cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.146740.v1/t142
title: "Table 71 Covariance" of "Underlying-event studies with strange hadrons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Statistical covariance between bins of Table 71
description: Properties of the underlying-event in $pp$ interactions are investigated primarily via the strange hadrons $K_{S}^{0}$, $\Lambda$ and $\bar\Lambda$, 
as reconstructed using the ATLAS detector at the LHC in minimum-bias $pp$ collision data at $\sqrt{s} = 13$ TeV.
The hadrons are reconstructed via the identification of the displaced two-particle vertices corresponding to the decay modes $K_{S}^{0}\rightarrow\pi^+\pi^-$, 
$\Lambda\rightarrow\pi^-p$ and $\bar\Lambda\rightarrow\pi^+\bar{p}$. 
These are used in the construction of underlying-event observables in azimuthal regions computed relative to the leading charged-particle jet in the event.
Events with a leading charged-particle jet in the range of $10 &lt; p_{T} \leq 40$ GeV are studied using the number of prompt charged particles in the transverse region.
DOI: 10.17182/hepdata.146740.v1/t143
title: "Table 72" of "Underlying-event studies with strange hadrons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Mean-$p_{T}$ of $\Lambda$ and $\bar{\Lambda}$ in the transverse region vs. $N_\textrm{ch,trans}$
description: Properties of the underlying-event in $pp$ interactions are investigated primarily via the strange hadrons $K_{S}^{0}$, $\Lambda$ and $\bar\Lambda$, 
as reconstructed using the ATLAS detector at the LHC in minimum-bias $pp$ collision data at $\sqrt{s} = 13$ TeV.
The hadrons are reconstructed via the identification of the displaced two-particle vertices corresponding to the decay modes $K_{S}^{0}\rightarrow\pi^+\pi^-$, 
$\Lambda\rightarrow\pi^-p$ and $\bar\Lambda\rightarrow\pi^+\bar{p}$. 
These are used in the construction of underlying-event observables in azimuthal regions computed relative to the leading charged-particle jet in the event.
Events with a leading charged-particle jet in the range of $10 &lt; p_{T} \leq 40$ GeV are studied using the number of prompt charged particles in the transverse region.
DOI: 10.17182/hepdata.146740.v1/t144
title: "Table 72 Covariance" of "Underlying-event studies with strange hadrons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Statistical covariance between bins of Table 72
description: Properties of the underlying-event in $pp$ interactions are investigated primarily via the strange hadrons $K_{S}^{0}$, $\Lambda$ and $\bar\Lambda$, 
as reconstructed using the ATLAS detector at the LHC in minimum-bias $pp$ collision data at $\sqrt{s} = 13$ TeV.
The hadrons are reconstructed via the identification of the displaced two-particle vertices corresponding to the decay modes $K_{S}^{0}\rightarrow\pi^+\pi^-$, 
$\Lambda\rightarrow\pi^-p$ and $\bar\Lambda\rightarrow\pi^+\bar{p}$. 
These are used in the construction of underlying-event observables in azimuthal regions computed relative to the leading charged-particle jet in the event.
Events with a leading charged-particle jet in the range of $10 &lt; p_{T} \leq 40$ GeV are studied using the number of prompt charged particles in the transverse region.
DOI: 10.17182/hepdata.146750.v1/t1
title: "Fig. 12, Part 1" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: Charged hadron spectra for centrality selected d+Au collisions.
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t2
title: "Fig. 12, Part 2" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: Charged hadron spectra for centrality selected d+Au collisions.
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t3
title: "Fig. 12, Part 3" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: Charged hadron spectra for centrality selected d+Au collisions.
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t4
title: "Fig. 12, Part 4" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: Charged hadron spectra for centrality selected d+Au collisions.
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t5
title: "Fig. 12, Part 5" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: Charged hadron spectra for centrality selected d+Au collisions.
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t6
title: "Fig. 12, Part 6" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: Charged hadron spectra for centrality selected N+Au collisions. All centralities.
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t10
title: "Fig. 12, Part 10" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: Charged hadron spectra for centrality selected N+Au collisions. Centrality D (Peripheral).
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t11
title: "Fig. 14, Part 1" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: $R_{dAu}$ as a function of $p_T$.
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t12
title: "Fig. 14, Part 2" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: $R_{dAu}$ as a function of $p_T$.
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t13
title: "Fig. 14, Part 3" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: $R_{dAu}$ as a function of $p_T$.
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t7
title: "Fig. 12, Part 7" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: Charged hadron spectra for centrality selected N+Au collisions. Centrality A (Central).
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t8
title: "Fig. 12, Part 8" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: Charged hadron spectra for centrality selected N+Au collisions. Centrality B.
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t9
title: "Fig. 12, Part 9" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: Charged hadron spectra for centrality selected N+Au collisions. Centrality C.
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t14
title: "Fig. 14, Part 4" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: $R_{dAu}$ as a function of $p_T$.
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t15
title: "Fig. 14, Part 5" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: $R_{NAu}$ as a function of $p_T$. Centrality A (Peripheral).
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t16
title: "Fig. 14, Part 6" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: $R_{NAu}$ as a function of $p_T$. Centrality B.
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t17
title: "Fig. 14, Part 7" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: $R_{dAu}$ as a function of $p_T$. Centrality C.
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t18
title: "Fig. 14, Part 8" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: $R_{dAu}$ as a function of $p_T$. Centrality D (Central).
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t19
title: "Fig. 15, Part 1" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: $R_{dAu}$ values averaged in three momentum ranges as functions of $\nu−1$. Horizontal bars show the uncertainty in the value of $\nu$ for each centrality class.
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t20
title: "Fig. 15, Part 2" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: $R_{NAu}$ values averaged in three momentum ranges as functions of $\nu−1$. Horizontal bars show the uncertainty in the value of $\nu$ for each centrality class.
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.
DOI: 10.17182/hepdata.146750.v1/t21
title: "Fig. 16" of "Centrality dependence of charged hadron production in deuteron+gold and nucleon+gold collisions at sqrt(s_NN)=200 GeV"

description: Charged hadron spectra for centrality selected d+Au collisions.
description: We present transverse momentum ($p_T$) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at $\sqrt{s} = 200 \mathrm{GeV}$ for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, $\nu$, suffered by deuteron nucleons. A comparison of charged particle yields to those in $p+p$ collisions show that the yield per nucleon-nucleon collision saturates with $\nu$ for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of $p_T$.