cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.147284.v1/t3
title: "Table 3" of "Skewness and kurtosis of mean transverse momentum fluctuations at the LHC energies"

description: Standardized skewness of $\langle p_\mathrm{T}\rangle$ as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|&lt;0.5}$ in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV.
description: Measurements of higher-order fluctuations of $\langle p_\mathrm{T}\rangle$ distribution in Pb$-$Pb collisions, Xe$-$Xe collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV and in pp collisions at at $\sqrt{s}$ = 5.02 TeV using the ALICE detector at the CERN LHC. Standardized skewness, intensive skewness and kurtosis of $\langle p_\mathrm{T}\rangle$ are presented as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|&lt;0.5}$ for all the collision systems. The charged particles are selected in the transverse momentum range, 0.2 &lt; $p_\mathrm{T}$ (GeV/c) &lt; 3.0 and pseudorapidity range, $|\eta|$ &lt; 0.8.
DOI: 10.17182/hepdata.147284.v1/t4
title: "Table 4" of "Skewness and kurtosis of mean transverse momentum fluctuations at the LHC energies"

description: Intensive skewness of $\langle p_\mathrm{T}\rangle$ as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|&lt;0.5}$ in pp collisions at $\sqrt{s}$ = 5.02 TeV.
description: Measurements of higher-order fluctuations of $\langle p_\mathrm{T}\rangle$ distribution in Pb$-$Pb collisions, Xe$-$Xe collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV and in pp collisions at at $\sqrt{s}$ = 5.02 TeV using the ALICE detector at the CERN LHC. Standardized skewness, intensive skewness and kurtosis of $\langle p_\mathrm{T}\rangle$ are presented as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|&lt;0.5}$ for all the collision systems. The charged particles are selected in the transverse momentum range, 0.2 &lt; $p_\mathrm{T}$ (GeV/c) &lt; 3.0 and pseudorapidity range, $|\eta|$ &lt; 0.8.
DOI: 10.17182/hepdata.147284.v1/t5
title: "Table 5" of "Skewness and kurtosis of mean transverse momentum fluctuations at the LHC energies"

description: Intensive skewness of $\langle p_\mathrm{T}\rangle$ as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|&lt;0.5}$ in Xe$-$Xe collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV.
description: Measurements of higher-order fluctuations of $\langle p_\mathrm{T}\rangle$ distribution in Pb$-$Pb collisions, Xe$-$Xe collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV and in pp collisions at at $\sqrt{s}$ = 5.02 TeV using the ALICE detector at the CERN LHC. Standardized skewness, intensive skewness and kurtosis of $\langle p_\mathrm{T}\rangle$ are presented as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|&lt;0.5}$ for all the collision systems. The charged particles are selected in the transverse momentum range, 0.2 &lt; $p_\mathrm{T}$ (GeV/c) &lt; 3.0 and pseudorapidity range, $|\eta|$ &lt; 0.8.
DOI: 10.17182/hepdata.147284.v1/t6
title: "Table 6" of "Skewness and kurtosis of mean transverse momentum fluctuations at the LHC energies"

description: Intensive skewness of $\langle p_\mathrm{T}\rangle$ as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|&lt;0.5}$ in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV.
description: Measurements of higher-order fluctuations of $\langle p_\mathrm{T}\rangle$ distribution in Pb$-$Pb collisions, Xe$-$Xe collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV and in pp collisions at at $\sqrt{s}$ = 5.02 TeV using the ALICE detector at the CERN LHC. Standardized skewness, intensive skewness and kurtosis of $\langle p_\mathrm{T}\rangle$ are presented as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|&lt;0.5}$ for all the collision systems. The charged particles are selected in the transverse momentum range, 0.2 &lt; $p_\mathrm{T}$ (GeV/c) &lt; 3.0 and pseudorapidity range, $|\eta|$ &lt; 0.8.
DOI: 10.17182/hepdata.147284.v1/t7
title: "Table 7" of "Skewness and kurtosis of mean transverse momentum fluctuations at the LHC energies"

description: Kurtosis of $\langle p_\mathrm{T}\rangle$ as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|&lt;0.5}$ in pp collisions at $\sqrt{s}$ = 5.02 TeV.
description: Measurements of higher-order fluctuations of $\langle p_\mathrm{T}\rangle$ distribution in Pb$-$Pb collisions, Xe$-$Xe collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV and in pp collisions at at $\sqrt{s}$ = 5.02 TeV using the ALICE detector at the CERN LHC. Standardized skewness, intensive skewness and kurtosis of $\langle p_\mathrm{T}\rangle$ are presented as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|&lt;0.5}$ for all the collision systems. The charged particles are selected in the transverse momentum range, 0.2 &lt; $p_\mathrm{T}$ (GeV/c) &lt; 3.0 and pseudorapidity range, $|\eta|$ &lt; 0.8.
DOI: 10.17182/hepdata.147284.v1/t8
title: "Table 8" of "Skewness and kurtosis of mean transverse momentum fluctuations at the LHC energies"

description: Kurtosis of $\langle p_\mathrm{T}\rangle$ as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|&lt;0.5}$ in Xe$-$Xe collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV.
description: Measurements of higher-order fluctuations of $\langle p_\mathrm{T}\rangle$ distribution in Pb$-$Pb collisions, Xe$-$Xe collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV and in pp collisions at at $\sqrt{s}$ = 5.02 TeV using the ALICE detector at the CERN LHC. Standardized skewness, intensive skewness and kurtosis of $\langle p_\mathrm{T}\rangle$ are presented as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|&lt;0.5}$ for all the collision systems. The charged particles are selected in the transverse momentum range, 0.2 &lt; $p_\mathrm{T}$ (GeV/c) &lt; 3.0 and pseudorapidity range, $|\eta|$ &lt; 0.8.
DOI: 10.17182/hepdata.147284.v1/t9
title: "Table 9" of "Skewness and kurtosis of mean transverse momentum fluctuations at the LHC energies"

description: Kurtosis of $\langle p_\mathrm{T}\rangle$ as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|&lt;0.5}$ in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV.
description: Measurements of higher-order fluctuations of $\langle p_\mathrm{T}\rangle$ distribution in Pb$-$Pb collisions, Xe$-$Xe collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV and in pp collisions at at $\sqrt{s}$ = 5.02 TeV using the ALICE detector at the CERN LHC. Standardized skewness, intensive skewness and kurtosis of $\langle p_\mathrm{T}\rangle$ are presented as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|&lt;0.5}$ for all the collision systems. The charged particles are selected in the transverse momentum range, 0.2 &lt; $p_\mathrm{T}$ (GeV/c) &lt; 3.0 and pseudorapidity range, $|\eta|$ &lt; 0.8.
DOI: 10.17182/hepdata.145640.v1/t1
title: "Figure 3 non-prompt D0 pp 13 TeV" of "Study of flavor dependence of the baryon-to-meson ratio in proton-proton collisions at $\sqrt{s} = 13$ TeV"

description: $p_{\mathrm{T}}$-differential D$^{0}$ production cross section in pp collisions at $\sqrt{s}$ = 13 TeV
description: No data abstract available.
DOI: 10.17182/hepdata.145640.v1/t2
title: "Figure 3 non-prompt Lc pp 13 TeV" of "Study of flavor dependence of the baryon-to-meson ratio in proton-proton collisions at $\sqrt{s} = 13$ TeV"

description: $p_{\mathrm{T}}$-differential $\Lambda_\mathrm{c}^{+}$ production cross section in pp collisions at $\sqrt{s}$ = 13 TeV
description: No data abstract available.
DOI: 10.17182/hepdata.145640.v1/t3
title: "Figure 5 non-prompt Lc over non-prompt D0 pp 13 TeV" of "Study of flavor dependence of the baryon-to-meson ratio in proton-proton collisions at $\sqrt{s} = 13$ TeV"

description: $p_{\mathrm{T}}$-differential non-prompt $\Lambda_\mathrm{c}^{+}$/non-prompt D$^{0}$ ratio in pp collisions at $\sqrt{s}$ = 13 TeV
description: No data abstract available.
DOI: 10.17182/hepdata.153919.v1/t1
title: "Figure 1 (top)" of "Multiplicity dependence of charged-particle intra-jet properties in pp collisions at $\sqrt{s}$ = 13 TeV"

description: Mean number of charged particles ($\langle N_{\mathrm{ch}} \rangle$) within leading charged-particle jets as a function of $p_{T}^{\mathrm{jet, ch}}$ for minimum-bias (MB) pp collisions.
description: The first measurement of the multiplicity dependence of intra-jet properties of leading charged-particle jets in proton-proton (pp) collisions is reported. The mean charged-particle multiplicity and jet fragmentation distributions are measured in minimum-bias and high-multiplicity pp collisions at center-of-mass energy $\sqrt{s}$ = 13 TeV using the ALICE detector. Jets are reconstructed from charged particles produced in the midrapidity region ($|\eta| &lt; 0.9$) using the sequential recombination anti-$k_{\rm T}$ algorithm with jet resolution parameters $R$ = 0.2, 0.3, and 0.4 for the transverse momentum ($p_{\rm T}$) interval 5$-$110 GeV/$c$. The high-multiplicity events are selected by the forward V0 scintillator detectors. The mean charged-particle multiplicity inside the leading jet cone rises monotonically with increasing jet $p_{\rm T}$ in qualitative agreement with previous measurements at lower energies. The distributions of jet fragmentation function variables $z^{\rm ch}$ and $\xi^{\rm ch}$ are measured for different jet-$p_{\rm T}$ intervals. Jet-$p_{\rm T}$ independent fragmentation of leading jets is observed for wider jets except at high- and low-$z^{\rm ch}$ values. The observed ``hump-backed plateau'' structure in the $\xi^{\rm ch}$ distribution indicates suppression of low-$p_{\rm T}$ particles. In high-multiplicity events, an enhancement of the fragmentation probability of low-$z^{\rm ch}$ particles accompanied by a suppression of high-$z^{\rm ch}$ particles is observed compared to minimum-bias events. This behavior becomes more prominent for low-$p_{\rm T}$ jets with larger jet radius. The results are compared with predictions of QCD-inspired event generators, PYTHIA 8 with Monash 2013 tune and EPOS LHC. It is found that PYTHIA 8 qualitatively reproduces the jet modification in high-multiplicity events except at high jet $p_{\rm T}$. These measurements provide important constraints to models of jet fragmentation.
DOI: 10.17182/hepdata.153919.v1/t2
title: "Figure 1 (bottom)" of "Multiplicity dependence of charged-particle intra-jet properties in pp collisions at $\sqrt{s}$ = 13 TeV"

description: Mean number of charged particles ($\langle N_{\mathrm{ch}} \rangle$) within leading charged-particle jets as a function of $p_{T}^{\mathrm{jet, ch}}$ for high-multiplicity (HM) pp collisions.
description: The first measurement of the multiplicity dependence of intra-jet properties of leading charged-particle jets in proton-proton (pp) collisions is reported. The mean charged-particle multiplicity and jet fragmentation distributions are measured in minimum-bias and high-multiplicity pp collisions at center-of-mass energy $\sqrt{s}$ = 13 TeV using the ALICE detector. Jets are reconstructed from charged particles produced in the midrapidity region ($|\eta| &lt; 0.9$) using the sequential recombination anti-$k_{\rm T}$ algorithm with jet resolution parameters $R$ = 0.2, 0.3, and 0.4 for the transverse momentum ($p_{\rm T}$) interval 5$-$110 GeV/$c$. The high-multiplicity events are selected by the forward V0 scintillator detectors. The mean charged-particle multiplicity inside the leading jet cone rises monotonically with increasing jet $p_{\rm T}$ in qualitative agreement with previous measurements at lower energies. The distributions of jet fragmentation function variables $z^{\rm ch}$ and $\xi^{\rm ch}$ are measured for different jet-$p_{\rm T}$ intervals. Jet-$p_{\rm T}$ independent fragmentation of leading jets is observed for wider jets except at high- and low-$z^{\rm ch}$ values. The observed ``hump-backed plateau'' structure in the $\xi^{\rm ch}$ distribution indicates suppression of low-$p_{\rm T}$ particles. In high-multiplicity events, an enhancement of the fragmentation probability of low-$z^{\rm ch}$ particles accompanied by a suppression of high-$z^{\rm ch}$ particles is observed compared to minimum-bias events. This behavior becomes more prominent for low-$p_{\rm T}$ jets with larger jet radius. The results are compared with predictions of QCD-inspired event generators, PYTHIA 8 with Monash 2013 tune and EPOS LHC. It is found that PYTHIA 8 qualitatively reproduces the jet modification in high-multiplicity events except at high jet $p_{\rm T}$. These measurements provide important constraints to models of jet fragmentation.
DOI: 10.17182/hepdata.153919.v1/t3
title: "Figure 2" of "Multiplicity dependence of charged-particle intra-jet properties in pp collisions at $\sqrt{s}$ = 13 TeV"

description: The ratio of $\langle N_{\mathrm{ch}} \rangle$ between high-multiplicity (HM) and minimum-bias (MB) events as a function of $p_{T}^{\mathrm{jet, ch}}$ for pp collisions.
description: The first measurement of the multiplicity dependence of intra-jet properties of leading charged-particle jets in proton-proton (pp) collisions is reported. The mean charged-particle multiplicity and jet fragmentation distributions are measured in minimum-bias and high-multiplicity pp collisions at center-of-mass energy $\sqrt{s}$ = 13 TeV using the ALICE detector. Jets are reconstructed from charged particles produced in the midrapidity region ($|\eta| &lt; 0.9$) using the sequential recombination anti-$k_{\rm T}$ algorithm with jet resolution parameters $R$ = 0.2, 0.3, and 0.4 for the transverse momentum ($p_{\rm T}$) interval 5$-$110 GeV/$c$. The high-multiplicity events are selected by the forward V0 scintillator detectors. The mean charged-particle multiplicity inside the leading jet cone rises monotonically with increasing jet $p_{\rm T}$ in qualitative agreement with previous measurements at lower energies. The distributions of jet fragmentation function variables $z^{\rm ch}$ and $\xi^{\rm ch}$ are measured for different jet-$p_{\rm T}$ intervals. Jet-$p_{\rm T}$ independent fragmentation of leading jets is observed for wider jets except at high- and low-$z^{\rm ch}$ values. The observed ``hump-backed plateau'' structure in the $\xi^{\rm ch}$ distribution indicates suppression of low-$p_{\rm T}$ particles. In high-multiplicity events, an enhancement of the fragmentation probability of low-$z^{\rm ch}$ particles accompanied by a suppression of high-$z^{\rm ch}$ particles is observed compared to minimum-bias events. This behavior becomes more prominent for low-$p_{\rm T}$ jets with larger jet radius. The results are compared with predictions of QCD-inspired event generators, PYTHIA 8 with Monash 2013 tune and EPOS LHC. It is found that PYTHIA 8 qualitatively reproduces the jet modification in high-multiplicity events except at high jet $p_{\rm T}$. These measurements provide important constraints to models of jet fragmentation.
DOI: 10.17182/hepdata.153919.v1/t4
title: "Figure 3 (top left)" of "Multiplicity dependence of charged-particle intra-jet properties in pp collisions at $\sqrt{s}$ = 13 TeV"

description: $z^{\mathrm{ch}}$ distributions in leading jets for different $p_{T}^{\mathrm{jet, ch}}$ intervals in minimum-bias (MB) pp collisions for jet resolution parameter ($R$) = 0.2.
description: The first measurement of the multiplicity dependence of intra-jet properties of leading charged-particle jets in proton-proton (pp) collisions is reported. The mean charged-particle multiplicity and jet fragmentation distributions are measured in minimum-bias and high-multiplicity pp collisions at center-of-mass energy $\sqrt{s}$ = 13 TeV using the ALICE detector. Jets are reconstructed from charged particles produced in the midrapidity region ($|\eta| &lt; 0.9$) using the sequential recombination anti-$k_{\rm T}$ algorithm with jet resolution parameters $R$ = 0.2, 0.3, and 0.4 for the transverse momentum ($p_{\rm T}$) interval 5$-$110 GeV/$c$. The high-multiplicity events are selected by the forward V0 scintillator detectors. The mean charged-particle multiplicity inside the leading jet cone rises monotonically with increasing jet $p_{\rm T}$ in qualitative agreement with previous measurements at lower energies. The distributions of jet fragmentation function variables $z^{\rm ch}$ and $\xi^{\rm ch}$ are measured for different jet-$p_{\rm T}$ intervals. Jet-$p_{\rm T}$ independent fragmentation of leading jets is observed for wider jets except at high- and low-$z^{\rm ch}$ values. The observed ``hump-backed plateau'' structure in the $\xi^{\rm ch}$ distribution indicates suppression of low-$p_{\rm T}$ particles. In high-multiplicity events, an enhancement of the fragmentation probability of low-$z^{\rm ch}$ particles accompanied by a suppression of high-$z^{\rm ch}$ particles is observed compared to minimum-bias events. This behavior becomes more prominent for low-$p_{\rm T}$ jets with larger jet radius. The results are compared with predictions of QCD-inspired event generators, PYTHIA 8 with Monash 2013 tune and EPOS LHC. It is found that PYTHIA 8 qualitatively reproduces the jet modification in high-multiplicity events except at high jet $p_{\rm T}$. These measurements provide important constraints to models of jet fragmentation.
DOI: 10.17182/hepdata.153919.v1/t5
title: "Figure 3 (top middle)" of "Multiplicity dependence of charged-particle intra-jet properties in pp collisions at $\sqrt{s}$ = 13 TeV"

description: $z^{\mathrm{ch}}$ distributions in leading jets for different $p_{T}^{\mathrm{jet, ch}}$ intervals in minimum-bias (MB) pp collisions for jet resolution parameter ($R$) = 0.3.
description: The first measurement of the multiplicity dependence of intra-jet properties of leading charged-particle jets in proton-proton (pp) collisions is reported. The mean charged-particle multiplicity and jet fragmentation distributions are measured in minimum-bias and high-multiplicity pp collisions at center-of-mass energy $\sqrt{s}$ = 13 TeV using the ALICE detector. Jets are reconstructed from charged particles produced in the midrapidity region ($|\eta| &lt; 0.9$) using the sequential recombination anti-$k_{\rm T}$ algorithm with jet resolution parameters $R$ = 0.2, 0.3, and 0.4 for the transverse momentum ($p_{\rm T}$) interval 5$-$110 GeV/$c$. The high-multiplicity events are selected by the forward V0 scintillator detectors. The mean charged-particle multiplicity inside the leading jet cone rises monotonically with increasing jet $p_{\rm T}$ in qualitative agreement with previous measurements at lower energies. The distributions of jet fragmentation function variables $z^{\rm ch}$ and $\xi^{\rm ch}$ are measured for different jet-$p_{\rm T}$ intervals. Jet-$p_{\rm T}$ independent fragmentation of leading jets is observed for wider jets except at high- and low-$z^{\rm ch}$ values. The observed ``hump-backed plateau'' structure in the $\xi^{\rm ch}$ distribution indicates suppression of low-$p_{\rm T}$ particles. In high-multiplicity events, an enhancement of the fragmentation probability of low-$z^{\rm ch}$ particles accompanied by a suppression of high-$z^{\rm ch}$ particles is observed compared to minimum-bias events. This behavior becomes more prominent for low-$p_{\rm T}$ jets with larger jet radius. The results are compared with predictions of QCD-inspired event generators, PYTHIA 8 with Monash 2013 tune and EPOS LHC. It is found that PYTHIA 8 qualitatively reproduces the jet modification in high-multiplicity events except at high jet $p_{\rm T}$. These measurements provide important constraints to models of jet fragmentation.
DOI: 10.17182/hepdata.153919.v1/t10
title: "Figure 5 (top)" of "Multiplicity dependence of charged-particle intra-jet properties in pp collisions at $\sqrt{s}$ = 13 TeV"

description: The ratio of $z^{\mathrm{ch}}$ distributions for $10 &lt; p_{\mathrm{T}}^{\mathrm{jet, ch}} &lt; 20$ GeV/c between high-multiplicity (HM) and minimum-bias (MB) events in pp collisions.
description: The first measurement of the multiplicity dependence of intra-jet properties of leading charged-particle jets in proton-proton (pp) collisions is reported. The mean charged-particle multiplicity and jet fragmentation distributions are measured in minimum-bias and high-multiplicity pp collisions at center-of-mass energy $\sqrt{s}$ = 13 TeV using the ALICE detector. Jets are reconstructed from charged particles produced in the midrapidity region ($|\eta| &lt; 0.9$) using the sequential recombination anti-$k_{\rm T}$ algorithm with jet resolution parameters $R$ = 0.2, 0.3, and 0.4 for the transverse momentum ($p_{\rm T}$) interval 5$-$110 GeV/$c$. The high-multiplicity events are selected by the forward V0 scintillator detectors. The mean charged-particle multiplicity inside the leading jet cone rises monotonically with increasing jet $p_{\rm T}$ in qualitative agreement with previous measurements at lower energies. The distributions of jet fragmentation function variables $z^{\rm ch}$ and $\xi^{\rm ch}$ are measured for different jet-$p_{\rm T}$ intervals. Jet-$p_{\rm T}$ independent fragmentation of leading jets is observed for wider jets except at high- and low-$z^{\rm ch}$ values. The observed ``hump-backed plateau'' structure in the $\xi^{\rm ch}$ distribution indicates suppression of low-$p_{\rm T}$ particles. In high-multiplicity events, an enhancement of the fragmentation probability of low-$z^{\rm ch}$ particles accompanied by a suppression of high-$z^{\rm ch}$ particles is observed compared to minimum-bias events. This behavior becomes more prominent for low-$p_{\rm T}$ jets with larger jet radius. The results are compared with predictions of QCD-inspired event generators, PYTHIA 8 with Monash 2013 tune and EPOS LHC. It is found that PYTHIA 8 qualitatively reproduces the jet modification in high-multiplicity events except at high jet $p_{\rm T}$. These measurements provide important constraints to models of jet fragmentation.