cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.152377.v1/t14
title: "Table 14" of "Measurements of jet quenching using semi-inclusive hadron+jet distributions in pp and central Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ ratios $R=$ 0.2 / 0.5 in pp and Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.
description: The ALICE Collaboration reports measurements of the semi-inclusive distribution of charged-particle jets recoiling from a high transverse momentum (high $p_\mathrm{T}$) charged hadron, in pp and central Pb--Pb collisions at center of mass energy per nucleon--nucleon collision $\sqrt{s_\mathrm{NN}}=5.02$ TeV. The large uncorrelated background in central Pb--Pb collisions is corrected using a data-driven statistical approach, which enables precise measurement of recoil jet distributions over a broad range in $p_\mathrm{T,ch jet}$ and jet resolution parameter $R$. Recoil jet yields are reported for $R=$ 0.2, 0.4, and 0.5 in the range $7
DOI: 10.17182/hepdata.152377.v1/t15
title: "Table 15" of "Measurements of jet quenching using semi-inclusive hadron+jet distributions in pp and central Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ ratios $R=$ 0.4 / 0.5 in pp and Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.
description: The ALICE Collaboration reports measurements of the semi-inclusive distribution of charged-particle jets recoiling from a high transverse momentum (high $p_\mathrm{T}$) charged hadron, in pp and central Pb--Pb collisions at center of mass energy per nucleon--nucleon collision $\sqrt{s_\mathrm{NN}}=5.02$ TeV. The large uncorrelated background in central Pb--Pb collisions is corrected using a data-driven statistical approach, which enables precise measurement of recoil jet distributions over a broad range in $p_\mathrm{T,ch jet}$ and jet resolution parameter $R$. Recoil jet yields are reported for $R=$ 0.2, 0.4, and 0.5 in the range $7
DOI: 10.17182/hepdata.152377.v1/t16
title: "Table 16" of "Measurements of jet quenching using semi-inclusive hadron+jet distributions in pp and central Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ for $R=$ 0.2, for various $\mathrm{TT_{sig}}$ selections in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.
description: The ALICE Collaboration reports measurements of the semi-inclusive distribution of charged-particle jets recoiling from a high transverse momentum (high $p_\mathrm{T}$) charged hadron, in pp and central Pb--Pb collisions at center of mass energy per nucleon--nucleon collision $\sqrt{s_\mathrm{NN}}=5.02$ TeV. The large uncorrelated background in central Pb--Pb collisions is corrected using a data-driven statistical approach, which enables precise measurement of recoil jet distributions over a broad range in $p_\mathrm{T,ch jet}$ and jet resolution parameter $R$. Recoil jet yields are reported for $R=$ 0.2, 0.4, and 0.5 in the range $7
DOI: 10.17182/hepdata.152377.v1/t17
title: "Table 17" of "Measurements of jet quenching using semi-inclusive hadron+jet distributions in pp and central Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ for $R=$ 0.4, for various $\mathrm{TT_{sig}}$ selections in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.
description: The ALICE Collaboration reports measurements of the semi-inclusive distribution of charged-particle jets recoiling from a high transverse momentum (high $p_\mathrm{T}$) charged hadron, in pp and central Pb--Pb collisions at center of mass energy per nucleon--nucleon collision $\sqrt{s_\mathrm{NN}}=5.02$ TeV. The large uncorrelated background in central Pb--Pb collisions is corrected using a data-driven statistical approach, which enables precise measurement of recoil jet distributions over a broad range in $p_\mathrm{T,ch jet}$ and jet resolution parameter $R$. Recoil jet yields are reported for $R=$ 0.2, 0.4, and 0.5 in the range $7
DOI: 10.17182/hepdata.144875.v1/t1
title: "Table 1" of "Exclusive and dissociative J/$\psi$ photoproduction, and exclusive dimuon production, in p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Differential cross sections DSIGMA/DM for exclusive GAMMA* GAMMA* to MU+ MU- production in p–Pb UPCs for each mass and rapidity interval
description: Exclusive and dissociative J/psi photoproduction, and exclusive dimuon production, in p–Pb collisions at sqrt(s_NN) = 8.16 TeV
DOI: 10.17182/hepdata.144875.v1/t2
title: "Table 2" of "Exclusive and dissociative J/$\psi$ photoproduction, and exclusive dimuon production, in p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Exclusive J/psi photoproduction cross section in p-Pb UPC.
description: Exclusive and dissociative J/psi photoproduction, and exclusive dimuon production, in p–Pb collisions at sqrt(s_NN) = 8.16 TeV
DOI: 10.17182/hepdata.144875.v1/t3
title: "Table 3" of "Exclusive and dissociative J/$\psi$ photoproduction, and exclusive dimuon production, in p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Dissociative J/psi photoproduction cross section in p-Pb UPC.
description: Exclusive and dissociative J/psi photoproduction, and exclusive dimuon production, in p–Pb collisions at sqrt(s_NN) = 8.16 TeV
DOI: 10.17182/hepdata.144875.v1/t4
title: "Table 4" of "Exclusive and dissociative J/$\psi$ photoproduction, and exclusive dimuon production, in p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Exclusive J/psi photoproduction cross section in gamma-p.
description: Exclusive and dissociative J/psi photoproduction, and exclusive dimuon production, in p–Pb collisions at sqrt(s_NN) = 8.16 TeV
DOI: 10.17182/hepdata.144875.v1/t5
title: "Table 5" of "Exclusive and dissociative J/$\psi$ photoproduction, and exclusive dimuon production, in p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Dissociative J/psi photoproduction gamma-p.
description: Exclusive and dissociative J/psi photoproduction, and exclusive dimuon production, in p–Pb collisions at sqrt(s_NN) = 8.16 TeV
DOI: 10.17182/hepdata.144875.v1/t6
title: "Table 6" of "Exclusive and dissociative J/$\psi$ photoproduction, and exclusive dimuon production, in p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV"

description: Cross section ratio, dissociative J/psi photoproduction gamma-p over exclusive J/psi photoproduction gamma-p.
description: Exclusive and dissociative J/psi photoproduction, and exclusive dimuon production, in p–Pb collisions at sqrt(s_NN) = 8.16 TeV
DOI: 10.17182/hepdata.151164.v1/t1
title: "$z_{\parallel}^{\rm{ch}}$" of "Exploring the non-universality of charm hadronisation through the measurement of the fraction of jet longitudinal momentum carried by $\Lambda_{\rm c}^+$ baryons in pp collisions"

description: $z_{\parallel}^{\rm{ch}}$ for $\Lambda_{\rm{c}}^{+}$-tagged jets and D$^{0}$-tagged jets in the $p_{\rm{T}}^{\rm{jet\text{ }ch}}$: 7-15 GeV/$c$ interval.
description: Recent measurements of charm-baryon production in hadronic collisions have questioned the universality of charm-quark fragmentation across different collision systems. In this work the fragmentation of charm quarks into charm baryons is probed, by presenting the first measurement of the longitudinal jet momentum fraction carried by $\Lambda_{\rm{c}}^{+}$ baryons, $z_{\parallel}$, in hadronic collisions. The results are obtained in proton--proton (pp) collisions at $\sqrt{s}=13$ TeV at the LHC, with $\Lambda_{\rm{c}}^{+}$ baryons and track-based jets reconstructed in the transverse momentum intervals of $3 \leq p_{\rm{T}}^{\Lambda_{\rm{c}}^{+}} &lt; 15$ GeV$/\it{c}$ and $7 \leq p_{\rm{T}}^{\rm{jet,ch}} &lt; 15$ GeV$/\it{c}$, respectively. The $z_{\parallel}$ distribution is compared to a measurement of D$^{0}$-tagged charged jets in pp collisions as well as to PYTHIA 8 simulations. The data hints that the fragmentation of charm quarks into charm baryons is softer with respect to charm mesons, as predicted by hadronisation models which include colour correlations beyond leading-colour in the string formation.
DOI: 10.17182/hepdata.151164.v1/t2
title: "$\Lambda_{\rm{c}}^{+}$ D$^{0}$ Ratio" of "Exploring the non-universality of charm hadronisation through the measurement of the fraction of jet longitudinal momentum carried by $\Lambda_{\rm c}^+$ baryons in pp collisions"

description: $z_{\parallel}^{\rm{ch}}$ ratio of $\Lambda_{\rm{c}}^{+}$-tagged jets and D$^{0}$-tagged jets in the $p_{\rm{T}}^{\rm{jet\text{ }ch}}$: 7-15 GeV/$c$ interval.
description: Recent measurements of charm-baryon production in hadronic collisions have questioned the universality of charm-quark fragmentation across different collision systems. In this work the fragmentation of charm quarks into charm baryons is probed, by presenting the first measurement of the longitudinal jet momentum fraction carried by $\Lambda_{\rm{c}}^{+}$ baryons, $z_{\parallel}$, in hadronic collisions. The results are obtained in proton--proton (pp) collisions at $\sqrt{s}=13$ TeV at the LHC, with $\Lambda_{\rm{c}}^{+}$ baryons and track-based jets reconstructed in the transverse momentum intervals of $3 \leq p_{\rm{T}}^{\Lambda_{\rm{c}}^{+}} &lt; 15$ GeV$/\it{c}$ and $7 \leq p_{\rm{T}}^{\rm{jet,ch}} &lt; 15$ GeV$/\it{c}$, respectively. The $z_{\parallel}$ distribution is compared to a measurement of D$^{0}$-tagged charged jets in pp collisions as well as to PYTHIA 8 simulations. The data hints that the fragmentation of charm quarks into charm baryons is softer with respect to charm mesons, as predicted by hadronisation models which include colour correlations beyond leading-colour in the string formation.
DOI: 10.17182/hepdata.136307.v1/t1
title: "Table 1" of "${\rm f}_{0}(980)$ production in inelastic pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $p_{\rm T}$-differential yields of $f_{0}(980)$ at midrapidity in the inelastic pp collisions at $\sqrt(s)$ = 5.02 TeV. The uncertainty 'syst' indicates the total systematic uncertainty and 'stat' indicates the statistical uncertainty. The branching ratio correction amounts to BR = (46 $\pm$ 6)% [ Phys. Rev. Lett. 111 no. 6, (2013) 062001] assuming dominance of $\pi\pi$ and KK channel has been applied to the $p_{\rm T}$-differential yields of $f_{0}(980)$. The normalisation and branching ratio relative uncertainties on the yields are independent of $p_{\rm{T}}$ and amount to 2.5% and 13%, respectively and therefore not included in the $p_{\rm T}$-differential yields of $f_{0}(980)$.
description: CERN-LHC. The measurement of the production of $\rm{f}_{0}(980)$ in inelastic pp collisions at $\sqrt{s}$ = 5.02 TeV is presented. This is the first reported measurement of inclusive $\rm{f}_{0}(980)$ yield at LHC energies. The production is measured at midrapidity, $\left | y \right | &lt; 0.5$, in a wide transverse momentum range, $0
DOI: 10.17182/hepdata.136307.v1/t2
title: "Table 2" of "${\rm f}_{0}(980)$ production in inelastic pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $p_{\rm T}$-integrated yield of $f_{0}(980)$, dN/dy at midrapidity as a function of $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle$. The uncertainty 'syst' indicates the total systematic uncertainty on the measurement. The branching ratio correction amounts to BR = (46 $\pm$ 6)% [ Phys. Rev. Lett. 111 no. 6, (2013) 062001] assuming dominance of $\pi\pi$ and KK channel has been applied to the $p_{\rm T}$-differential yields of $f_{0}(980)$. Here, the branching ratio relative uncertainty (13%) for $f_{0}(980)$ is not included.
description: CERN-LHC. The measurement of the production of $\rm{f}_{0}(980)$ in inelastic pp collisions at $\sqrt{s}$ = 5.02 TeV is presented. This is the first reported measurement of inclusive $\rm{f}_{0}(980)$ yield at LHC energies. The production is measured at midrapidity, $\left | y \right | &lt; 0.5$, in a wide transverse momentum range, $0
DOI: 10.17182/hepdata.136307.v1/t3
title: "Table 3" of "${\rm f}_{0}(980)$ production in inelastic pp collisions at $\sqrt{s} = 5.02$ TeV"

description: mean-$p_{\rm{T}}$ of $f_{0}(980)$, (&lt;$p_{\rm{T}}$&gt;) at midrapidity as a function of $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle$. The uncertainty 'syst' indicates the total systematic uncertainty on the measurement.
description: CERN-LHC. The measurement of the production of $\rm{f}_{0}(980)$ in inelastic pp collisions at $\sqrt{s}$ = 5.02 TeV is presented. This is the first reported measurement of inclusive $\rm{f}_{0}(980)$ yield at LHC energies. The production is measured at midrapidity, $\left | y \right | &lt; 0.5$, in a wide transverse momentum range, $0
DOI: 10.17182/hepdata.136307.v1/t4
title: "Table 4" of "${\rm f}_{0}(980)$ production in inelastic pp collisions at $\sqrt{s} = 5.02$ TeV"

description: $f_{0}(980)$ to pions ($(\pi^{+}+\pi^{-})/2$), $p_{\rm T}$-integrated yield ratio at midrapidity as a function of $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle$. The uncertainty 'stat,syst' indicates the total uncertainty (stat+syst) on the measurement. The branching ratio correction amounts to BR = (46 $\pm$ 6)% [ Phys. Rev. Lett. 111 no. 6, (2013) 062001] assuming dominance of $\pi\pi$ and KK channel has been applied to the $p_{\rm T}$-differential yields of $f_{0}(980)$. Here, the branching ratio relative uncertainty (13%) for $f_{0}(980)$ is not included.
description: CERN-LHC. The measurement of the production of $\rm{f}_{0}(980)$ in inelastic pp collisions at $\sqrt{s}$ = 5.02 TeV is presented. This is the first reported measurement of inclusive $\rm{f}_{0}(980)$ yield at LHC energies. The production is measured at midrapidity, $\left | y \right | &lt; 0.5$, in a wide transverse momentum range, $0
DOI: 10.15468/dl.52x6e2
title: Occurrence Download

description: A dataset containing 0 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is Esox reichertii",
 "HasCoordinate is true",
 "Geometry POLYGON((-78 12, -73 12, -73 0, -78 0, -78 12))"
 ]
}

 The dataset includes 0 records from 0 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0034384-251025141854904/datasets/export for details.
DOI: 10.15468/dl.asgk2h
title: Occurrence Download

description: A dataset containing 16 species occurrences available in GBIF matching the query:
{
 "Geometry" : [
 "POLYGON ((-107.2188 22.94913, -107.0688 22.94913, -107.0688 23.09913, -107.2188 23.09913, -107.2188 22.94913))"
 ]
}

 The dataset includes 16 records from 8 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0034385-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.141857.v1/t1
title: "Table 1" of "Azimuthal correlations of heavy-flavor hadron decay electrons with charged particles in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: $\Delta\varphi$ distribution between heavy-flavor decay electrons and associated charged particles for $4 &lt; p_{\rm T}^{\rm e} &lt; 12$ ${\rm GeV}/c$ and $1 &lt; p_{\rm T}^{\rm assoc} &lt; 7$ ${\rm GeV}/c$ in pp collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV. The publication shows $\Delta\varphi$ distribution only for the ranges $1 &lt; p_{\rm T}^{\rm assoc} &lt; 2$, $2 &lt; p_{\rm T}^{\rm assoc} &lt; 3$, and $5 &lt; p_{\rm T}^{\rm assoc} &lt; 7$ ${\rm GeV}/c$.
description: The azimuthal ($\Delta\varphi$) correlation distributions between heavy-flavor decay electrons and associated charged particles are measured in pp and p$\textendash$Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV. Results are reported for electrons with transverse momentum $4
DOI: 10.17182/hepdata.141857.v1/t2
title: "Table 2" of "Azimuthal correlations of heavy-flavor hadron decay electrons with charged particles in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: $\Delta\varphi$ distribution between heavy-flavor decay electrons and associated charged particles for $4 &lt; p_{\rm T}^{\rm e} &lt; 12$ ${\rm GeV}/c$ and $1 &lt; p_{\rm T}^{\rm assoc} &lt; 7$ ${\rm GeV}/c$ in p$\textendash$Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV. The publication shows $\Delta\varphi$ distribution only for the ranges $1 &lt; p_{\rm T}^{\rm assoc} &lt; 2$, $2 &lt; p_{\rm T}^{\rm assoc} &lt; 3$, and $5 &lt; p_{\rm T}^{\rm assoc} &lt; 7$ ${\rm GeV}/c$.
description: The azimuthal ($\Delta\varphi$) correlation distributions between heavy-flavor decay electrons and associated charged particles are measured in pp and p$\textendash$Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV. Results are reported for electrons with transverse momentum $4
DOI: 10.17182/hepdata.141857.v1/t3
title: "Table 3" of "Azimuthal correlations of heavy-flavor hadron decay electrons with charged particles in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Baseline of $\Delta\varphi$ distribution between heavy-flavor decay electrons and associated charged particles for $4 &lt; p_{\rm T}^{\rm e} &lt; 12$ ${\rm GeV}/c$ in pp and p$\textendash$Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV. The publication shows $\Delta\varphi$ distribution only for the ranges $1 &lt; p_{\rm T}^{\rm assoc} &lt; 2$, $2 &lt; p_{\rm T}^{\rm assoc} &lt; 3$, and $5 &lt; p_{\rm T}^{\rm assoc} &lt; 7$ ${\rm GeV}/c$.
description: The azimuthal ($\Delta\varphi$) correlation distributions between heavy-flavor decay electrons and associated charged particles are measured in pp and p$\textendash$Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV. Results are reported for electrons with transverse momentum $4
DOI: 10.17182/hepdata.141857.v1/t4
title: "Table 4" of "Azimuthal correlations of heavy-flavor hadron decay electrons with charged particles in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Baseline subtracted $\Delta\varphi$ distribution between heavy-flavor decay electrons and associated charged particles for $4 &lt; p_{\rm T}^{\rm e} &lt; 12$ ${\rm GeV}/c$ and $1 &lt; p_{\rm T}^{\rm assoc} &lt; 7$ ${\rm GeV}/c$ in pp collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV.
description: The azimuthal ($\Delta\varphi$) correlation distributions between heavy-flavor decay electrons and associated charged particles are measured in pp and p$\textendash$Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV. Results are reported for electrons with transverse momentum $4
DOI: 10.17182/hepdata.141857.v1/t5
title: "Table 5" of "Azimuthal correlations of heavy-flavor hadron decay electrons with charged particles in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Baseline subtracted $\Delta\varphi$ distribution between heavy-flavor decay electrons and associated charged particles for $4 &lt; p_{\rm T}^{\rm e} &lt; 12$ ${\rm GeV}/c$ and $1 &lt; p_{\rm T}^{\rm assoc} &lt; 7$ ${\rm GeV}/c$ in p$\textendash$Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV.
description: The azimuthal ($\Delta\varphi$) correlation distributions between heavy-flavor decay electrons and associated charged particles are measured in pp and p$\textendash$Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV. Results are reported for electrons with transverse momentum $4
DOI: 10.17182/hepdata.141857.v1/t6
title: "Table 6" of "Azimuthal correlations of heavy-flavor hadron decay electrons with charged particles in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Associated yield of near-side (NS) $\Delta\varphi$ distribution between heavy-flavor decay electrons and associated charged particles as a function of $p_{\rm T}^{\rm{assoc}}$ for $4 &lt; p_{\rm T}^{\rm e} &lt; 12$ ${\rm GeV}/c$ in pp and p$\textendash$Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV.
description: The azimuthal ($\Delta\varphi$) correlation distributions between heavy-flavor decay electrons and associated charged particles are measured in pp and p$\textendash$Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV. Results are reported for electrons with transverse momentum $4
DOI: 10.17182/hepdata.141857.v1/t7
title: "Table 7" of "Azimuthal correlations of heavy-flavor hadron decay electrons with charged particles in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Associated yield of away-side (AS) $\Delta\varphi$ distribution between heavy-flavor decay electrons and associated charged particles as a function of $p_{\rm T}^{\rm{assoc}}$ for $4 &lt; p_{\rm T}^{\rm e} &lt; 12$ ${\rm GeV}/c$ in pp and p$\textendash$Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV.
description: The azimuthal ($\Delta\varphi$) correlation distributions between heavy-flavor decay electrons and associated charged particles are measured in pp and p$\textendash$Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV. Results are reported for electrons with transverse momentum $4
DOI: 10.17182/hepdata.141857.v1/t10
title: "Table 10" of "Azimuthal correlations of heavy-flavor hadron decay electrons with charged particles in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Associated yield of near-side (NS) $\Delta\varphi$ distribution between heavy-flavor decay electrons and associated charged particles as a function of $p_{\rm T}^{\rm{assoc}}$ for $4 &lt; p_{\rm T}^{\rm e} &lt; 7$ and $7 &lt; p_{\rm T}^{\rm e} &lt; 16$ ${\rm GeV}/c$ in pp collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV.
description: The azimuthal ($\Delta\varphi$) correlation distributions between heavy-flavor decay electrons and associated charged particles are measured in pp and p$\textendash$Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV. Results are reported for electrons with transverse momentum $4
DOI: 10.17182/hepdata.141857.v1/t11
title: "Table 11" of "Azimuthal correlations of heavy-flavor hadron decay electrons with charged particles in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Associated yield of away-side (AS) $\Delta\varphi$ distribution between heavy-flavor decay electrons and associated charged particles as a function of $p_{\rm T}^{\rm{assoc}}$ for $4 &lt; p_{\rm T}^{\rm e} &lt; 7$ and $7 &lt; p_{\rm T}^{\rm e} &lt; 16$ ${\rm GeV}/c$ in pp collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV.
description: The azimuthal ($\Delta\varphi$) correlation distributions between heavy-flavor decay electrons and associated charged particles are measured in pp and p$\textendash$Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV. Results are reported for electrons with transverse momentum $4
DOI: 10.17182/hepdata.141857.v1/t12
title: "Table 12" of "Azimuthal correlations of heavy-flavor hadron decay electrons with charged particles in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Width of near-side (NS) $\Delta\varphi$ distribution between heavy-flavor decay electrons and associated charged particles as a function of $p_{\rm T}^{\rm{assoc}}$ for $4 &lt; p_{\rm T}^{\rm e} &lt; 7$ and $7 &lt; p_{\rm T}^{\rm e} &lt; 16$ ${\rm GeV}/c$ in pp collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV.
description: The azimuthal ($\Delta\varphi$) correlation distributions between heavy-flavor decay electrons and associated charged particles are measured in pp and p$\textendash$Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV. Results are reported for electrons with transverse momentum $4
DOI: 10.17182/hepdata.141857.v1/t13
title: "Table 13" of "Azimuthal correlations of heavy-flavor hadron decay electrons with charged particles in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Width of away-side (AS) $\Delta\varphi$ distribution between heavy-flavor decay electrons and associated charged particles as a function of $p_{\rm T}^{\rm{assoc}}$ for $4 &lt; p_{\rm T}^{\rm e} &lt; 7$ and $7 &lt; p_{\rm T}^{\rm e} &lt; 16$ ${\rm GeV}/c$ in pp collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV.
description: The azimuthal ($\Delta\varphi$) correlation distributions between heavy-flavor decay electrons and associated charged particles are measured in pp and p$\textendash$Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV. Results are reported for electrons with transverse momentum $4