cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.144919.v1/t8
title: "Table2 from Fig 6a" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: '$\overline{\Lambda}$ $D_{LL}$ as a function of $p_{T}$ at $0 &lt; \eta_{\Lambda(\overline{\Lambda})} &lt; 1.2$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t10
title: "Table2 from Fig 6b upper sub-panel" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: 'Two-year-combined $\overline{\Lambda}$ $D_{LL}$ as a function of $p_{T}$ at $0 &lt; \eta_{\Lambda(\overline{\Lambda})} &lt; 1.2$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t11
title: "Table3 from Fig 6b lower sub-panel" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: 'Two-year-combined $\Lambda+\overline{\Lambda}$ $D_{LL}$ as a function of $p_{T}$ at $0 &lt; \eta_{\Lambda(\overline{\Lambda})} &lt; 1.2$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t12
title: "Table1 from Fig 6c" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: 'Two-year-combined $\Lambda$ $D_{LL}$ as a function of $p_{T}$ at $-1.2 &lt; \eta_{\Lambda(\overline{\Lambda})} &lt; 0$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t13
title: "Table2 from Fig 6c" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: 'Two-year-combined $\overline{\Lambda}$ $D_{LL}$ as a function of $p_{T}$ at $-1.2 &lt; \eta_{\Lambda(\overline{\Lambda})} &lt; 0$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t14
title: "Table1 from Fig 7a" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: '$\Lambda$ $D_{LL}$ as a function of z at $0 &lt; \eta_{jet} &lt; 1.0$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t15
title: "Table2 from Fig 7a" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: '$\overline{\Lambda}$ $D_{LL}$ as a function of z at $0 &lt; \eta_{jet} &lt; 1.0$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t16
title: "Table1 from Fig 7b" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: '$\Lambda$ $D_{LL}$ as a function of z at $-1.0 &lt; \eta_{jet} &lt; 0$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t9
title: "Table1 from Fig 6b upper sub-panel" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: 'Two-year-combined $\Lambda$ $D_{LL}$ as a function of $p_{T}$ at $0 &lt; \eta_{\Lambda(\overline{\Lambda})} &lt; 1.2$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t17
title: "Table2 from Fig 7b" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: '$\overline{\Lambda}$ $D_{LL}$ as a function of z at $-1.0 &lt; \eta_{jet} &lt; 0$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t18
title: "Table1 from Fig 7c" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: 'particle jet pt as a function of $\Lambda$ z'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t19
title: "Table2 from Fig 7c" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: 'particle jet pt as a function of $\overline{\Lambda}$ z'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t20
title: "Table1 from Fig 8a" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: '$\Lambda$ $D_{TT}$ as a function of $p_{T}$ at $0 &lt; \eta_{\Lambda(\overline{\Lambda})} &lt; 1.2$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t21
title: "Table2 from Fig 8a" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: '$\overline{\Lambda}$ $D_{TT}$ as a function of $p_{T}$ at $0 &lt; \eta_{\Lambda(\overline{\Lambda})} &lt; 1.2$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t22
title: "Table1 from Fig 8b" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: '$\Lambda$ $D_{TT}$ as a function of $p_{T}$ at $-1.2 &lt; \eta_{\Lambda(\overline{\Lambda})} &lt; 0$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t23
title: "Table2 from Fig 8b" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: '$\overline{\Lambda}$ $D_{TT}$ as a function of $p_{T}$ at $-1.2 &lt; \eta_{\Lambda(\overline{\Lambda})} &lt; 0$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t24
title: "Table1 from Fig 9a" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: '$\Lambda$ $D_{TT}$ as a function of $p_{T}$ at $0 &lt; \eta_{\Lambda(\overline{\Lambda})} &lt; 1.2$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t25
title: "Table2 from Fig 9a" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: '$\overline{\Lambda}$ $D_{TT}$ as a function of $p_{T}$ at $0 &lt; \eta_{\Lambda(\overline{\Lambda})} &lt; 1.2$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t26
title: "Table1 from Fig 9b" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: 'Two-year-combined $\Lambda$ $D_{TT}$ as a function of $p_{T}$ at $0 &lt; \eta_{\Lambda(\overline{\Lambda})} &lt; 1.2$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t27
title: "Table2 from Fig 9b" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: 'Two-year-combined $\overline{\Lambda}$ $D_{TT}$ as a function of $p_{T}$ at $0 &lt; \eta_{\Lambda(\overline{\Lambda})} &lt; 1.2$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t28
title: "Table1 from Fig 9c" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: 'Two-year-combined $\Lambda$ $D_{TT}$ as a function of $p_{T}$ at $-1.2 &lt; \eta_{\Lambda(\overline{\Lambda})} &lt; 0$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t29
title: "Table2 from Fig 9c" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: 'Two-year-combined $\overline{\Lambda}$ $D_{TT}$ as a function of $p_{T}$ at $-1.2 &lt; \eta_{\Lambda(\overline{\Lambda})} &lt; 0$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t30
title: "Table1 from Fig 10a" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: '$\Lambda$ $D_{TT}$ as a function of z at $0 &lt; \eta_{jet} &lt; 1.0$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t31
title: "Table2 from Fig 10a" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: '$\overline{\Lambda}$ $D_{TT}$ as a function of z at $0 &lt; \eta_{jet} &lt; 1.0$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t32
title: "Table1 from Fig 10b" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: '$\Lambda$ $D_{TT}$ as a function of z at $-1.0 &lt; \eta_{jet} &lt; 0$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t33
title: "Table2 from Fig 10b" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: '$\overline{\Lambda}$ $D_{TT}$ as a function of z at $-1.0 &lt; \eta_{jet} &lt; 0$'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t34
title: "Table1 from Fig 10c" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: 'particle jet pt as a function of $\Lambda$ z'
description: No data abstract available.
DOI: 10.17182/hepdata.144919.v1/t35
title: "Table2 from Fig 10c" of "Longitudinal and transverse spin transfer to $\Lambda$ and $\overline{\Lambda}$ hyperons in polarized $p$+$p$ collisions at $\sqrt{s} = 200$ GeV"

description: 'particle jet pt as a function of $\overline{\Lambda}$ z'
description: No data abstract available.
DOI: 10.17182/hepdata.144920.v1/t1
title: "Figure 7" of "Results on Elastic Cross Sections in Proton-Proton Collisions at $\sqrt{s} = 510$ GeV with the STAR Detector at RHIC"

description: Top panel: The $pp$ elastic differential cross section $d\sigma/dt$ fitted with an exponential $A e^{-B(t)|t|}$. Bottom panel: Residuals (Data - Fit)/Error. Uncertainties on the data points are smaller than the symbol size. The vertical scale uncertainty of 2.5% is not included in in the full error.
description: We report results on an elastic cross section measurement in proton--proton collisions at a center-of-mass energy $\sqrt{s}=510$ GeV, obtained with the Roman Pot setup of the STAR experiment at the Relativistic Heavy Ion Collider (RHIC).The elastic differential cross section is measured in the four-momentum transfer squared range $0.23 \leq -t \leq 0.67$ GeV$^2$. This is the only measurement of the proton-proton elastic cross section in this $t$ range for collision energies above the Intersecting Storage Rings (ISR) and below the Large Hadron Collider (LHC) colliders.We find that a constant slope $B$ does not fit the data in the aforementioned $t$ range, and we obtain a much better fit using a second-order polynomial for $B(t)$. This is the first measurement below the LHC energies for which the non-constant behavior $B(t)$ is observed. The $t$ dependence of $B$ is determined using six subintervals of $t$ in the STAR measured $t$ range, and is in good agreement with the phenomenological models. The measured elastic differential cross section $\mathrm{d}\sigma/\mathrm{dt}$ agrees well with the results obtained at $\sqrt{s} = 540$ GeV for proton--antiproton collisions by the UA4 experiment. We also determine that the integrated elastic cross section within the STAR $t$-range is $\sigma^\mathrm{fid}_\mathrm{el} = 462.1 \pm 0.9 (\mathrm{stat.}) \pm 1.1 (\mathrm {syst.}) \pm 11.6 (\mathrm {scale})$ $\mu\mathrm{b}$.
DOI: 10.17182/hepdata.144920.v1/t2
title: "Results Summary" of "Results on Elastic Cross Sections in Proton-Proton Collisions at $\sqrt{s} = 510$ GeV with the STAR Detector at RHIC"

description: Results of the exponential function $A e^{-B(t)|t|}$ fit to the elastic differential cross section data as well as the integrated fiducial cross section are listed. Also listed are the corresponding values of the statistical and systematic uncertainties. The scale (luminosity and trigger efficiency) uncertainty of 2.5% applicable to the fit parameter $A$ and fiducial cross section $\sigma^\mathrm{fid}_\mathrm{el}$ is not included in the full error.
description: We report results on an elastic cross section measurement in proton--proton collisions at a center-of-mass energy $\sqrt{s}=510$ GeV, obtained with the Roman Pot setup of the STAR experiment at the Relativistic Heavy Ion Collider (RHIC).The elastic differential cross section is measured in the four-momentum transfer squared range $0.23 \leq -t \leq 0.67$ GeV$^2$. This is the only measurement of the proton-proton elastic cross section in this $t$ range for collision energies above the Intersecting Storage Rings (ISR) and below the Large Hadron Collider (LHC) colliders.We find that a constant slope $B$ does not fit the data in the aforementioned $t$ range, and we obtain a much better fit using a second-order polynomial for $B(t)$. This is the first measurement below the LHC energies for which the non-constant behavior $B(t)$ is observed. The $t$ dependence of $B$ is determined using six subintervals of $t$ in the STAR measured $t$ range, and is in good agreement with the phenomenological models. The measured elastic differential cross section $\mathrm{d}\sigma/\mathrm{dt}$ agrees well with the results obtained at $\sqrt{s} = 540$ GeV for proton--antiproton collisions by the UA4 experiment. We also determine that the integrated elastic cross section within the STAR $t$-range is $\sigma^\mathrm{fid}_\mathrm{el} = 462.1 \pm 0.9 (\mathrm{stat.}) \pm 1.1 (\mathrm {syst.}) \pm 11.6 (\mathrm {scale})$ $\mu\mathrm{b}$.
DOI: 10.17182/hepdata.145071.v1/t1
title: "Table 1" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Summary of results for cross-section of prompt $J/\psi$ decaying to a muon pair for 13 TeV data in fb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
DOI: 10.17182/hepdata.145071.v1/t2
title: "Table 2" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Summary of results for cross-section of non-prompt $J/\psi$ decaying to a muon pair for 13 TeV data in fb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
DOI: 10.17182/hepdata.145071.v1/t3
title: "Table 3" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Summary of results for cross-section of prompt $\psi(2S)$ decaying to a muon pair for 13 TeV data in fb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
DOI: 10.17182/hepdata.145071.v1/t4
title: "Table 4" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Summary of results for cross-section of non-prompt $\psi(2S)$ decaying to a muon pair for 13 TeV data in fb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
DOI: 10.17182/hepdata.145071.v1/t5
title: "Table 5" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Summary of results for non-prompt fraction of $J/\psi$ decaying to a muon pair as a percentage for 13 TeV data. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
DOI: 10.17182/hepdata.145071.v1/t6
title: "Table 6" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Summary of results for non-prompt fraction of $\psi(2S)$ decaying to a muon pair as a percentage for 13 TeV data. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
DOI: 10.17182/hepdata.145071.v1/t7
title: "Table 7" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Summary of results for prompt $\psi(2S)$ over $J/\psi$ ratio as a percentage for 13 TeV data. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
DOI: 10.17182/hepdata.145071.v1/t8
title: "Table 8" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Summary of results for non-prompt $\psi(2S)$ over $J/\psi$ ratio as a percentage for 13 TeV data. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
DOI: 10.17182/hepdata.145071.v1/t9
title: "Table 9" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Correction factors for an assumed angular dependence $\propto 1+\lambda_{\theta} \cos^2\theta $ in the helicity frame, for several values of the parameter $\lambda_{\theta}$. The correction factors were found to be the same (within 1% - 2%) for $J\psi$ and $\psi(2S)$ mesons, for prompt and non-prompt production mechanisms, and for the three rapidity intervals considered in this paper.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
DOI: 10.17182/hepdata.145071.v2/t1
title: "Table 1" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Summary of results for cross-section of prompt $J/\psi$ decaying to a muon pair for 13 TeV data in fb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.