Search results for "Strange Production"

showing 10 items of 325 documents

"Table 9" of "Collins and Sivers asymmetries for pions and kaons in muon-deuteron DIS"

2008

The Collins and Sivers asymmetry as a function of Z for 'ALL' positive kaons from the 2003-2004 data.. Errors are statistical only.

MU+ DEUT --> MU+ K+ XInclusiveStrange productionAsymmetry MeasurementNuclear TheoryNeutral CurrentDeep Inelastic ScatteringComputer Science::Symbolic ComputationHigh Energy Physics::ExperimentNuclear ExperimentMuon productionASYM
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"Table 35" of "K*(892)^0 and PHI(1020) production in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV"

2015

Enhancement ratio of Lambda for different centrality intervals in Pb-Pb collisions at sqrt(sNN)=2.76 TeV. The enhancement ratio is the ratio of the yield of a particle in A-A collisions to the yield of the particle in pp collisions, scaled by the average number of participant nucleons: Enhancement=[Yield(A-A)/]/[Yield(pp)/2]. The Lambda yield for pp collisions at sqrt(s)=2.76 TeV is extrapolated from the measured yield at sqrt(s)=7 TeV. In the tables, the first systematic uncertainty is the uncertainty from the Pb-Pb data and the second is from the uncertainty in . In the paper this ratio is plotted as a function of the values taken from PRC 88, 044909 (2013).

N/NInclusiveStrange production2760.0Nuclear ExperimentPB PB --> LAMBDA X
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"Table 34" of "K*(892)^0 and PHI(1020) production in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV"

2015

Enhancement ratio of phi(1020) for different centrality intervals in Pb-Pb collisions at sqrt(sNN)=2.76 TeV. The enhancement ratio is the ratio of the yield of a particle in A-A collisions to the yield of the particle in pp collisions, scaled by the average number of participant nucleons: Enhancement=[Yield(A-A)/]/[Yield(pp)/2]. The phi(1020) yield for pp collisions at sqrt(s)=2.76 TeV is interpolated between the measured yields at sqrt(s)=900 GeV and sqrt(s)=7 TeV. In the tables, the first systematic uncertainty is the uncorrelated uncertainty from the Pb-Pb data, the second is the normalization uncertainty from the Pb-Pb data, and the third is from the uncertainty in . In the paper this r…

N/NInclusiveStrange production2760.0PB PB --> PHI XNuclear Experiment
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"Table 3" of "Measurement of the transverse polarization of $\Lambda$ and $\bar{\Lambda}$ hyperons produced in proton-proton collisions at $\sqrt{s}=…

2015

Transverse polarization POL of LAMBDA and LAMBDABAR hyperons as a function of PT.

Nonlinear Sciences::Chaotic DynamicsPOLInclusiveProton-Proton ScatteringStrange productionPolarizationHigh Energy Physics::PhenomenologyNuclear Theory7000.0High Energy Physics::ExperimentP P --> LAMBDA XNuclear Experiment
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"Table 2" of "Measurement of the transverse polarization of $\Lambda$ and $\bar{\Lambda}$ hyperons produced in proton-proton collisions at $\sqrt{s}=…

2015

Transverse polarization POL of LAMBDA and LAMBDABAR hyperons as a function of XF.

Nonlinear Sciences::Chaotic DynamicsPOLInclusiveProton-Proton ScatteringStrange productionPolarizationHigh Energy Physics::PhenomenologyNuclear Theory7000.0High Energy Physics::ExperimentP P --> LAMBDA XNuclear Experiment
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"Table 4" of "Meson production in p + U, O + U and S + U interactions at 200-GeV/nucleon."

1993

No description provided.

P NUCLEUS --> PI- XInclusiveSingle Differential Cross SectionStrange productionP NUCLEUS --> K- XP U --> K- XDSIG/DPT**2Transverse Momentum DependenceP U --> PI- X
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"Table 1" of "Measurement of $D^{*\pm}$, $D^\pm$ and $D_s^\pm$ meson production cross sections in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS …

2017

The visible low-$p_T$, $3.5

P P --> D*(2010)- XP P --> D*(2010)+ XIntegrated Cross Section7000.0P P --> D/S+ XCross SectionP P --> D+ XSIGP P --> D/S- XInclusiveStrange ProductionP P --> D- XProton-Proton ScatteringCharm Production
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"Table 10" of "Multiplicity dependence of charged pion, kaon, and (anti)proton production at large transverse momentum in p-Pb collisions at $\mathbf…

2016

The nuclear modification factor RPPB of charged pions, charged kaons and protons+antiprotons as a function of pT in NSD p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV. The first uncertainty is statistical, the second is the systematic one.

P P --> K+ XP P --> P XNuclear TheoryP PB --> P XP P --> K- X5.02P PB --> PI- XInclusiveStrange ProductionRATIOP PB --> K+ XProton-Proton ScatteringP PB --> K- XP P --> PBAR XPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentP P --> PI+ XNuclear ExperimentP PB --> PBAR XP P --> PI- XP PB --> PI+ X
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"Table 5" of "Production of charged pions, kaons and protons at large transverse momenta in pp and Pb-Pb collisions at sqrt(sNN) = 2.76 TeV"

2014

Kaon-to-pion ratios as a function of pT measured in Pb-Pb and pp collisions.

P P --> K+ XStrange production2760.0Nuclear TheoryPB PB --> PI+ XPB PB --> PI- XP P --> K- XInclusiveRATIOProton-Proton ScatteringPB PB --> K- XHigh Energy Physics::ExperimentP P --> PI+ XPB PB --> K+ XNuclear ExperimentP P --> PI- X
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"Table 2" of "Production of charged pions, kaons and protons at large transverse momenta in pp and Pb-Pb collisions at sqrt(sNN) = 2.76 TeV"

2014

Invariant yields of identified kaons in central and peripheral Pb-Pb collisions, together with the unscaled pp reference yields.

P P --> K+ XStrange production2760.0Nuclear TheorySingle Differential DistributionP P --> K- XDN/DPTInclusiveProton-Proton ScatteringPB PB --> K- XHigh Energy Physics::ExperimentPB PB --> K+ XNuclear ExperimentTransverse Momentum DependenceComputer Science::Distributed Parallel and Cluster Computing
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