0000000000756310

AUTHOR

Lu X. G.

showing 3 related works from this author

Freeze-out radii extracted from three-pion cumulants in pp, p–Pb and Pb–Pb collisions at the LHC

2014

In high-energy collisions, the spatio-temporal size of the particle production region can be measured using the Bose-Einstein correlations of identical bosons at low relative momentum. The source radii are typically extracted using two-pion correlations, and characterize the system at the last stage of interaction, called kinetic freeze-out. In low-multiplicity collisions, unlike in high-multiplicity collisions, two-pion correlations are substantially altered by background correlations, e.g. mini-jets. Such correlations can be suppressed using three-pion cumulant correlations. We present the first measurements of the size of the system at freeze-out extracted from three-pion cumulant correl…

kinetic freezout heavy-ion experiments particle cummulantsMULTIPLICITY DEPENDENCEfreeze-out radius; three-pion cumulants; pp; p–Pb and Pb–Pb collisionsPb-Pb and p-Pb collisions at the LHCpp01 natural sciencesHigh Energy Physics - Experimentlaw.inventionColor-glass condensateHigh Energy Physics - Experiment (hep-ex)ALICElawheavy-ion experiments[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]PbPbNuclear Experiment (nucl-ex)[ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]kinetic freezoutNuclear ExperimentNuclear ExperimentBosonPhysicsLarge Hadron ColliderPhysicsfreeze-out radiusHEAVY-ION GENERATORlcsh:QC1-999:Mathematics and natural scienses: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP]Three-pion cumulant correlations3. Good healthPRIRODNE ZNANOSTI. Fizika.BOSE-EINSTEIN CORRELATIONSParticle Physics - ExperimentNuclear and High Energy PhysicsParticle physics[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]QC1-999particle cummulantsVDP::Matematikk og naturvitenskap: 400::Fysikk: 430::Kjerne- og elementærpartikkelfysikk: 431FOS: Physical sciencesALICE; pp; pPb; PbPb; Bose-Einstein; correlation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Kinetic energyp-pNuclear physicsBOSE-EINSTEIN CORRELATIONS; RANGE ANGULAR-CORRELATIONS; HEAVY-ION GENERATOR; MULTIPLICITY DEPENDENCEPion0103 physical sciencesNuclear Physics - Experimentddc:530Multiplicity (chemistry)010306 general physicsta114p–Pb and Pb–Pb collisionsVDP::Mathematics and natural scienses: 400::Physics: 430::Nuclear and elementary particle physics: 431010308 nuclear & particles physics:Matematikk og naturvitenskap: 400::Fysikk: 430::Kjerne- og elementærpartikkelfysikk: 431 [VDP]ALICE experimentBose–Einstein correlationsBose-EinsteinNATURAL SCIENCES. Physics.correlationpPbthree-pion cumulantslcsh:PhysicsBose–Einstein condensateRANGE ANGULAR-CORRELATIONSPhysics Letters B
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Charged jet cross sections and properties in proton-proton collisions at $\sqrt{s}=7$ TeV

2015

The differential charged jet cross sections, jet fragmentation distributions, and jet shapes are measured in minimum bias proton-proton collisions at centre-of-mass energy $\sqrt{s}=7$ TeV using the ALICE detector at the LHC. Jets are reconstructed from charged particle momenta in the mid-rapidity region using the sequential recombination $k_{\rm T}$ and anti-$k_{\rm T}$ as well as the SISCone jet finding algorithms with several resolution parameters in the range $R=0.2$ to $0.6$. Differential jet production cross sections measured with the three jet finders are in agreement in the transverse momentum ($p_{\rm T}$) interval $20<p_{\rm T}^{\rm jet,ch}<100$ GeV/$c$. They are also consistent w…

shapes:Kjerne- og elementærpartikkelfysikk: 431 [VDP]parton distributionsMonte Carlo methodP(P)OVER-BAR COLLISIONSALICE Charged jet proton-proton 7 TeVATLAS DETECTOR01 natural sciencesSpectral lineHigh Energy Physics - Experimentdifferential charged jet cross sectionENERGYHigh Energy Physics - Experiment (hep-ex)ALICEFragmentation (mass spectrometry)Nuclear and High Energy Physics differential charged jet cross sectionfragmentation[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment (nucl-ex)ROOT-S(NN)=2.76 TEVNuclear ExperimentNuclear Experimentroot-s(nn)=2.76 tevatlas detectorPhysicsLarge Hadron Collidercross sectionPhysicsDetectorCharged particle3. Good health:Mathematics and natural scienses: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP]charged jetsPRIRODNE ZNANOSTI. Fizika.:Nuclear and elementary particle physics: 431 [VDP]SHAPESTransverse momentumHADRON-COLLISIONSFRAGMENTATIONpp collisionsenergyParticle physicsNuclear and High Energy PhysicsAstrophysics::High Energy Astrophysical PhenomenaCharged jetVDP::Matematikk og naturvitenskap: 400::Fysikk: 430::Kjerne- og elementærpartikkelfysikk: 431FOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]114 Physical sciencestransverse-momentumNuclear physicsMinimum bias(P)OVER-BAR-P COLLISIONS P(P)OVER-BAR COLLISIONS PP COLLISIONS PARTON DISTRIBUTIONS TRANSVERSE-MOMENTUM SHAPES ALGORITHM ENERGY0103 physical sciences7 TeVNuclear Physics - Experimentproton-protonALGORITHM010306 general physics(p)over-bar-p collisionsPP COLLISIONSta114(P)OVER-BAR-P COLLISIONSVDP::Mathematics and natural scienses: 400::Physics: 430::Nuclear and elementary particle physics: 431010308 nuclear & particles physics:Matematikk og naturvitenskap: 400::Fysikk: 430::Kjerne- og elementærpartikkelfysikk: 431 [VDP]TRANSVERSE-MOMENTUMNATURAL SCIENCES. Physics.(p)over-bar-p collisions ; parton distributions ; transverse-momentum ; root-s(nn)=2.76 tev ; hadron-collisions ; atlas detector ; pp collisions ; fragmentation ; shapes ; energy ; charged jet ; cross section ; proton-proton ; 7 TeVhadron-collisionsPARTON DISTRIBUTIONSALICE; Charged jet; proton-proton; 7 TeVproton-proton collisionsHigh Energy Physics::Experimentcharged jet
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Precision measurement of the mass difference between light nuclei and anti-nuclei

2015

The measurement of the mass differences for systems bound by the strong force has reached a very high precision with protons and anti-protons. The extension of such measurement from (anti-)baryons to (anti-)nuclei allows one to probe any difference in the interactions between nucleons and anti-nucleons encoded in the (anti-)nuclei masses. This force is a remnant of the underlying strong interaction among quarks and gluons and can be described by effective theories, but cannot yet be directly derived from quantum chromodynamics. Here we report a measurement of the difference between the ratios of the mass and charge of deuterons and anti-deuterons, and $^{3}{\rm He}$ and $^3\overline{\rm He}…

electronQuarkspectroscopyAntiparticleParticle physicsPhysics of Elementary Particles and FieldsCPT symmetryStrong interactionNuclear TheoryantunucleiFOS: Physical sciencesAntiprotonGeneral Physics and Astronomy[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ElectronHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Physics and Astronomy (all)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Physics - ExperimentNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentAntihydrogenSpectroscopyNuclear Physicsantihydrogenmass measurementQuantum chromodynamicsPhysicsanti-nucleita114SPECTROSCOPY; ANTIHYDROGEN; ANTIPROTON; ELECTRONmass difference nuclei antunucleiHigh Energy Physics::Phenomenologymass differenceNATURAL SCIENCES. Physics.3. Good healthGluonPRIRODNE ZNANOSTI. Fizika.antiprotonnucleiQuark–gluon plasmamassmass difference ; nuclei ; anti-nuclei ; ALICE ; CERNHigh Energy Physics::ExperimentNucleon
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