cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.93741.v1/t6
title: "Table 6" of "Multiplicity dependence of (anti-)deuteron production in pp collisions at $\sqrt{s}$ = 7 TeV"

description: Coalescence parameter $B_2$ of (anti-)deuterons vs. the transverse momentum per nucleon in V0M multiplicity class I+II
description: In this letter, the production of deuterons and anti-deuterons in pp collisions at $\sqrt{s}$ = 7 TeV is studied as a function of the charged-particle multiplicity density at mid-rapidity with the ALICE detector at the LHC. Production yields are measured at mid-rapidity in five multiplicity classes and as a function of the deuteron transverse momentum (pT). The measurements are discussed in the context of hadron-coalescence models. The coalescence parameter B2, extracted from the measured spectra of (anti-)deuterons and primary (anti-)protons, exhibits no significant pT-dependence for pT &lt; 3 GeV/c, in agreement with the expectations of a simple coalescence picture. At fixed transverse momentum per nucleon, the B2 parameter is found to decrease smoothly from low multiplicity pp to Pb-Pb collisions, in qualitative agreement with more elaborate coalescence models. The measured mean transverse momentum of (anti-)deuterons in pp is not reproduced by the Blast-Wave model calculations that simultaneously describe pion, kaon and proton spectra, in contrast to central Pb-Pb collisions. The ratio between the pT-integrated yield of deuterons to protons, d/p, is found to increase with the charged-particle multiplicity, as observed in inelastic pp collisions at different centre-of-mass energies. The d/p ratios are reported in a wide range, from the lowest to the highest multiplicity values measured in pp collisions at the LHC.
DOI: 10.17182/hepdata.93741.v1/t8
title: "Table 8" of "Multiplicity dependence of (anti-)deuteron production in pp collisions at $\sqrt{s}$ = 7 TeV"

description: Coalescence parameter $B_2$ of (anti-)deuterons vs. the transverse momentum per nucleon in V0M multiplicity class IV+V
description: In this letter, the production of deuterons and anti-deuterons in pp collisions at $\sqrt{s}$ = 7 TeV is studied as a function of the charged-particle multiplicity density at mid-rapidity with the ALICE detector at the LHC. Production yields are measured at mid-rapidity in five multiplicity classes and as a function of the deuteron transverse momentum (pT). The measurements are discussed in the context of hadron-coalescence models. The coalescence parameter B2, extracted from the measured spectra of (anti-)deuterons and primary (anti-)protons, exhibits no significant pT-dependence for pT &lt; 3 GeV/c, in agreement with the expectations of a simple coalescence picture. At fixed transverse momentum per nucleon, the B2 parameter is found to decrease smoothly from low multiplicity pp to Pb-Pb collisions, in qualitative agreement with more elaborate coalescence models. The measured mean transverse momentum of (anti-)deuterons in pp is not reproduced by the Blast-Wave model calculations that simultaneously describe pion, kaon and proton spectra, in contrast to central Pb-Pb collisions. The ratio between the pT-integrated yield of deuterons to protons, d/p, is found to increase with the charged-particle multiplicity, as observed in inelastic pp collisions at different centre-of-mass energies. The d/p ratios are reported in a wide range, from the lowest to the highest multiplicity values measured in pp collisions at the LHC.
DOI: 10.17182/hepdata.93741.v1/t9
title: "Table 9" of "Multiplicity dependence of (anti-)deuteron production in pp collisions at $\sqrt{s}$ = 7 TeV"

description: Coalescence parameter $B_2$ of (anti-)deuterons vs. the transverse momentum per nucleon in V0M multiplicity class VI+VII
description: In this letter, the production of deuterons and anti-deuterons in pp collisions at $\sqrt{s}$ = 7 TeV is studied as a function of the charged-particle multiplicity density at mid-rapidity with the ALICE detector at the LHC. Production yields are measured at mid-rapidity in five multiplicity classes and as a function of the deuteron transverse momentum (pT). The measurements are discussed in the context of hadron-coalescence models. The coalescence parameter B2, extracted from the measured spectra of (anti-)deuterons and primary (anti-)protons, exhibits no significant pT-dependence for pT &lt; 3 GeV/c, in agreement with the expectations of a simple coalescence picture. At fixed transverse momentum per nucleon, the B2 parameter is found to decrease smoothly from low multiplicity pp to Pb-Pb collisions, in qualitative agreement with more elaborate coalescence models. The measured mean transverse momentum of (anti-)deuterons in pp is not reproduced by the Blast-Wave model calculations that simultaneously describe pion, kaon and proton spectra, in contrast to central Pb-Pb collisions. The ratio between the pT-integrated yield of deuterons to protons, d/p, is found to increase with the charged-particle multiplicity, as observed in inelastic pp collisions at different centre-of-mass energies. The d/p ratios are reported in a wide range, from the lowest to the highest multiplicity values measured in pp collisions at the LHC.
DOI: 10.17182/hepdata.93743.v1/t1
title: "Table 1" of "Measurement of the top quark pair production cross section in dilepton final states containing one $\tau$ lepton in pp collisions at $\sqrt{s}=$ 13 TeV"

description: The measured inclusive top quark pair production cross section in the dilepton final state with one tau lepton.
description: CERN-LHC. The cross section of top quark pair production is measured in the dilepton final state with one tau lepton decaying hadronically.
The data sample corresponds to an integrated luminosity of 35.9 inverse femtobarns
collected in proton-proton collisions at sqrt(s) = 13 TeV in 2016 with the CMS detector.
The ratio of the cross sections in the lepton-tau and light dilepton final states
and the ratio of the partial width to the total decay width of the top quark are also measured.
DOI: 10.17182/hepdata.93743.v1/t2
title: "Table 2" of "Measurement of the top quark pair production cross section in dilepton final states containing one $\tau$ lepton in pp collisions at $\sqrt{s}=$ 13 TeV"

description: The ratio between top quark production cross sections measured in lepton-tau and light dilepton final states.
description: CERN-LHC. The cross section of top quark pair production is measured in the dilepton final state with one tau lepton decaying hadronically.
The data sample corresponds to an integrated luminosity of 35.9 inverse femtobarns
collected in proton-proton collisions at sqrt(s) = 13 TeV in 2016 with the CMS detector.
The ratio of the cross sections in the lepton-tau and light dilepton final states
and the ratio of the partial width to the total decay width of the top quark are also measured.
DOI: 10.17182/hepdata.93743.v1/t3
title: "Table 3" of "Measurement of the top quark pair production cross section in dilepton final states containing one $\tau$ lepton in pp collisions at $\sqrt{s}=$ 13 TeV"

description: The ratio of the partial width to the total decay width of the top quark.
description: CERN-LHC. The cross section of top quark pair production is measured in the dilepton final state with one tau lepton decaying hadronically.
The data sample corresponds to an integrated luminosity of 35.9 inverse femtobarns
collected in proton-proton collisions at sqrt(s) = 13 TeV in 2016 with the CMS detector.
The ratio of the cross sections in the lepton-tau and light dilepton final states
and the ratio of the partial width to the total decay width of the top quark are also measured.
DOI: 10.17182/hepdata.93789.v1/t1
title: "Figure 1.0.0" of "Measurement of Groomed Jet Substructure Observables in \pp Collisions at $\sqrt{s} = 200$ GeV with STAR"

description: The data points and the error bars represent the mean $p_{\rm{T, jet}}^{\rm{det}}$ and the width (RMS) for a given $p_{\rm{T, jet}}^{\rm{part}}$ selection $R = 0.4$.
description: In this letter, a comprehensive suite of jet substructure measurements via the SoftDrop algorithm, including the shared momentum fraction ($z_{\rm{g}}$) and the groomed jet radius ($R_{\rm{g}}$), are reported in \pp collisions at $\sqrt{s} = 200$ GeV collected by the STAR experiment. These substructure observables are differentially measured for jets of varying resolution parameters from $R = 0.2$ to $R = 0.6$ and transverse momentum range $15 &lt; p_{\rm{T, jet}} &lt; 60$ GeV$/c$. These studies show that, at RHIC kinematics with increasing jet resolution parameter and jet energy, the $z_{\rm{g}}$ distribution asymptotically converges to the DGLAP splitting kernel. The groomed jet radius measurements reflect a momentum-dependent narrowing of the jet structure for jets of a given resolution parameter, i.e., the larger the $p_{\rm{T, jet}}$, the narrower the first split. For the first time, these fully corrected measurements are compared to leading order Monte Carlo generators and to state-of-the-art theoretical calculations at next-to-leading-log accuracy. We observe that RHIC-tuned PYTHIA 6 is able to quantitatively reproduce data whereas the LHC-tuned event generators, PYTHIA 8 and HERWIG 7, are unable to provide a simultaneous description of both the $z_{\rm{g}}$ and $R_{\rm{g}}$, resulting in opportunities for fine parameter tuning of these models in \pp collisions at varying collision energies. We also find that the theoretical calculations without non-perturbative corrections are able to qualitatively describe the trend in data for jets of large resolution parameters at high $p_{\rm{T, jet}}$, but fail at small jet resolution parameters and low jet momenta.
DOI: 10.17182/hepdata.93789.v1/t2
title: "Figure 3.0.0" of "Measurement of Groomed Jet Substructure Observables in \pp Collisions at $\sqrt{s} = 200$ GeV with STAR"

description: Uncorrected $z_{g}$ for $20 &lt; p_{\rm{T, jet}} &lt; 25$ GeV/c, R=0.4 anti-kT jets
description: In this letter, a comprehensive suite of jet substructure measurements via the SoftDrop algorithm, including the shared momentum fraction ($z_{\rm{g}}$) and the groomed jet radius ($R_{\rm{g}}$), are reported in \pp collisions at $\sqrt{s} = 200$ GeV collected by the STAR experiment. These substructure observables are differentially measured for jets of varying resolution parameters from $R = 0.2$ to $R = 0.6$ and transverse momentum range $15 &lt; p_{\rm{T, jet}} &lt; 60$ GeV$/c$. These studies show that, at RHIC kinematics with increasing jet resolution parameter and jet energy, the $z_{\rm{g}}$ distribution asymptotically converges to the DGLAP splitting kernel. The groomed jet radius measurements reflect a momentum-dependent narrowing of the jet structure for jets of a given resolution parameter, i.e., the larger the $p_{\rm{T, jet}}$, the narrower the first split. For the first time, these fully corrected measurements are compared to leading order Monte Carlo generators and to state-of-the-art theoretical calculations at next-to-leading-log accuracy. We observe that RHIC-tuned PYTHIA 6 is able to quantitatively reproduce data whereas the LHC-tuned event generators, PYTHIA 8 and HERWIG 7, are unable to provide a simultaneous description of both the $z_{\rm{g}}$ and $R_{\rm{g}}$, resulting in opportunities for fine parameter tuning of these models in \pp collisions at varying collision energies. We also find that the theoretical calculations without non-perturbative corrections are able to qualitatively describe the trend in data for jets of large resolution parameters at high $p_{\rm{T, jet}}$, but fail at small jet resolution parameters and low jet momenta.
DOI: 10.17182/hepdata.93789.v1/t3
title: "Figure 3.1.0" of "Measurement of Groomed Jet Substructure Observables in \pp Collisions at $\sqrt{s} = 200$ GeV with STAR"

description: Uncorrected $R_{g}$ for $20 &lt; p_{\rm{T, jet}} &lt; 25$ GeV/c, R=0.4 anti-kT jets
description: In this letter, a comprehensive suite of jet substructure measurements via the SoftDrop algorithm, including the shared momentum fraction ($z_{\rm{g}}$) and the groomed jet radius ($R_{\rm{g}}$), are reported in \pp collisions at $\sqrt{s} = 200$ GeV collected by the STAR experiment. These substructure observables are differentially measured for jets of varying resolution parameters from $R = 0.2$ to $R = 0.6$ and transverse momentum range $15 &lt; p_{\rm{T, jet}} &lt; 60$ GeV$/c$. These studies show that, at RHIC kinematics with increasing jet resolution parameter and jet energy, the $z_{\rm{g}}$ distribution asymptotically converges to the DGLAP splitting kernel. The groomed jet radius measurements reflect a momentum-dependent narrowing of the jet structure for jets of a given resolution parameter, i.e., the larger the $p_{\rm{T, jet}}$, the narrower the first split. For the first time, these fully corrected measurements are compared to leading order Monte Carlo generators and to state-of-the-art theoretical calculations at next-to-leading-log accuracy. We observe that RHIC-tuned PYTHIA 6 is able to quantitatively reproduce data whereas the LHC-tuned event generators, PYTHIA 8 and HERWIG 7, are unable to provide a simultaneous description of both the $z_{\rm{g}}$ and $R_{\rm{g}}$, resulting in opportunities for fine parameter tuning of these models in \pp collisions at varying collision energies. We also find that the theoretical calculations without non-perturbative corrections are able to qualitatively describe the trend in data for jets of large resolution parameters at high $p_{\rm{T, jet}}$, but fail at small jet resolution parameters and low jet momenta.
DOI: 10.17182/hepdata.93789.v1/t4
title: "Figure 4.0.0" of "Measurement of Groomed Jet Substructure Observables in \pp Collisions at $\sqrt{s} = 200$ GeV with STAR"

description: Fully corrected $z_{g}$ for $15 &lt; p_{\rm{T, jet}} &lt; 20$ GeV/c, R=0.4 anti-kT jets
description: In this letter, a comprehensive suite of jet substructure measurements via the SoftDrop algorithm, including the shared momentum fraction ($z_{\rm{g}}$) and the groomed jet radius ($R_{\rm{g}}$), are reported in \pp collisions at $\sqrt{s} = 200$ GeV collected by the STAR experiment. These substructure observables are differentially measured for jets of varying resolution parameters from $R = 0.2$ to $R = 0.6$ and transverse momentum range $15 &lt; p_{\rm{T, jet}} &lt; 60$ GeV$/c$. These studies show that, at RHIC kinematics with increasing jet resolution parameter and jet energy, the $z_{\rm{g}}$ distribution asymptotically converges to the DGLAP splitting kernel. The groomed jet radius measurements reflect a momentum-dependent narrowing of the jet structure for jets of a given resolution parameter, i.e., the larger the $p_{\rm{T, jet}}$, the narrower the first split. For the first time, these fully corrected measurements are compared to leading order Monte Carlo generators and to state-of-the-art theoretical calculations at next-to-leading-log accuracy. We observe that RHIC-tuned PYTHIA 6 is able to quantitatively reproduce data whereas the LHC-tuned event generators, PYTHIA 8 and HERWIG 7, are unable to provide a simultaneous description of both the $z_{\rm{g}}$ and $R_{\rm{g}}$, resulting in opportunities for fine parameter tuning of these models in \pp collisions at varying collision energies. We also find that the theoretical calculations without non-perturbative corrections are able to qualitatively describe the trend in data for jets of large resolution parameters at high $p_{\rm{T, jet}}$, but fail at small jet resolution parameters and low jet momenta.
DOI: 10.17182/hepdata.93789.v1/t5
title: "Figure 4.1.0" of "Measurement of Groomed Jet Substructure Observables in \pp Collisions at $\sqrt{s} = 200$ GeV with STAR"

description: Fully corrected $z_{g}$ for $20 &lt; p_{\rm{T, jet}} &lt; 25$ GeV/c, R=0.4 anti-kT jets
description: In this letter, a comprehensive suite of jet substructure measurements via the SoftDrop algorithm, including the shared momentum fraction ($z_{\rm{g}}$) and the groomed jet radius ($R_{\rm{g}}$), are reported in \pp collisions at $\sqrt{s} = 200$ GeV collected by the STAR experiment. These substructure observables are differentially measured for jets of varying resolution parameters from $R = 0.2$ to $R = 0.6$ and transverse momentum range $15 &lt; p_{\rm{T, jet}} &lt; 60$ GeV$/c$. These studies show that, at RHIC kinematics with increasing jet resolution parameter and jet energy, the $z_{\rm{g}}$ distribution asymptotically converges to the DGLAP splitting kernel. The groomed jet radius measurements reflect a momentum-dependent narrowing of the jet structure for jets of a given resolution parameter, i.e., the larger the $p_{\rm{T, jet}}$, the narrower the first split. For the first time, these fully corrected measurements are compared to leading order Monte Carlo generators and to state-of-the-art theoretical calculations at next-to-leading-log accuracy. We observe that RHIC-tuned PYTHIA 6 is able to quantitatively reproduce data whereas the LHC-tuned event generators, PYTHIA 8 and HERWIG 7, are unable to provide a simultaneous description of both the $z_{\rm{g}}$ and $R_{\rm{g}}$, resulting in opportunities for fine parameter tuning of these models in \pp collisions at varying collision energies. We also find that the theoretical calculations without non-perturbative corrections are able to qualitatively describe the trend in data for jets of large resolution parameters at high $p_{\rm{T, jet}}$, but fail at small jet resolution parameters and low jet momenta.
DOI: 10.17182/hepdata.93789.v1/t10
title: "Figure 5.1.0" of "Measurement of Groomed Jet Substructure Observables in \pp Collisions at $\sqrt{s} = 200$ GeV with STAR"

description: Fully corrected $R_{g}$ for $20 &lt; p_{\rm{T, jet}} &lt; 25$ GeV/c, R=0.4 anti-kT jets
description: In this letter, a comprehensive suite of jet substructure measurements via the SoftDrop algorithm, including the shared momentum fraction ($z_{\rm{g}}$) and the groomed jet radius ($R_{\rm{g}}$), are reported in \pp collisions at $\sqrt{s} = 200$ GeV collected by the STAR experiment. These substructure observables are differentially measured for jets of varying resolution parameters from $R = 0.2$ to $R = 0.6$ and transverse momentum range $15 &lt; p_{\rm{T, jet}} &lt; 60$ GeV$/c$. These studies show that, at RHIC kinematics with increasing jet resolution parameter and jet energy, the $z_{\rm{g}}$ distribution asymptotically converges to the DGLAP splitting kernel. The groomed jet radius measurements reflect a momentum-dependent narrowing of the jet structure for jets of a given resolution parameter, i.e., the larger the $p_{\rm{T, jet}}$, the narrower the first split. For the first time, these fully corrected measurements are compared to leading order Monte Carlo generators and to state-of-the-art theoretical calculations at next-to-leading-log accuracy. We observe that RHIC-tuned PYTHIA 6 is able to quantitatively reproduce data whereas the LHC-tuned event generators, PYTHIA 8 and HERWIG 7, are unable to provide a simultaneous description of both the $z_{\rm{g}}$ and $R_{\rm{g}}$, resulting in opportunities for fine parameter tuning of these models in \pp collisions at varying collision energies. We also find that the theoretical calculations without non-perturbative corrections are able to qualitatively describe the trend in data for jets of large resolution parameters at high $p_{\rm{T, jet}}$, but fail at small jet resolution parameters and low jet momenta.
DOI: 10.17182/hepdata.93789.v1/t11
title: "Figure 5.2.0" of "Measurement of Groomed Jet Substructure Observables in \pp Collisions at $\sqrt{s} = 200$ GeV with STAR"

description: Fully corrected $R_{g}$ for $25 &lt; p_{\rm{T, jet}} &lt; 30$ GeV/c, R=0.4 anti-kT jets
description: In this letter, a comprehensive suite of jet substructure measurements via the SoftDrop algorithm, including the shared momentum fraction ($z_{\rm{g}}$) and the groomed jet radius ($R_{\rm{g}}$), are reported in \pp collisions at $\sqrt{s} = 200$ GeV collected by the STAR experiment. These substructure observables are differentially measured for jets of varying resolution parameters from $R = 0.2$ to $R = 0.6$ and transverse momentum range $15 &lt; p_{\rm{T, jet}} &lt; 60$ GeV$/c$. These studies show that, at RHIC kinematics with increasing jet resolution parameter and jet energy, the $z_{\rm{g}}$ distribution asymptotically converges to the DGLAP splitting kernel. The groomed jet radius measurements reflect a momentum-dependent narrowing of the jet structure for jets of a given resolution parameter, i.e., the larger the $p_{\rm{T, jet}}$, the narrower the first split. For the first time, these fully corrected measurements are compared to leading order Monte Carlo generators and to state-of-the-art theoretical calculations at next-to-leading-log accuracy. We observe that RHIC-tuned PYTHIA 6 is able to quantitatively reproduce data whereas the LHC-tuned event generators, PYTHIA 8 and HERWIG 7, are unable to provide a simultaneous description of both the $z_{\rm{g}}$ and $R_{\rm{g}}$, resulting in opportunities for fine parameter tuning of these models in \pp collisions at varying collision energies. We also find that the theoretical calculations without non-perturbative corrections are able to qualitatively describe the trend in data for jets of large resolution parameters at high $p_{\rm{T, jet}}$, but fail at small jet resolution parameters and low jet momenta.
DOI: 10.17182/hepdata.93789.v1/t12
title: "Figure 5.3.0" of "Measurement of Groomed Jet Substructure Observables in \pp Collisions at $\sqrt{s} = 200$ GeV with STAR"

description: Fully corrected $R_{g}$ for $30 &lt; p_{\rm{T, jet}} &lt; 40$ GeV/c, R=0.4 anti-kT jets
description: In this letter, a comprehensive suite of jet substructure measurements via the SoftDrop algorithm, including the shared momentum fraction ($z_{\rm{g}}$) and the groomed jet radius ($R_{\rm{g}}$), are reported in \pp collisions at $\sqrt{s} = 200$ GeV collected by the STAR experiment. These substructure observables are differentially measured for jets of varying resolution parameters from $R = 0.2$ to $R = 0.6$ and transverse momentum range $15 &lt; p_{\rm{T, jet}} &lt; 60$ GeV$/c$. These studies show that, at RHIC kinematics with increasing jet resolution parameter and jet energy, the $z_{\rm{g}}$ distribution asymptotically converges to the DGLAP splitting kernel. The groomed jet radius measurements reflect a momentum-dependent narrowing of the jet structure for jets of a given resolution parameter, i.e., the larger the $p_{\rm{T, jet}}$, the narrower the first split. For the first time, these fully corrected measurements are compared to leading order Monte Carlo generators and to state-of-the-art theoretical calculations at next-to-leading-log accuracy. We observe that RHIC-tuned PYTHIA 6 is able to quantitatively reproduce data whereas the LHC-tuned event generators, PYTHIA 8 and HERWIG 7, are unable to provide a simultaneous description of both the $z_{\rm{g}}$ and $R_{\rm{g}}$, resulting in opportunities for fine parameter tuning of these models in \pp collisions at varying collision energies. We also find that the theoretical calculations without non-perturbative corrections are able to qualitatively describe the trend in data for jets of large resolution parameters at high $p_{\rm{T, jet}}$, but fail at small jet resolution parameters and low jet momenta.