Search results for "5023.0"

showing 10 items of 29 documents

"Table 2.3" of "Measurement of electrons from semileptonic heavy-flavour hadron decays at midrapidity in pp and Pb-Pb collisions at $\sqrt{s_{\rm{NN}…

2020

HFe cross section in Pb-Pb, 60-80 centrality

5023.01/(Nev*2*PI*PT)*D2(N)/DPT/DYRAPSemileptonic Heavy-Flavour Hadron DecaysCentrality 60-80%Invariant Yield
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"Table 1" of "Measurement of electrons from semileptonic heavy-flavour hadron decays at midrapidity in pp and Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}…

2020

HFe cross section in pp

5023.01/(Nev*2*PI*PT)*D2(N)/DPT/DYRAPSemileptonic Heavy-Flavour Hadron DecaysCross Section
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"Table 2.2" of "Measurement of electrons from semileptonic heavy-flavour hadron decays at midrapidity in pp and Pb-Pb collisions at $\sqrt{s_{\rm{NN}…

2020

HFe cross section in Pb-Pb, 30-50 centrality

5023.01/(Nev*2*PI*PT)*D2(N)/DPT/DYRAPSemileptonic Heavy-Flavour Hadron DecaysInvariant YieldCentrality 30-50%
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"Table 2.1" of "Measurement of electrons from semileptonic heavy-flavour hadron decays at midrapidity in pp and Pb-Pb collisions at $\sqrt{s_{\rm{NN}…

2020

HFe cross section in Pb-Pb, 0-10 centrality

5023.0Centrality 0-10%1/(Nev*2*PI*PT)*D2(N)/DPT/DYRAPSemileptonic Heavy-Flavour Hadron DecaysInvariant Yield
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"Table 3.1" of "Measurement of electrons from semileptonic heavy-flavour hadron decays at midrapidity in pp and Pb-Pb collisions at $\sqrt{s_{\rm{NN}…

2020

HFe RAA in Pb-Pb, 0-10 centrality

5023.0Centrality 0-10%Semileptonic Heavy-Flavour Hadron DecaysRAANuclear Modification Factor
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"DN/DETARAP" of "Centrality dependence of the pseudorapidity density distribution for charged particles in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.0…

2017

Charged-particle pseudorapidity density for ten centrality classes over a broad $\eta$ range in Pb-Pb collisions at $\sqrt{s_{_{\mathrm{NN}}}}=5.02\,\mathrm{TeV}$. Boxes around the points reflect the total uncorrelated systematic uncertainties, while the filled squares on the right reflect the correlated systematic uncertainty (evaluated at $\eta=0$). Statistical errors are generally insignificant and smaller than the markers. Also shown is the reflection of the $3.5<\eta<5$ values around $\eta=0$ (open circles). The line corresponds to fits of the difference between two Gaussians centred at $\eta=0$ ($f_{\text{GG}}$) [PLB754.373] to the data.

5023.0DN/DETARAPHigh Energy Physics::ExperimentNuclear ExperimentPB PB --> CHARGED X
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"DN/DETARAP(ETARAP=0)" of "Centrality dependence of the pseudorapidity density distribution for charged particles in Pb-Pb collisions at $\sqrt{s_{\r…

2017

Charged-particle pseudorapidity density at midrapidity in most perihperhal (80-90%) Pb-Pb collisions at $\sqrt{s_{\scriptscriptstyle\mathrm{NN}}}=5.02\,\mathrm{TeV}$.

5023.0DN/DETARAPPB PB --> Charged XHigh Energy Physics::ExperimentNuclear Experiment
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"Table 1.4" of "Probing the effects of strong electromagnetic fields with charge-dependent directed flow in Pb-Pb collisions at the LHC"

2020

Directed flow D0 meson 10-40%

5023.0High Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryHigh Energy Physics::ExperimentD0 mesonDirected flowNuclear Experiment
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"Table 1.5" of "Probing the effects of strong electromagnetic fields with charge-dependent directed flow in Pb-Pb collisions at the LHC"

2020

Directed flow D0-bar meson 10-40%

5023.0High Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyD0-bar mesonHigh Energy Physics::ExperimentDirected flowNuclear Experiment
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"MULT" of "Centrality dependence of the pseudorapidity density distribution for charged particles in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

2017

Total number of charged particles as a function of the mean number of participating nucleons [PRC88.044909]. The total charged-particle multiplicity is given as the integral over $\mathrm{d}N_{\mathrm{ch}}/\mathrm{d}\eta$ over the measured region ($-3.5<\eta<5$) and extrapolations from fitted functions in the unmeasured regions. The contribution from unmeasured $\eta$ regions amounts to $\approx30\%$ of the total number of charged particles. The uncertainty on the extrapolation to the unmeasured pseudorapidity region is smaller than the size of the markers. The contribution to the systematic uncertainties from the centrality determination and electromagnetic processes are vanishing co…

5023.0PB PB --> CHARGED XMULT
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