cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.72936.v1/t5
title: "Table 5" of "Inclusive quarkonium production at forward rapidity in pp collisions at $\sqrt{s}=8$ TeV"

description: Differential production cross sections of $\psi$(2S) as a function of rapidity.
description: CERN-LHC. We report on the inclusive production cross sections of J/$\psi$, $\psi$(2S), $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S), measured at forward rapidity with the ALICE detector in pp collisions at a center-of-mass energy $\sqrt{s} = 8$ TeV. The analysis is based on data collected at the LHC and corresponds to an integrated luminosity of 1.23 pb$^{-1}$. Quarkonia are reconstructed in the dimuon-decay channel. The differential production cross sections are measured as a function of the transverse momentum $p_{\rm T}$ and rapidity $y$, over the $p_{\rm T}$ ranges 0 &lt; $p_{\rm T}$ &lt; 20 GeV/$c$ for J/$\psi$, 0 &lt; $p_{\rm T}$ &lt; 12 GeV/$c$ for all other resonances, and for 2.5 &lt; $y$ &lt; 4. The cross sections, integrated over $y$ and $p_{\rm T}$, and assuming unpolarized quarkonia, are $\sigma_{\text{J}/\psi} = 8.98 \pm 0.04 \pm 0.82$ $\mu$b, $\sigma_{\psi\text{(2S)}} = 1.23 \pm 0.08 \pm 0.22$ $\mu$b, $\sigma_{\Upsilon\text{(1S)}} = 71 \pm 6 \pm 7$ nb, $\sigma_{\Upsilon\text{(2S)}} = 26 \pm 5 \pm 4$ nb and $\sigma_{\Upsilon\text{(3S)}} = 9 \pm 4 \pm 1$ nb, where the first uncertainty is statistical and the second one is systematic. These values agree, within at most 1.4\sigma, with measurements performed by the LHCb collaboration in the same rapidity range.
DOI: 10.17182/hepdata.72936.v1/t6
title: "Table 6" of "Inclusive quarkonium production at forward rapidity in pp collisions at $\sqrt{s}=8$ TeV"

description: integrated production cross section of $\psi$(2S).
description: CERN-LHC. We report on the inclusive production cross sections of J/$\psi$, $\psi$(2S), $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S), measured at forward rapidity with the ALICE detector in pp collisions at a center-of-mass energy $\sqrt{s} = 8$ TeV. The analysis is based on data collected at the LHC and corresponds to an integrated luminosity of 1.23 pb$^{-1}$. Quarkonia are reconstructed in the dimuon-decay channel. The differential production cross sections are measured as a function of the transverse momentum $p_{\rm T}$ and rapidity $y$, over the $p_{\rm T}$ ranges 0 &lt; $p_{\rm T}$ &lt; 20 GeV/$c$ for J/$\psi$, 0 &lt; $p_{\rm T}$ &lt; 12 GeV/$c$ for all other resonances, and for 2.5 &lt; $y$ &lt; 4. The cross sections, integrated over $y$ and $p_{\rm T}$, and assuming unpolarized quarkonia, are $\sigma_{\text{J}/\psi} = 8.98 \pm 0.04 \pm 0.82$ $\mu$b, $\sigma_{\psi\text{(2S)}} = 1.23 \pm 0.08 \pm 0.22$ $\mu$b, $\sigma_{\Upsilon\text{(1S)}} = 71 \pm 6 \pm 7$ nb, $\sigma_{\Upsilon\text{(2S)}} = 26 \pm 5 \pm 4$ nb and $\sigma_{\Upsilon\text{(3S)}} = 9 \pm 4 \pm 1$ nb, where the first uncertainty is statistical and the second one is systematic. These values agree, within at most 1.4\sigma, with measurements performed by the LHCb collaboration in the same rapidity range.
DOI: 10.17182/hepdata.72936.v1/t7
title: "Table 7" of "Inclusive quarkonium production at forward rapidity in pp collisions at $\sqrt{s}=8$ TeV"

description: Differential production cross sections of $\Upsilon$(1S) as a function of $p_{\rm T}$.
description: CERN-LHC. We report on the inclusive production cross sections of J/$\psi$, $\psi$(2S), $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S), measured at forward rapidity with the ALICE detector in pp collisions at a center-of-mass energy $\sqrt{s} = 8$ TeV. The analysis is based on data collected at the LHC and corresponds to an integrated luminosity of 1.23 pb$^{-1}$. Quarkonia are reconstructed in the dimuon-decay channel. The differential production cross sections are measured as a function of the transverse momentum $p_{\rm T}$ and rapidity $y$, over the $p_{\rm T}$ ranges 0 &lt; $p_{\rm T}$ &lt; 20 GeV/$c$ for J/$\psi$, 0 &lt; $p_{\rm T}$ &lt; 12 GeV/$c$ for all other resonances, and for 2.5 &lt; $y$ &lt; 4. The cross sections, integrated over $y$ and $p_{\rm T}$, and assuming unpolarized quarkonia, are $\sigma_{\text{J}/\psi} = 8.98 \pm 0.04 \pm 0.82$ $\mu$b, $\sigma_{\psi\text{(2S)}} = 1.23 \pm 0.08 \pm 0.22$ $\mu$b, $\sigma_{\Upsilon\text{(1S)}} = 71 \pm 6 \pm 7$ nb, $\sigma_{\Upsilon\text{(2S)}} = 26 \pm 5 \pm 4$ nb and $\sigma_{\Upsilon\text{(3S)}} = 9 \pm 4 \pm 1$ nb, where the first uncertainty is statistical and the second one is systematic. These values agree, within at most 1.4\sigma, with measurements performed by the LHCb collaboration in the same rapidity range.
DOI: 10.17182/hepdata.72936.v1/t8
title: "Table 8" of "Inclusive quarkonium production at forward rapidity in pp collisions at $\sqrt{s}=8$ TeV"

description: Differential production cross sections of $\Upsilon$(1S) as a function of rapidity.
description: CERN-LHC. We report on the inclusive production cross sections of J/$\psi$, $\psi$(2S), $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S), measured at forward rapidity with the ALICE detector in pp collisions at a center-of-mass energy $\sqrt{s} = 8$ TeV. The analysis is based on data collected at the LHC and corresponds to an integrated luminosity of 1.23 pb$^{-1}$. Quarkonia are reconstructed in the dimuon-decay channel. The differential production cross sections are measured as a function of the transverse momentum $p_{\rm T}$ and rapidity $y$, over the $p_{\rm T}$ ranges 0 &lt; $p_{\rm T}$ &lt; 20 GeV/$c$ for J/$\psi$, 0 &lt; $p_{\rm T}$ &lt; 12 GeV/$c$ for all other resonances, and for 2.5 &lt; $y$ &lt; 4. The cross sections, integrated over $y$ and $p_{\rm T}$, and assuming unpolarized quarkonia, are $\sigma_{\text{J}/\psi} = 8.98 \pm 0.04 \pm 0.82$ $\mu$b, $\sigma_{\psi\text{(2S)}} = 1.23 \pm 0.08 \pm 0.22$ $\mu$b, $\sigma_{\Upsilon\text{(1S)}} = 71 \pm 6 \pm 7$ nb, $\sigma_{\Upsilon\text{(2S)}} = 26 \pm 5 \pm 4$ nb and $\sigma_{\Upsilon\text{(3S)}} = 9 \pm 4 \pm 1$ nb, where the first uncertainty is statistical and the second one is systematic. These values agree, within at most 1.4\sigma, with measurements performed by the LHCb collaboration in the same rapidity range.
DOI: 10.17182/hepdata.72936.v1/t9
title: "Table 9" of "Inclusive quarkonium production at forward rapidity in pp collisions at $\sqrt{s}=8$ TeV"

description: integrated production cross section of $\Upsilon$(1S).
description: CERN-LHC. We report on the inclusive production cross sections of J/$\psi$, $\psi$(2S), $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S), measured at forward rapidity with the ALICE detector in pp collisions at a center-of-mass energy $\sqrt{s} = 8$ TeV. The analysis is based on data collected at the LHC and corresponds to an integrated luminosity of 1.23 pb$^{-1}$. Quarkonia are reconstructed in the dimuon-decay channel. The differential production cross sections are measured as a function of the transverse momentum $p_{\rm T}$ and rapidity $y$, over the $p_{\rm T}$ ranges 0 &lt; $p_{\rm T}$ &lt; 20 GeV/$c$ for J/$\psi$, 0 &lt; $p_{\rm T}$ &lt; 12 GeV/$c$ for all other resonances, and for 2.5 &lt; $y$ &lt; 4. The cross sections, integrated over $y$ and $p_{\rm T}$, and assuming unpolarized quarkonia, are $\sigma_{\text{J}/\psi} = 8.98 \pm 0.04 \pm 0.82$ $\mu$b, $\sigma_{\psi\text{(2S)}} = 1.23 \pm 0.08 \pm 0.22$ $\mu$b, $\sigma_{\Upsilon\text{(1S)}} = 71 \pm 6 \pm 7$ nb, $\sigma_{\Upsilon\text{(2S)}} = 26 \pm 5 \pm 4$ nb and $\sigma_{\Upsilon\text{(3S)}} = 9 \pm 4 \pm 1$ nb, where the first uncertainty is statistical and the second one is systematic. These values agree, within at most 1.4\sigma, with measurements performed by the LHCb collaboration in the same rapidity range.
DOI: 10.17182/hepdata.72936.v1/t10
title: "Table 10" of "Inclusive quarkonium production at forward rapidity in pp collisions at $\sqrt{s}=8$ TeV"

description: Differential production cross sections of $\Upsilon$(2S) as a function of rapidity.
description: CERN-LHC. We report on the inclusive production cross sections of J/$\psi$, $\psi$(2S), $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S), measured at forward rapidity with the ALICE detector in pp collisions at a center-of-mass energy $\sqrt{s} = 8$ TeV. The analysis is based on data collected at the LHC and corresponds to an integrated luminosity of 1.23 pb$^{-1}$. Quarkonia are reconstructed in the dimuon-decay channel. The differential production cross sections are measured as a function of the transverse momentum $p_{\rm T}$ and rapidity $y$, over the $p_{\rm T}$ ranges 0 &lt; $p_{\rm T}$ &lt; 20 GeV/$c$ for J/$\psi$, 0 &lt; $p_{\rm T}$ &lt; 12 GeV/$c$ for all other resonances, and for 2.5 &lt; $y$ &lt; 4. The cross sections, integrated over $y$ and $p_{\rm T}$, and assuming unpolarized quarkonia, are $\sigma_{\text{J}/\psi} = 8.98 \pm 0.04 \pm 0.82$ $\mu$b, $\sigma_{\psi\text{(2S)}} = 1.23 \pm 0.08 \pm 0.22$ $\mu$b, $\sigma_{\Upsilon\text{(1S)}} = 71 \pm 6 \pm 7$ nb, $\sigma_{\Upsilon\text{(2S)}} = 26 \pm 5 \pm 4$ nb and $\sigma_{\Upsilon\text{(3S)}} = 9 \pm 4 \pm 1$ nb, where the first uncertainty is statistical and the second one is systematic. These values agree, within at most 1.4\sigma, with measurements performed by the LHCb collaboration in the same rapidity range.
DOI: 10.17182/hepdata.72936.v1/t11
title: "Table 11" of "Inclusive quarkonium production at forward rapidity in pp collisions at $\sqrt{s}=8$ TeV"

description: integrated production cross section of Upsilon (2S).
description: CERN-LHC. We report on the inclusive production cross sections of J/$\psi$, $\psi$(2S), $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S), measured at forward rapidity with the ALICE detector in pp collisions at a center-of-mass energy $\sqrt{s} = 8$ TeV. The analysis is based on data collected at the LHC and corresponds to an integrated luminosity of 1.23 pb$^{-1}$. Quarkonia are reconstructed in the dimuon-decay channel. The differential production cross sections are measured as a function of the transverse momentum $p_{\rm T}$ and rapidity $y$, over the $p_{\rm T}$ ranges 0 &lt; $p_{\rm T}$ &lt; 20 GeV/$c$ for J/$\psi$, 0 &lt; $p_{\rm T}$ &lt; 12 GeV/$c$ for all other resonances, and for 2.5 &lt; $y$ &lt; 4. The cross sections, integrated over $y$ and $p_{\rm T}$, and assuming unpolarized quarkonia, are $\sigma_{\text{J}/\psi} = 8.98 \pm 0.04 \pm 0.82$ $\mu$b, $\sigma_{\psi\text{(2S)}} = 1.23 \pm 0.08 \pm 0.22$ $\mu$b, $\sigma_{\Upsilon\text{(1S)}} = 71 \pm 6 \pm 7$ nb, $\sigma_{\Upsilon\text{(2S)}} = 26 \pm 5 \pm 4$ nb and $\sigma_{\Upsilon\text{(3S)}} = 9 \pm 4 \pm 1$ nb, where the first uncertainty is statistical and the second one is systematic. These values agree, within at most 1.4\sigma, with measurements performed by the LHCb collaboration in the same rapidity range.
DOI: 10.17182/hepdata.72936.v1/t12
title: "Table 12" of "Inclusive quarkonium production at forward rapidity in pp collisions at $\sqrt{s}=8$ TeV"

description: integrated production cross section of Upsilon (3S).
description: CERN-LHC. We report on the inclusive production cross sections of J/$\psi$, $\psi$(2S), $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S), measured at forward rapidity with the ALICE detector in pp collisions at a center-of-mass energy $\sqrt{s} = 8$ TeV. The analysis is based on data collected at the LHC and corresponds to an integrated luminosity of 1.23 pb$^{-1}$. Quarkonia are reconstructed in the dimuon-decay channel. The differential production cross sections are measured as a function of the transverse momentum $p_{\rm T}$ and rapidity $y$, over the $p_{\rm T}$ ranges 0 &lt; $p_{\rm T}$ &lt; 20 GeV/$c$ for J/$\psi$, 0 &lt; $p_{\rm T}$ &lt; 12 GeV/$c$ for all other resonances, and for 2.5 &lt; $y$ &lt; 4. The cross sections, integrated over $y$ and $p_{\rm T}$, and assuming unpolarized quarkonia, are $\sigma_{\text{J}/\psi} = 8.98 \pm 0.04 \pm 0.82$ $\mu$b, $\sigma_{\psi\text{(2S)}} = 1.23 \pm 0.08 \pm 0.22$ $\mu$b, $\sigma_{\Upsilon\text{(1S)}} = 71 \pm 6 \pm 7$ nb, $\sigma_{\Upsilon\text{(2S)}} = 26 \pm 5 \pm 4$ nb and $\sigma_{\Upsilon\text{(3S)}} = 9 \pm 4 \pm 1$ nb, where the first uncertainty is statistical and the second one is systematic. These values agree, within at most 1.4\sigma, with measurements performed by the LHCb collaboration in the same rapidity range.
DOI: 10.17182/hepdata.72936.v1/t13
title: "Table 13" of "Inclusive quarkonium production at forward rapidity in pp collisions at $\sqrt{s}=8$ TeV"

description: $\psi$(2S) over J/$\psi$ ratio as a function of $p_{\rm T}$.
description: CERN-LHC. We report on the inclusive production cross sections of J/$\psi$, $\psi$(2S), $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S), measured at forward rapidity with the ALICE detector in pp collisions at a center-of-mass energy $\sqrt{s} = 8$ TeV. The analysis is based on data collected at the LHC and corresponds to an integrated luminosity of 1.23 pb$^{-1}$. Quarkonia are reconstructed in the dimuon-decay channel. The differential production cross sections are measured as a function of the transverse momentum $p_{\rm T}$ and rapidity $y$, over the $p_{\rm T}$ ranges 0 &lt; $p_{\rm T}$ &lt; 20 GeV/$c$ for J/$\psi$, 0 &lt; $p_{\rm T}$ &lt; 12 GeV/$c$ for all other resonances, and for 2.5 &lt; $y$ &lt; 4. The cross sections, integrated over $y$ and $p_{\rm T}$, and assuming unpolarized quarkonia, are $\sigma_{\text{J}/\psi} = 8.98 \pm 0.04 \pm 0.82$ $\mu$b, $\sigma_{\psi\text{(2S)}} = 1.23 \pm 0.08 \pm 0.22$ $\mu$b, $\sigma_{\Upsilon\text{(1S)}} = 71 \pm 6 \pm 7$ nb, $\sigma_{\Upsilon\text{(2S)}} = 26 \pm 5 \pm 4$ nb and $\sigma_{\Upsilon\text{(3S)}} = 9 \pm 4 \pm 1$ nb, where the first uncertainty is statistical and the second one is systematic. These values agree, within at most 1.4\sigma, with measurements performed by the LHCb collaboration in the same rapidity range.
DOI: 10.17182/hepdata.72936.v1/t14
title: "Table 14" of "Inclusive quarkonium production at forward rapidity in pp collisions at $\sqrt{s}=8$ TeV"

description: $\psi$(2S) over J/$\psi$ ratio as a function of rapidity.
description: CERN-LHC. We report on the inclusive production cross sections of J/$\psi$, $\psi$(2S), $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S), measured at forward rapidity with the ALICE detector in pp collisions at a center-of-mass energy $\sqrt{s} = 8$ TeV. The analysis is based on data collected at the LHC and corresponds to an integrated luminosity of 1.23 pb$^{-1}$. Quarkonia are reconstructed in the dimuon-decay channel. The differential production cross sections are measured as a function of the transverse momentum $p_{\rm T}$ and rapidity $y$, over the $p_{\rm T}$ ranges 0 &lt; $p_{\rm T}$ &lt; 20 GeV/$c$ for J/$\psi$, 0 &lt; $p_{\rm T}$ &lt; 12 GeV/$c$ for all other resonances, and for 2.5 &lt; $y$ &lt; 4. The cross sections, integrated over $y$ and $p_{\rm T}$, and assuming unpolarized quarkonia, are $\sigma_{\text{J}/\psi} = 8.98 \pm 0.04 \pm 0.82$ $\mu$b, $\sigma_{\psi\text{(2S)}} = 1.23 \pm 0.08 \pm 0.22$ $\mu$b, $\sigma_{\Upsilon\text{(1S)}} = 71 \pm 6 \pm 7$ nb, $\sigma_{\Upsilon\text{(2S)}} = 26 \pm 5 \pm 4$ nb and $\sigma_{\Upsilon\text{(3S)}} = 9 \pm 4 \pm 1$ nb, where the first uncertainty is statistical and the second one is systematic. These values agree, within at most 1.4\sigma, with measurements performed by the LHCb collaboration in the same rapidity range.
DOI: 10.17182/hepdata.72936.v1/t15
title: "Table 15" of "Inclusive quarkonium production at forward rapidity in pp collisions at $\sqrt{s}=8$ TeV"

description: integrated $\psi$(2S) over J/$\psi$ production cross section ratio.
description: CERN-LHC. We report on the inclusive production cross sections of J/$\psi$, $\psi$(2S), $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S), measured at forward rapidity with the ALICE detector in pp collisions at a center-of-mass energy $\sqrt{s} = 8$ TeV. The analysis is based on data collected at the LHC and corresponds to an integrated luminosity of 1.23 pb$^{-1}$. Quarkonia are reconstructed in the dimuon-decay channel. The differential production cross sections are measured as a function of the transverse momentum $p_{\rm T}$ and rapidity $y$, over the $p_{\rm T}$ ranges 0 &lt; $p_{\rm T}$ &lt; 20 GeV/$c$ for J/$\psi$, 0 &lt; $p_{\rm T}$ &lt; 12 GeV/$c$ for all other resonances, and for 2.5 &lt; $y$ &lt; 4. The cross sections, integrated over $y$ and $p_{\rm T}$, and assuming unpolarized quarkonia, are $\sigma_{\text{J}/\psi} = 8.98 \pm 0.04 \pm 0.82$ $\mu$b, $\sigma_{\psi\text{(2S)}} = 1.23 \pm 0.08 \pm 0.22$ $\mu$b, $\sigma_{\Upsilon\text{(1S)}} = 71 \pm 6 \pm 7$ nb, $\sigma_{\Upsilon\text{(2S)}} = 26 \pm 5 \pm 4$ nb and $\sigma_{\Upsilon\text{(3S)}} = 9 \pm 4 \pm 1$ nb, where the first uncertainty is statistical and the second one is systematic. These values agree, within at most 1.4\sigma, with measurements performed by the LHCb collaboration in the same rapidity range.
DOI: 10.17182/hepdata.72936.v1/t16
title: "Table 16" of "Inclusive quarkonium production at forward rapidity in pp collisions at $\sqrt{s}=8$ TeV"

description: integrated $\Upsilon$(2S) over $\Upsilon$(1S) production cross section ratio.
description: CERN-LHC. We report on the inclusive production cross sections of J/$\psi$, $\psi$(2S), $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S), measured at forward rapidity with the ALICE detector in pp collisions at a center-of-mass energy $\sqrt{s} = 8$ TeV. The analysis is based on data collected at the LHC and corresponds to an integrated luminosity of 1.23 pb$^{-1}$. Quarkonia are reconstructed in the dimuon-decay channel. The differential production cross sections are measured as a function of the transverse momentum $p_{\rm T}$ and rapidity $y$, over the $p_{\rm T}$ ranges 0 &lt; $p_{\rm T}$ &lt; 20 GeV/$c$ for J/$\psi$, 0 &lt; $p_{\rm T}$ &lt; 12 GeV/$c$ for all other resonances, and for 2.5 &lt; $y$ &lt; 4. The cross sections, integrated over $y$ and $p_{\rm T}$, and assuming unpolarized quarkonia, are $\sigma_{\text{J}/\psi} = 8.98 \pm 0.04 \pm 0.82$ $\mu$b, $\sigma_{\psi\text{(2S)}} = 1.23 \pm 0.08 \pm 0.22$ $\mu$b, $\sigma_{\Upsilon\text{(1S)}} = 71 \pm 6 \pm 7$ nb, $\sigma_{\Upsilon\text{(2S)}} = 26 \pm 5 \pm 4$ nb and $\sigma_{\Upsilon\text{(3S)}} = 9 \pm 4 \pm 1$ nb, where the first uncertainty is statistical and the second one is systematic. These values agree, within at most 1.4\sigma, with measurements performed by the LHCb collaboration in the same rapidity range.
DOI: 10.17182/hepdata.72936.v1/t17
title: "Table 17" of "Inclusive quarkonium production at forward rapidity in pp collisions at $\sqrt{s}=8$ TeV"

description: integrated $\Upsilon$(3S) over $\Upsilon$(1S) production cross section ratio.
description: CERN-LHC. We report on the inclusive production cross sections of J/$\psi$, $\psi$(2S), $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S), measured at forward rapidity with the ALICE detector in pp collisions at a center-of-mass energy $\sqrt{s} = 8$ TeV. The analysis is based on data collected at the LHC and corresponds to an integrated luminosity of 1.23 pb$^{-1}$. Quarkonia are reconstructed in the dimuon-decay channel. The differential production cross sections are measured as a function of the transverse momentum $p_{\rm T}$ and rapidity $y$, over the $p_{\rm T}$ ranges 0 &lt; $p_{\rm T}$ &lt; 20 GeV/$c$ for J/$\psi$, 0 &lt; $p_{\rm T}$ &lt; 12 GeV/$c$ for all other resonances, and for 2.5 &lt; $y$ &lt; 4. The cross sections, integrated over $y$ and $p_{\rm T}$, and assuming unpolarized quarkonia, are $\sigma_{\text{J}/\psi} = 8.98 \pm 0.04 \pm 0.82$ $\mu$b, $\sigma_{\psi\text{(2S)}} = 1.23 \pm 0.08 \pm 0.22$ $\mu$b, $\sigma_{\Upsilon\text{(1S)}} = 71 \pm 6 \pm 7$ nb, $\sigma_{\Upsilon\text{(2S)}} = 26 \pm 5 \pm 4$ nb and $\sigma_{\Upsilon\text{(3S)}} = 9 \pm 4 \pm 1$ nb, where the first uncertainty is statistical and the second one is systematic. These values agree, within at most 1.4\sigma, with measurements performed by the LHCb collaboration in the same rapidity range.
DOI: 10.17182/hepdata.72937.v1/t1
title: "Table 1" of "Multipion Bose-Einstein correlations in pp, p-Pb, and Pb-Pb collisions at the LHC"

description: Mixed charge (- - - +) C4QS, a4QS, c4QS at low KT4 in pp collisions projected against Q4.
description: CERN-LHC. Three- and four-pion Bose-Einstein correlations are presented in pp, p-Pb, and Pb-Pb collisions at the LHC. We compare our measured four-pion correlations to the expectation derived from two- and three-pion measurements. Such a comparison provides a method to search for coherent pion emission. We also present mixed-charge correlations in order to demonstrate the effectiveness of several analysis procedures such as Coulomb corrections. Same-charge four-pion correlations in pp and p-Pb appear consistent with the expectations from three-pion measurements. However, the presence of non-negligible background correlations in both systems prevent a conclusive statement. In Pb-Pb collisions, we observe a significant suppression of three- and four-pion Bose-Einstein correlations compared to expectations from two-pion measurements. There appears to be no centrality dependence of the suppression within the 0-50% centrality interval. The origin of the suppression is not clear. However, by postulating either coherent pion emission or large multibody Coulomb effects, the suppression may be explained.
DOI: 10.17182/hepdata.72937.v1/t2
title: "Table 2" of "Multipion Bose-Einstein correlations in pp, p-Pb, and Pb-Pb collisions at the LHC"

description: Mixed charge (- - - +) C4QS, a4QS, c4QS at high KT4 in pp collisions projected against Q4.
description: CERN-LHC. Three- and four-pion Bose-Einstein correlations are presented in pp, p-Pb, and Pb-Pb collisions at the LHC. We compare our measured four-pion correlations to the expectation derived from two- and three-pion measurements. Such a comparison provides a method to search for coherent pion emission. We also present mixed-charge correlations in order to demonstrate the effectiveness of several analysis procedures such as Coulomb corrections. Same-charge four-pion correlations in pp and p-Pb appear consistent with the expectations from three-pion measurements. However, the presence of non-negligible background correlations in both systems prevent a conclusive statement. In Pb-Pb collisions, we observe a significant suppression of three- and four-pion Bose-Einstein correlations compared to expectations from two-pion measurements. There appears to be no centrality dependence of the suppression within the 0-50% centrality interval. The origin of the suppression is not clear. However, by postulating either coherent pion emission or large multibody Coulomb effects, the suppression may be explained.
DOI: 10.17182/hepdata.72937.v1/t3
title: "Table 3" of "Multipion Bose-Einstein correlations in pp, p-Pb, and Pb-Pb collisions at the LHC"

description: Mixed charge (- - - +) C4QS, a4QS, c4QS at low KT4 in pPb collisions projected against Q4.
description: CERN-LHC. Three- and four-pion Bose-Einstein correlations are presented in pp, p-Pb, and Pb-Pb collisions at the LHC. We compare our measured four-pion correlations to the expectation derived from two- and three-pion measurements. Such a comparison provides a method to search for coherent pion emission. We also present mixed-charge correlations in order to demonstrate the effectiveness of several analysis procedures such as Coulomb corrections. Same-charge four-pion correlations in pp and p-Pb appear consistent with the expectations from three-pion measurements. However, the presence of non-negligible background correlations in both systems prevent a conclusive statement. In Pb-Pb collisions, we observe a significant suppression of three- and four-pion Bose-Einstein correlations compared to expectations from two-pion measurements. There appears to be no centrality dependence of the suppression within the 0-50% centrality interval. The origin of the suppression is not clear. However, by postulating either coherent pion emission or large multibody Coulomb effects, the suppression may be explained.