Search results for "DEPENDENCE"

showing 10 items of 2462 documents

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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"Table 3" of "Model-independent measurement of the W boson helicity in top quark decays at D0"

2008

COS(THETA*) distribution for W decay in dilepton events.. Data are read from plots and errors are statistcial (sqrt(N)).

PBAR P --> LEPTON+ LEPTON- XPBAR P --> TOP TOPBARNuclear TheoryW pair ProductionDN/DCOSTHETATopPBAR P --> W+ W- BOTTOM BOTTOMBARSingle Differential DistributionInclusiveExclusiveHigh Energy Physics::ExperimentNuclear Experiment1960.0Angular DependenceDrell YanW Production
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"Table 6" of "Model-independent measurement of the W boson helicity in top quark decays at D0"

2008

COS(THETA*) distribution for W decay in dilepton events.. The data in this table are PRELIMINARY and taken from D0 Note 5722-CONF. Data are read from plots and errors are statistcial (sqrt(N)).

PBAR P --> LEPTON+ LEPTON- XPBAR P --> TOP TOPBARW pair ProductionDN/DCOSTHETATopPBAR P --> W+ W- BOTTOM BOTTOMBARSingle Differential DistributionInclusiveExclusiveHigh Energy Physics::ExperimentNuclear Experiment1960.0Angular DependenceDrell YanW Production
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"Table 1" of "Model-independent measurement of the W boson helicity in top quark decays at D0"

2008

COS(THETA*) distribution for leptonic W decay in lepton+jets events.. Data are read from plots and errors are statistcial (sqrt(N)).

PBAR P --> TOP TOPBARHigh Energy Physics::PhenomenologyW pair ProductionDN/DCOSTHETATopPBAR P --> W+ W- BOTTOM BOTTOMBARSingle Differential DistributionJet ProductionInclusiveExclusiveHigh Energy Physics::ExperimentPBAR P --> LEPTON JETS X1960.0Angular DependenceW Production
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"Table 4" of "Model-independent measurement of the W boson helicity in top quark decays at D0"

2008

COS(THETA*) distribution for leptonic W decay in lepton+jets events.. The data in this table are PRELIMINARY and taken from D0 Note 5722-CONF. Data are read from plots and errors are statistcial (sqrt(N)).

PBAR P --> TOP TOPBARHigh Energy Physics::PhenomenologyW pair ProductionDN/DCOSTHETATopPBAR P --> W+ W- BOTTOM BOTTOMBARSingle Differential DistributionJet ProductionInclusiveExclusiveHigh Energy Physics::ExperimentPBAR P --> LEPTON JETS X1960.0Angular DependenceW Production
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"Table 5" of "Model-independent measurement of the W boson helicity in top quark decays at D0"

2008

COS(THETA*) distribution for hadronic W decay in lepton+jets events.. The data in this table are PRELIMINARY and taken from D0 Note 5722-CONF. Data are read from plots and errors are statistcial (sqrt(N)).

PBAR P --> TOP TOPBARHigh Energy Physics::PhenomenologyW pair ProductionDN/DCOSTHETATopPBAR P --> W+ W- BOTTOM BOTTOMBARSingle Differential DistributionJet ProductionInclusiveExclusiveHigh Energy Physics::ExperimentPBAR P --> LEPTON JETS XNuclear Experiment1960.0Angular DependenceW Production
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"Table 2" of "Model-independent measurement of the W boson helicity in top quark decays at D0"

2008

COS(THETA*) distribution for hadronic W decay in lepton+jets events.. Data are read from plots and errors are statistcial (sqrt(N)).

PBAR P --> TOP TOPBARHigh Energy Physics::PhenomenologyW pair ProductionDN/DCOSTHETATopPBAR P --> W+ W- BOTTOM BOTTOMBARSingle Differential DistributionJet ProductionInclusiveExclusiveHigh Energy Physics::ExperimentPBAR P --> LEPTON JETS XNuclear Experiment1960.0Angular DependenceW Production
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"Table 4" of "Measurement of inclusive jet cross-sections in Z/gamma*(---> e+ e-) + jets production in p anti-p collisions at s**(1/2) = 1.96-TeV"

2007

Measured inclusive jet differential cross section for .GE.1JET.

PBAR P --> Z0 .GE.1JET XInclusiveSingle Differential Cross SectionPBAR P --> GAMMA* .GE.1JET XZ ProductionElectron productionDSIG/DPTJet ProductionTransverse Momentum Dependence1960.0
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"Table 2" of "Production properties of D0, D+, D*+ and D(s)+ in 230-GeV/c pi- and K- Cu interactions"

1992

Data fitted with the form d2sig/dxdpt**2 alpha ((1-x)**N)* EXP(-B*PT**2) using combined maximum likelihood fit to the invariant mass spectrum and the x and pt**2 distributions. The values for N and B are given here. Additional systematic errors are 10 pct for N and 3 pct for B.

PI- CU --> D*(2010)+ XPI- CU --> D/S- XStrange productionPI- CU --> D*(2010)- XPI- CU --> D/S+ XDSIG/DXLPI- CU --> D+ XPI- CU --> DBAR0 XInclusiveSingle Differential Cross SectionPI- NUCLEUS --> CHARM XPI- NUCLEUS --> CHARMBAR XCharm productionPI- CU --> D- XPI- CU --> D0 XDSIG/DPT**22.300E+022.300E+02Transverse Momentum Dependence
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"Table 1" of "Production properties of D0, D+, D*+ and D(s)+ in 230-GeV/c pi- and K- Cu interactions"

1992

Data fitted with the form d2sig/dxdpt**2 alpha ((1-x)**N)* EXP(-B*PT**2) using combined maximum likelihood fit to the invariant mass spectrum and the x and pt**2 distributions. The values for N and B are given here. Additional systematic errors are 10 pct for N and 3 pct for B.

PI- CU --> D*(2010)+ XPI- CU --> D/S- XStrange productionPI- CU --> D*(2010)- XPI- CU --> D/S+ XDSIG/DXLPI- CU --> D+ XPI- CU --> DBAR0 XInclusiveSingle Differential Cross SectionPI- NUCLEUS --> CHARM XPI- NUCLEUS --> CHARMBAR XCharm productionPI- CU --> D- XPI- CU --> D0 XDSIG/DPT**22.300E+022.300E+02Transverse Momentum Dependence
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