Search results for "transverse-momentum"

showing 10 items of 19 documents

Charged jet cross section and fragmentation in proton-proton collisions at √s = 7 TeV

2019

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI. We report the differential charged jet cross section and jet fragmentation distributions measured with the ALICE detector in proton-proton collisions at a center-of-mass energy √s=7  TeV. Jets with pseudorapidity |η|40  GeV/c, the pythia calculations also agree with the measured charged jet cross section. pythia6 simulations describe the fragmentation distributions to 15%. Larger discrepancies are observed for pythia8. SCOAP

:Kjerne- og elementærpartikkelfysikk: 431 [VDP]Physics and Astronomy (miscellaneous)fragmentation [jet]Astrophysics::High Energy Astrophysical Phenomenameasured [cross section]transverse momentumhiukkasfysiikka01 natural sciencesscattering [pp]Nuclear physicsALICEFragmentation (mass spectrometry)0103 physical sciencesjet fragmentation010306 general physicsNuclear ExperimentPhysicsQuantum chromodynamicsPP COLLISIONSta114010308 nuclear & particles physicsPB COLLISIONS:Matematikk og naturvitenskap: 400::Fysikk: 430::Kjerne- og elementærpartikkelfysikk: 431 [VDP]TRANSVERSE-MOMENTUMVDP::Kjerne- og elementærpartikkelfysikk: 431resolution16. Peace & justicecharged particlejet cross sectionCharged particleNATURAL SCIENCES. Physics.ddc::Mathematics and natural scienses: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP]PRIRODNE ZNANOSTI. Fizika.:Nuclear and elementary particle physics: 431 [VDP]pp: scattering ; jet: fragmentation ; cross section: measured ; transverse momentum ; charged particle ; resolution ; PYTHIA ; ALICEVDP::Nuclear and elementary particle physics: 431PseudorapidityTransverse momentumPYTHIAHigh Energy Physics::Experimentproton-proton collisionsTRANSVERSE-MOMENTUM; PP COLLISIONS; PB COLLISIONS; PARTICLEPARTICLEPhysical Review D
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Charged-particle multiplicities in pp interactions measured with the ATLAS detector at the LHC

2011

Measurements are presented from proton–proton collisions at centre-of-mass energies of \sqrt{s} = 0.9 , 2.36 and 7 TeV recorded with the ATLAS detector at the LHC. Events were collected using a single-arm minimum-bias trigger. The charged-particle multiplicity, its dependence on transverse momentum and pseudorapidity and the relationship between the mean transverse momentum and charged-particle multiplicity are measured. Measurements in different regions of phase space are shown, providing diffraction-reduced measurements as well as more inclusive ones. The observed distributions are corrected to well-defined phase-space regions, using model-independent corrections. The results are compared…

Atlas detectorMonte Carlo methodLarge hadron colliderNuclear physicsGeneral Physics and Astronomy01 natural sciencesTransverse-Momentum SpectraHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Pseudorapidity[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]CollisionsQANuclear ExperimentTransverse momentumQCPhysicsLarge Hadron ColliderPhysicsSettore FIS/01 - Fisica SperimentaleParticle physicsATLAS detector; LHC; pp collisionsATLASSquare-Root-SMonte carlo methodCharged particle3. Good healthPseudorapidityddc:540ComputingMethodologies_DOCUMENTANDTEXTPROCESSINGTsallis distributionFísica nuclearDistributionsLHCpp collisionsParticle Physics - ExperimentParticle physicsCiências Naturais::Ciências FísicasAtlas detector:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesCharged particleInclusive production with identified hadronsPhase spaceddc:500.2530Nuclear physics0103 physical sciencesddc:530High Energy Physics010306 general physicsATLAS detector010308 nuclear & particles physicsFísicaMultiplicity (mathematics)Perturbative calculationsMultiplicity (mathematics)pp interactions; LHC; ATLAS detectorPhase spaceHADRON-HADRON COLLISIONSExperimental High Energy PhysicsCM EnergiesTevHigh Energy Physics::ExperimentCollider
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Production of Λ and KS0 in jets in p–Pb collisions at √sNN = 5.02 TeV and pp collisions at √s = 7 TeV

2022

The production of Λ baryons and KS0 mesons (V0 particles) was measured in p–Pb collisions at √sNN=5.02 TeV and pp collisions at √s=7 TeV with ALICE at the LHC. The production of these strange particles is studied separately for particles associated with hard scatterings and the underlying event to shed light on the baryon-to-meson ratio enhancement observed at intermediate transverse momentum (pT) in high multiplicity pp and p–Pb collisions. Hard scatterings are selected on an event-by-event basis with jets reconstructed with the anti-kT algorithm using charged particles. The production of strange particles associated with jets pT,jetch>10 and pT,jetch>20 GeV/c in p–Pb collisions, and with …

Charged-particle productionNuclear and High Energy PhysicsLong-rangeAstrophysics::High Energy Astrophysical Phenomenakvarkki-gluoniplasmahiukkasfysiikkaProton-proton collisionsTransverse-momentum dependenceMultiplicity2-particle correlationsRange angular-correlationsAzimuthal correlationsSideHigh Energy Physics::ExperimentNuclear modificationNuclear Experiment
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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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Hot spots and gluon field fluctuations as causes of eccentricity in small systems

2021

We calculate eccentricities in high energy proton-nucleus collisions, by calculating correlation functions of the energy density field of the Glasma immediately after the collision event at proper time tau = 0. We separately consider the effects of color charge and geometrical hot spot fluctuations, analytically performing the averages over both in a dilute-dense limit. We show that geometric fluctuations of hot spots inside the proton are the dominant source of eccentricity whereas color charge fluctuations only give a negligible correction. The size and number of hot spots are the most important parameters characterizing the eccentricities.

Nuclear TheoryField (physics)ProtonAZIMUTHAL ANISOTROPIESFLOWmedia_common.quotation_subjectFOS: Physical sciencesHot spot (veterinary medicine)hiukkasfysiikka114 Physical sciences01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesProper timeEccentricity (behavior)LONG-RANGEHARMONICSNuclear Experiment010306 general physicsPLUS PB COLLISIONSGluon fieldmedia_commonPROTON-LEAD COLLISIONSPhysics010308 nuclear & particles physicskvarkki-gluoniplasmaANGULAR-CORRELATIONSComputational physicsHigh Energy Physics - PhenomenologyNEAR-SIDEAstrophysics::Earth and Planetary AstrophysicsHIGH TRANSVERSE-MOMENTUMPPBEvent (particle physics)Color chargePhysical Review D
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Tracing the origin of azimuthal gluon correlations in the color glass condensate

2016

We examine the origins of azimuthal correlations observed in high energy proton-nucleus collisions by considering the simple example of the scattering of uncorrelated partons off color fields in a large nucleus. We demonstrate how the physics of fluctuating color fields in the color glass condensate (CGC) effective theory generates these azimuthal multiparticle correlations and compute the corresponding Fourier coefficients v_n within different CGC approximation schemes. We discuss in detail the qualitative and quantitative differences between the different schemes. We will show how a recently introduced color field domain model that captures key features of the observed azimuthal correlati…

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryField (physics)LARGE NUCLEIFOS: Physical sciencesParton01 natural sciencesFLUX TUBES114 Physical sciencesColor-glass condensateNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)DEPENDENCE0103 physical sciencesEffective field theorySCATTERINGStatistical physicsLIGHT ION COLLISIONSheavy ion phenomenology010306 general physicsNuclear ExperimentFourier seriesPhysicsta114010308 nuclear & particles physicsScatteringPB COLLISIONSQUARKTRANSVERSE-MOMENTUMENERGY PA-COLLISIONSQCD phenomenologyEVOLUTION3. Good healthGluonAzimuthHigh Energy Physics - PhenomenologyJournal of High Energy Physics
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Azimuthal harmonics of color fields in a high energy nucleus

2015

Recent experimental results have revealed a surprisingly rich structure of multiparticle azimuthal correlations in high energy proton-nucleus collisions. Final state collective effects can be responsible for many of the observed effects, but it has recently been argued that a part of these correlations are present already in the wavefunctions of the colliding particles. We evaluate the momentum space 2-particle cumulant azimuthal anisotropy coefficients v_n{2}, n=2,3,4 from fundamental representation Wilson line distributions describing the high energy nucleus. These would correspond to the flow coefficients in very forward proton nucleus scattering. We find significant differences beteen W…

Nuclear and High Energy PhysicsWilson loopNuclear TheoryGLASMA FLUX TUBESFOS: Physical sciencesPosition and momentum space114 Physical sciences01 natural sciencesColor-glass condensateNuclear Theory (nucl-th)GLUON DISTRIBUTION-FUNCTIONSHigh Energy Physics - Phenomenology (hep-ph)CONDENSATE0103 physical sciencesSIDEproton-nucleus collisionsMultiplicity (chemistry)LONG-RANGE010306 general physicsAnisotropyWave functionNuclear ExperimentPhysicsta114010308 nuclear & particles physicsScatteringPB COLLISIONSTRANSVERSE-MOMENTUMMULTIPLICITYPPB COLLISIONSANGULAR-CORRELATIONSlcsh:QC1-999High Energy Physics - PhenomenologyQuantum electrodynamicsmultiparticle azimuthal correlationsColor chargelcsh:PhysicsPhysics Letters B
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Jet quenching as a probe of the initial stages in heavy-ion collisions

2019

Jet quenching provides a very flexible variety of observables which are sensitive to different energy- and time-scales of the strongly interacting matter created in heavy-ion collisions. Exploiting this versatility would make jet quenching an excellent chronometer of the yoctosecond structure of the evolution process. Here we show, for the first time, that a combination of jet quenching observables is sensitive to the initial stages of heavy-ion collisions, when the approach to local thermal equilibrium is expected to happen. Specifically, we find that in order to reproduce at the same time the inclusive particle production suppression, $R_{AA}$, and the high-$p_T$ azimuthal asymmetries, $v…

PB-PB COLLISIONSNuclear and High Energy Physicsnucl-thNuclear TheoryFLOWInitial stagesFlow (psychology)PREDICTIONSFOS: Physical scienceshiukkasfysiikkanucl-ex114 Physical sciences01 natural sciencesENERGYNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Phenomenology (hep-ph)heavy-ionsTRANSVERSE-MOMENTUM DEPENDENCE0103 physical sciencesNuclear Physics - ExperimentROOT-S(NN)=2.76 TEVNuclear Experiment (nucl-ex)010306 general physicsJet quenchingNuclear ExperimentNuclear ExperimentParticle Physics - PhenomenologyHeavy-ionsPhysicsThermal equilibriumJet (fluid)ionit010308 nuclear & particles physicsElliptic flowLEAD COLLISIONShep-phObservablelcsh:QC1-999initial stagesJet quenchingjet quenchingHigh Energy Physics - PhenomenologyNuclear Physics - TheoryParticleHeavy ionlcsh:PhysicsPhysics Letters B
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Initial conditions in AA and pA collisions

2016

A full understanding of the spacetime evolution of the QCD matter created in a heavy ion collision requires understanding the properties of the initial stages. In the weak coupling picture these are dominated by classical gluon fields, whose properties can also be studied via the scattering of dilute probes off a high energy hadron or nucleus. A particular challenge is understanding small systems, where LHC data is also showing signs of collective behavior. We discuss some recent results of on the initial matter production and thermalization in heavy ion collisions, in particular in the gluon saturation framework.

Particle physicsCollective behaviorNuclear TheoryQC1-999HadronFOS: Physical sciencesGLUON PRODUCTION114 Physical sciences01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)quantum chromodynamics0103 physical sciencesNuclear Experiment010306 general physicsPLUS PB COLLISIONSNUCLEUSQCD matterPhysicsgluon fieldsLarge Hadron Colliderta114010308 nuclear & particles physicsScatteringPhysicsCGC PREDICTIONSHigh Energy Physics::PhenomenologyTRANSVERSE-MOMENTUMCOLOR GLASS CONDENSATEFIELDSEVOLUTIONGluonheavy ion collisionHigh Energy Physics - PhenomenologyCoupling (physics)ThermalisationLHCgluon saturationEPJ Web of Conferences
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Confronting current NLO parton fragmentation functions with inclusive charged-particle spectra at hadron colliders

2013

The inclusive spectra of charged particles measured at high transverse momenta ($p_T\gtrsim$2GeV/c) in proton-proton and proton-antiproton collisions in the range of center-of-mass energies $\sqrt{s}=200-7000$GeV are compared with next-to-leading order perturbative QCD calculations using seven recent sets of parton-to-hadron fragmentation functions (FFs). Accounting for the uncertainties in the scale choices and in the parton distribution functions, we find that most of the theoretical predictions tend to overpredict the measured LHC and Tevatron cross sections by up to a factor of two. We identify the currently too-hard gluon-to-hadron FFs as the probable source of the problem, and justify…

Particle physicsNuclear and High Energy PhysicsNuclear TheoryHadroneducationTevatronFOS: Physical sciencesPartonPROTON114 Physical sciencesSpectral lineHigh Energy Physics - ExperimentNuclear physicsNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)DISTRIBUTIONSSCATTERINGQCD ANALYSISNuclear ExperimentParticle Physics - PhenomenologySUPPRESSIONPhysicsLarge Hadron ColliderPP COLLISIONSROOT-S=7 TEVta114High Energy Physics::PhenomenologyPerturbative QCDCharged particleEVOLUTIONHigh Energy Physics - PhenomenologyDistribution functionHigh Energy Physics::ExperimentTRANSVERSE-MOMENTUM SPECTRATO-LEADING ORDERNuclear Physics B
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