Search results for "Quenching"

showing 10 items of 275 documents

The Influence of Flow on the Jet Quenching Power in Heavy-Ion Collisions

2005

The flow pattern and evolution of the medium created in ultrarelativistic heavy ion collisions can have significant influence on the energy loss of hard partons traversing the medium. We demonstrate that within a range of assumptions for longitudinal and transverse flow which are all compatible with the measured hadronic single particle distributions, the quenching power of the medium can vary within almost a factor five. Thus, the choice of the medium evolution is one of the biggest uncertainties in jet quenching calculations and needs to be addressed with some care.

PhysicsQuenchingNuclear and High Energy PhysicsRange (particle radiation)Particle physicsFlow (psychology)HadronFOS: Physical sciencesGeneral Physics and AstronomyPartonNuclear physicsHigh Energy Physics - PhenomenologyTransverse planeHigh Energy Physics - Phenomenology (hep-ph)ParticleNuclear ExperimentJet quenchingActa Physica Hungarica A) Heavy Ion Physics
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Measurements of inclusive jet spectra in pp and central Pb-Pb collisions at sNN=5.02TeV

2020

This article reports measurements of the pT- differential inclusive jet cross section in pp collisions at √s=5 .02TeV and the pT- differential inclusive jet yield in Pb-Pb 0–10% central collisions at√sNN =5.02TeV. Jets were reconstructed at midrapidity with the ALICE tracking detectors and electromagnetic calorimeter using the anti-kT algorithm. For ppcollisions, we report jet cross sections for jet resolution parameters R =0.1–0.6 over the range 20 < pT, jet < 140 GeV/c, as well as the jet cross-section ratios of different R and comparisons to two next-to-leading-order (NLO)– based theoretical predictions. For Pb-Pb collisions, we report the R=0.2 and R=0.4 jet spectra for 40 < pT, jet < 1…

PhysicsRange (particle radiation)Jet (fluid)Large Hadron Collider010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical Phenomena01 natural sciencesSpectral lineNuclear physicsElectromagnetic calorimeter0103 physical sciencesQuark–gluon plasmaHigh Energy Physics::ExperimentImpact parameterNuclear Experiment010306 general physicsJet quenchingPhysical Review C
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Transverse Momentum Distribution and Nuclear Modification Factor of Charged Particles inp+PbCollisions atsNN=5.02  TeV

2013

The transverse momentum (pT) distribution of primary charged particles is measured in minimum bias (non-single-diffractive) p + Pb collisions at root(NN)-N-s = 5.02 TeV with the ALICE detector at the LHC. The pT spectra measured near central rapidity in the range 0.5< p(T) < 20 GeV/c exhibit a weak pseudorapidity dependence. The nuclear modification factor R-pPb is consistent with unity for p(T) above 2 GeV/c. This measurement indicates that the strong suppression of hadron production at high p(T) observed in Pb + Pb collisions at the LHC is not due to an initial-state effect. The measurement is compared to theoretical calculations. DOI: 10.1103/PhysRevLett.110.082302

PhysicsRange (particle radiation)Large Hadron Collider010308 nuclear & particles physicsHadronGeneral Physics and Astronomy01 natural sciencesCharged particleSpectral lineNuclear physicsPseudorapidity0103 physical sciencesHigh Energy Physics::ExperimentRapidityNuclear Experiment010306 general physicsJet quenchingPhysical Review Letters
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Centrality dependence of the nuclear modification factor of charged pions, kaons, and protons in Pb-Pb collisions atsNN=2.76TeV

2016

Transverse momentum (pT) spectra of pions, kaons, and protons up to pT=20GeV/c have been measured in Pb-Pb collisions at √sNN=2.76TeV using the ALICE detector for six different centrality classes covering 0%–80%. The proton-to-pion and the kaon-to-pion ratios both show a distinct peak at pT≈3GeV/c in central Pb-Pb collisions that decreases for more peripheral collisions. For pT>10GeV/c, the nuclear modification factor is found to be the same for all three particle species in each centrality interval within systematic uncertainties of 10%–20%. This suggests there is no direct interplay between the energy loss in the medium and the particle species composition in the hard core of the quenched…

PhysicsSemileptonic decayParticle physics010308 nuclear & particles physicsNuclear TheoryHadron01 natural sciencesCharged particleParticle identificationBaryonNuclear physicsPion0103 physical sciencesQuark–gluon plasmaHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsJet quenchingPhysical Review C
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COHERENT constraints after the COHERENT-2020 quenching factor measurement

2020

Recently an improved quenching factor (QF) measurement for low-energy nuclear recoils in CsI[Na] has been reported by the COHERENT Collaboration. The new energy-dependent QF is characterized by a reduced systematic uncertainty and leads to a better agreement between the experimental COHERENT data and the Standard Model (SM) expectation. In this work, we report updated constraints on parameters that describe the process of coherent elastic neutrino-nucleus scattering within and beyond the SM, and we also present how the new QF affects their interpretation.

PhysicsSystematic errorQuenchingWork (thermodynamics)010308 nuclear & particles physicsScatteringFOS: Physical sciences01 natural sciencesInterpretation (model theory)Standard ModelComputational physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physics
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Impact of the quenching of gA on the sensitivity of 0νββ experiments

2017

Detection of the neutrinoless $\ensuremath{\beta}\ensuremath{\beta}$ ($0\ensuremath{\nu}\ensuremath{\beta}\ensuremath{\beta}$) decay is of high priority in the particle- and neutrino-physics communities. The detectability of this decay mode is strongly influenced by the value of the weak axial-vector coupling constant ${g}_{A}$. The recent nuclear-model analyses of $\ensuremath{\beta}$ and $\ensuremath{\beta}\ensuremath{\beta}$ decays suggest that the value of ${g}_{A}$ could be dramatically quenched, reaching ratios of ${g}_{A}^{\mathrm{free}}/{g}_{A}\ensuremath{\approx}4$, where ${g}_{A}^{\mathrm{free}}=1.27$ is the free, neutron-decay, value of ${g}_{A}$. The effects of this quenching ap…

PhysicsTurn (biochemistry)Coupling constantQuenching010308 nuclear & particles physicsFourth power0103 physical sciencesBeta (velocity)Sensitivity (control systems)Atomic physics010306 general physics01 natural sciencesNuclear theoryPhysical Review C
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Proton-neutron correlations and the longitudinal nuclear response

1988

We study the influence of the proton-neutron correlations, in particular of the tensor ones, on the longitudinal nuclear response. They generate a high-energy tail that we evaluate. We show that this tail produces an apparent quenching of the Coulomb sum rule. The amount of quenching found is significant, although insufficient to explain the totality of the missing strength.

Physics[PHYS]Physics [physics]Nuclear and High Energy PhysicsQuenching (fluorescence)Proton01 natural sciences010305 fluids & plasmasNuclear physics0103 physical sciencesCoulombNuclear fusionNeutronSum rule in quantum mechanicsTensor010306 general physicsNuclear Physics
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Theoretical study of energy transfer in Rb(7S) + Rb(5S) and Rb(5D) + Rb(5S) collisions

2000

We present results of theoretical studies of the non-resonant excitation transfer in Rb(7S) + Rb(5S) and Rb(5D) + Rb(5S) collisions at thermal collision energies. Rb2 adiabatic molecular terms correlating with the 5S+7S, 5S+5D and 5P+5P states of separated atoms were calculated for internuclear distances R > 20 a.u. using asymptotic approximation. Mechanisms of collisional population and quenching of the 5D state were treated on the basis of the computed molecular terms, and the respective cross-sections were calculated. Theoretical cross-sections are in good agreement with the experimental values at thermal collision energies (\(\) K).

Physicseducation.field_of_studyQuenching (fluorescence)PopulationOptical physicschemistry.chemical_elementPlasmaInelastic scatteringAtomic and Molecular Physics and OpticsRubidiumchemistryAtomic physicsAdiabatic processeducationExcitationThe European Physical Journal D
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Identification of disulphide bonds in the refolding of bovine pancreatic RNase A

1996

Background: Comprehension of the rules that govern the folding process is still far from satisfactory, though it is nevertheless clear that all the information required to define the folding is encoded in the amino acid sequence. In proteins that contain disulphide bonds, folding is associated with disulphide bond formation. Protein species with different numbers of disulphides tend to accumulate during the process; these species can be trapped in a stable form, by quenching any remaining free SH groups, and then characterized in order to identify the disulphide bonds formed. Results The refolding pathway of reduced and denatured RNase A has been studied using mass spectrometric strategies …

Protein FoldingSh groupsRNase P010402 general chemistryPeptide Mapping01 natural sciencesBiochemistryrefolding03 medical and health sciencesRNase AAnimalsDisulfidesES-MSPeptide sequencedisulphide bonds030304 developmental biology0303 health sciencesQuenching (fluorescence)ChemistryFAB-MSRibonuclease Pancreatic0104 chemical sciencesFolding (chemistry)CrystallographyMolecular MedicineCattlePancreatic RNaseDisulphide bondsCysteineFolding and Design
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Jet correlations: opportunities and pitfalls

2014

The simplest observables used to probe the interaction of hard partons with a QCD medium in ultrarelativistic heavy ion collisions measure disappearance, such as the nuclear modification factor R_AA. The information content of such observables is however limited. More differential information is obtained from triggered correlation observables where a trigger condition ensures that a hard event has taken place and the correlation of other objects in the event with the trigger contains information about the nature of parton-medium interaction. By construction, triggered correlation observables are conditional probabilities, i.e. they measure events biased by the trigger condition. The presenc…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsta114Conditional probabilityFOS: Physical sciencesPartonModification factorObservableHigh Energy Physics - PhenomenologyDifferential informationHigh Energy Physics - Phenomenology (hep-ph)Jet quenchingNuclear ExperimentPhenomenology (particle physics)Nuclear Physics A
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