wavelet analysis for detecting the onset and the status of flow-induced cavitation is investigated for the first time. Even under noisy conditions, the detection of incipient cavitation was possible when combining measurements with data from structural and fluid dynamic simulations. The distribution of coefficients of suitably selected wavelets yields a quantitative measure for the extent of cavitation in the EURISOL target mock-up under representative flow conditions. Withou…

PhysicsNuclear and High Energy PhysicsUniform distribution (continuous)business.industryGaussianProbability density functionMechanicsComputational fluid dynamicsStandard deviationsymbols.namesakeAccelerationWaveletCavitationsymbolsbusinessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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