Search results for "Pb"

showing 10 items of 3522 documents

"Table 3" of "$\Upsilon$ production and nuclear modification at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\textbf{NN}}}=5.02…

2021

$p_{\mathrm{T}}$-differential yield of $\Upsilon(1\mathrm{S}) \rightarrow \mu^{+}\mu^{-}$ divided by the average nuclear overlap function $\langle T_{\mathrm{AA}} \rangle$ for the 0–90% centrality interval ($\langle T_{\mathrm{AA}} \rangle$ = 6.28 $\pm$ 0.06 mb$^{-1}$).

5020.0InclusiveUpsilonD2N/DYRAP/DPTPb Pb --> UPSI(1S) < MU+ MU- > XTransverse Momentum DependenceLead-Lead Scattering
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"Table 8" of "$\rm \Lambda_{c}^{+}$ production and baryon-to-meson ratios in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV at the LHC"

2021

$p_{\rm {T}}$-integrated ($p_{\rm {T}} > 0$) $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ ratio in pp collisions at $\sqrt{s} = 5.02$ TeV in the rapidity interval $|y|<0.5$, and in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV in the rapidity interval $-0.96 \lt y \lt 0.04$. The second (sys) error is from the extrapolation to the full $p_{\rm {T}}$ range.

5020.0Lc/D0P P --> Lc XP PB --> Lc Xbaryon-to-meson ratio
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"Table 6" of "$\rm \Lambda_{c}^{+}$ production and baryon-to-meson ratios in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV at the LHC"

2021

The $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ ratio measured in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV in the transverse momentum interval $2 \lt p_{\rm T} \lt 12$ GeV/c and in the rapidity interval $-0.96 \lt y \lt 0.04$.

5020.0Lc/D0P PB --> D0 XP PB --> Lc Xbaryon-to-meson ratio
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"Table 5" of "$\rm \Lambda_{c}^{+}$ production and baryon-to-meson ratios in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV at the LHC"

2021

The $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ ratio as a function of $p_{\rm {T}}$ measured in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV in the rapidity interval $ -0.96\lt y \lt 0.04$.

5020.0Lc/D0P PB --> D0 XP PB --> Lc Xbaryon-to-meson ratio
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"Table 1" of "First observation of an attractive interaction between a proton and a multi-strange baryon"

2019

The p$-$p $\oplus$ $\overline{\mathrm{p}}-\overline{\mathrm{p}}$ correlation function.

5020.0Mathematics::Complex VariablesCORRHigh Energy Physics::PhenomenologyP P --> P P XP P --> PBAR PBAR X
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"Table 5" of "Measurement of Z$^0$-boson production at large rapidities in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

2018

Invariant yield of Z$^{0}$ production in 2.5 < y < 4.0 divided by the average nuclear overlap function as a function of the average number of participants scaled by the average number of binary nucleon-nucleon collisions. The first uncertainty is statistical, the second is the uncorrelated systematic and the third is the correlated systematic.

5020.0Nuclear TheoryDN/DYRAP/MEAN(TAA)Nuclear ExperimentPB PB --> Z0 < MU+ MU- > X
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"Table 6" of "Measurement of Z$^0$-boson production at large rapidities in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

2018

Nuclear modification factor of Z$^{0}$ production in 2.5 < y < 4.0 as a function of the average number of participants scaled by the average number of binary nucleon-nucleon collisions. The first uncertainty is statistical, the second is the uncorrelated systematic and the third is the correlated systematic.

5020.0Nuclear TheoryNuclear ExperimentPB PB --> Z0 < MU+ MU- > XRAA
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"Table 7" of "Dielectron production in proton-proton and proton-lead collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

2020

Dielectron nuclear modification factor $R_{\rm pPb}$ at $\sqrt{s}$ = 5.02 TeV as a function of $m_{\rm ee}$. Electrons are measured within $|\eta_{\rm e}| < 0.8$ and $p_{\rm T,e} > 0.2$ GeV/$c$.

5020.0P P --> E+ E- XDielectron nuclear modification factorDSIG/DMP PB --> E+ E- X
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"Table 8" of "Dielectron production in proton-proton and proton-lead collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

2020

Dielectron nuclear modification factor $R_{\rm pPb}$ at $\sqrt{s}$ = 5.02 TeV as a function of $p_{\rm T,ee}$ for $0.5 < m_{\rm ee} < 1.1$ GeV/$c$. Electrons are measured within $|\eta_{\rm e}| < 0.8$ and $p_{\rm T,e} > 0.2$ GeV/$c$.

5020.0P P --> E+ E- XDielectron nuclear modification factorP PB --> E+ E- XDSIG/DPTEE
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"Table 9" of "Dielectron production in proton-proton and proton-lead collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

2020

Dielectron nuclear modification factor $R_{\rm pPb}$ at $\sqrt{s}$ = 5.02 TeV as a function of $p_{\rm T,ee}$ for $1.1 < m_{\rm ee} < 2.7$ GeV/$c$. Electrons are measured within $|\eta_{\rm e}| < 0.8$ and $p_{\rm T,e} > 0.2$ GeV/$c$.

5020.0P P --> E+ E- XDielectron nuclear modification factorP PB --> E+ E- XDSIG/DPTEE
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