cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.142148.v1/t9
title: "Figure 1e" of "Jet structure of baryon excess in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Partner Particle $v_2$ values.
description: Two particle correlations between identified meson and baryon trigger particles with 2.5 &lt; $p_T$ &lt; 4.0 GeV/$c$ and lower $p_T$ charged hadrons have been measured at midrapidity by the PHENIX experiment at RHIC in $p$+$p$, $d$+Au and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. In noncentral Au+Au collisions, the probability of finding a hadron near in azimuthal angle to the trigger particles is almost identical for mesons and baryons and significantly higher than in $p$+$p$ collisions. The associated yields for trigger baryons decrease in the most central collisions, consistent with some baryon production by thermal recombination in addition to hard scattering.
DOI: 10.17182/hepdata.142148.v1/t11
title: "Figure 2a-2" of "Jet structure of baryon excess in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Yield per trigger for associated charged hadrons between 1.7 &lt; $p_T$ &lt; 2.5 GeV/$c$ for the near- (top) and away- (bottom) side jets.
description: Two particle correlations between identified meson and baryon trigger particles with 2.5 &lt; $p_T$ &lt; 4.0 GeV/$c$ and lower $p_T$ charged hadrons have been measured at midrapidity by the PHENIX experiment at RHIC in $p$+$p$, $d$+Au and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. In noncentral Au+Au collisions, the probability of finding a hadron near in azimuthal angle to the trigger particles is almost identical for mesons and baryons and significantly higher than in $p$+$p$ collisions. The associated yields for trigger baryons decrease in the most central collisions, consistent with some baryon production by thermal recombination in addition to hard scattering.
DOI: 10.17182/hepdata.142148.v1/t12
title: "Figure 2b-1" of "Jet structure of baryon excess in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Uncertainties in Figure 2 as a function of $N_{part}$ and trigger type for AuAu and $d$+Au.
description: Two particle correlations between identified meson and baryon trigger particles with 2.5 &lt; $p_T$ &lt; 4.0 GeV/$c$ and lower $p_T$ charged hadrons have been measured at midrapidity by the PHENIX experiment at RHIC in $p$+$p$, $d$+Au and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. In noncentral Au+Au collisions, the probability of finding a hadron near in azimuthal angle to the trigger particles is almost identical for mesons and baryons and significantly higher than in $p$+$p$ collisions. The associated yields for trigger baryons decrease in the most central collisions, consistent with some baryon production by thermal recombination in addition to hard scattering.
DOI: 10.17182/hepdata.142148.v1/t13
title: "Figure 2b-2" of "Jet structure of baryon excess in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Uncertainties in Figure 2 as a function of $N_{part}$ and trigger type for AuAu and $d$+Au.
description: Two particle correlations between identified meson and baryon trigger particles with 2.5 &lt; $p_T$ &lt; 4.0 GeV/$c$ and lower $p_T$ charged hadrons have been measured at midrapidity by the PHENIX experiment at RHIC in $p$+$p$, $d$+Au and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. In noncentral Au+Au collisions, the probability of finding a hadron near in azimuthal angle to the trigger particles is almost identical for mesons and baryons and significantly higher than in $p$+$p$ collisions. The associated yields for trigger baryons decrease in the most central collisions, consistent with some baryon production by thermal recombination in addition to hard scattering.
DOI: 10.17182/hepdata.142148.v1/t14
title: "Figure 3a-1" of "Jet structure of baryon excess in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $p_T$ spectra of the near side associated charged hadrons corrected to the full jet yield for meson triggers at 2.5 &lt; $p_T$ &lt; 4.0 GeV/$c$ and $|\eta|$ &lt; 0.35 for six centralities in Au+Au and $d$+Au collisions.
description: Two particle correlations between identified meson and baryon trigger particles with 2.5 &lt; $p_T$ &lt; 4.0 GeV/$c$ and lower $p_T$ charged hadrons have been measured at midrapidity by the PHENIX experiment at RHIC in $p$+$p$, $d$+Au and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. In noncentral Au+Au collisions, the probability of finding a hadron near in azimuthal angle to the trigger particles is almost identical for mesons and baryons and significantly higher than in $p$+$p$ collisions. The associated yields for trigger baryons decrease in the most central collisions, consistent with some baryon production by thermal recombination in addition to hard scattering.
DOI: 10.17182/hepdata.142148.v1/t15
title: "Figure 3a-2" of "Jet structure of baryon excess in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $p_T$ spectra of the near side associated charged hadrons corrected to the full jet yield for meson triggers at 2.5 &lt; $p_T$ &lt; 4.0 GeV/$c$ and $|\eta|$ &lt; 0.35 for six centralities in Au+Au and $d$+Au collisions.
description: Two particle correlations between identified meson and baryon trigger particles with 2.5 &lt; $p_T$ &lt; 4.0 GeV/$c$ and lower $p_T$ charged hadrons have been measured at midrapidity by the PHENIX experiment at RHIC in $p$+$p$, $d$+Au and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. In noncentral Au+Au collisions, the probability of finding a hadron near in azimuthal angle to the trigger particles is almost identical for mesons and baryons and significantly higher than in $p$+$p$ collisions. The associated yields for trigger baryons decrease in the most central collisions, consistent with some baryon production by thermal recombination in addition to hard scattering.
DOI: 10.17182/hepdata.142148.v1/t16
title: "Figure 3b" of "Jet structure of baryon excess in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $p_T$ spectra of the near side associated charged hadrons corrected to the full jet yield for baryon triggers at 2.5 &lt; $p_T$ &lt; 4.0 GeV/$c$ and $|\eta|$ &lt; 0.35 for six centralities in Au+Au, $d$+Au and $p$+$p$ collisions.
description: Two particle correlations between identified meson and baryon trigger particles with 2.5 &lt; $p_T$ &lt; 4.0 GeV/$c$ and lower $p_T$ charged hadrons have been measured at midrapidity by the PHENIX experiment at RHIC in $p$+$p$, $d$+Au and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. In noncentral Au+Au collisions, the probability of finding a hadron near in azimuthal angle to the trigger particles is almost identical for mesons and baryons and significantly higher than in $p$+$p$ collisions. The associated yields for trigger baryons decrease in the most central collisions, consistent with some baryon production by thermal recombination in addition to hard scattering.
DOI: 10.17182/hepdata.142148.v1/t17
title: "Figure 4a" of "Jet structure of baryon excess in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Inverse slopes from the fits in Figure 3.
description: Two particle correlations between identified meson and baryon trigger particles with 2.5 &lt; $p_T$ &lt; 4.0 GeV/$c$ and lower $p_T$ charged hadrons have been measured at midrapidity by the PHENIX experiment at RHIC in $p$+$p$, $d$+Au and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. In noncentral Au+Au collisions, the probability of finding a hadron near in azimuthal angle to the trigger particles is almost identical for mesons and baryons and significantly higher than in $p$+$p$ collisions. The associated yields for trigger baryons decrease in the most central collisions, consistent with some baryon production by thermal recombination in addition to hard scattering.
DOI: 10.17182/hepdata.142148.v1/t18
title: "Figure 4b-1" of "Jet structure of baryon excess in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Inverse slopes from the fits in Figure 3.
description: Two particle correlations between identified meson and baryon trigger particles with 2.5 &lt; $p_T$ &lt; 4.0 GeV/$c$ and lower $p_T$ charged hadrons have been measured at midrapidity by the PHENIX experiment at RHIC in $p$+$p$, $d$+Au and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. In noncentral Au+Au collisions, the probability of finding a hadron near in azimuthal angle to the trigger particles is almost identical for mesons and baryons and significantly higher than in $p$+$p$ collisions. The associated yields for trigger baryons decrease in the most central collisions, consistent with some baryon production by thermal recombination in addition to hard scattering.
DOI: 10.17182/hepdata.142148.v1/t19
title: "Figure 4b-2" of "Jet structure of baryon excess in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Inverse slopes from the fits in Figure 3.
description: Two particle correlations between identified meson and baryon trigger particles with 2.5 &lt; $p_T$ &lt; 4.0 GeV/$c$ and lower $p_T$ charged hadrons have been measured at midrapidity by the PHENIX experiment at RHIC in $p$+$p$, $d$+Au and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. In noncentral Au+Au collisions, the probability of finding a hadron near in azimuthal angle to the trigger particles is almost identical for mesons and baryons and significantly higher than in $p$+$p$ collisions. The associated yields for trigger baryons decrease in the most central collisions, consistent with some baryon production by thermal recombination in addition to hard scattering.
DOI: 10.17182/hepdata.142234.v1/t1
title: "Table 1" of "Measurement of the lifetime and $\Lambda$ separation energy of $^{3}_{\Lambda}\mathrm H$"

description: $^{3}_{\Lambda}\mathrm H$ Lifetime and $\mathrm{B_{\Lambda}}$
description: The most precise measurements to date of the $^{3}_{\Lambda}\mathrm H$ lifetime $\tau_{^{3}_{\Lambda}\mathrm H}$ and $\Lambda$ separation energy $\mathrm{B_{\Lambda}}$ are obtained using the data sample of Pb--Pb collisionsat $\sqrt{s_{\mathrm{NN}}}=$5.02 TeV collected by the ALICE experiment at the LHC. The ^{3}_{\Lambda}\mathrm H is reconstructed via its charged two-body mesonic decay channel ($^{3}_{\Lambda}\mathrm H$ $\rightarrow$ $^3$He + $\pi^-$and the charge-conjugate process). The measured values $\tau_{^{3}_{\Lambda}\mathrm H} = [253 \pm 11 \text{~(stat.)} \pm 6 \text{~(syst.)}]$ ps and $\mathrm{B_{\Lambda}} = [102 \pm 63 \text{~(stat.)} \pm 67 \text{~(syst.)}]$ keV are compatible with predictions from effective field theories and conclusively confirm that the $^{3}_{\Lambda}\mathrm H$ is a weakly-bound system.
DOI: 10.17182/hepdata.142287.v1/t1
title: "Figure 8a" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: The $\chi^2(DOF)$ $\sigma_N$ and $\sqrt{}$ values extracted for the correlation function in GeV/$c$.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t2
title: "Figure 8b" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: The $\chi^2(DOF)$ $\sigma_N$ and $\sqrt{}$ values extracted for the correlation function in GeV/$c$.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t3
title: "Figure 9a" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: Measured widths of the near- and away-angle $\pi^0$ - $h^{\pm}$ correlation peaks for various trigger momenta.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t10
title: "Figure 12" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: The $\sqrt{}$ values in GeV/$c$.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t4
title: "Figure 9b" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: Measured widths of the near- and away-angle $\pi^0$ - $h^{\pm}$ correlation peaks for various trigger momenta.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t5
title: "Figure 9c" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: Measured widths of the near- and away-angle $\pi^0$ - $h^{\pm}$ correlation peaks for various trigger momenta.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t6
title: "Figure 9d" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: Measured widths of the near- and away-angle $\pi^0$ - $h^{\pm}$ correlation peaks for various trigger momenta.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t7
title: "Figure 10" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: The $\sigma_N$ and $\sigma_A$ values in GeV/$c$.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.
DOI: 10.17182/hepdata.142287.v1/t8
title: "Figure 11a" of "Jet properties from dihadron correlations in p+p collisions at s**(1/2) = 200-GeV"

description: The $\sqrt{}$ values in GeV/$c$.
description: The properties of jets produced in $p$+$p$ collisions at $\sqrt{s}$ = 200 GeV are measured using the method of two particle correlations. The trigger particle is a leading particle from a large transverse momentum jet while the associated particle comes from either the same jet or the away-side jet. Analysis of the angular width of the near-side peak in the correlation function determines the jet fragmentation transverse momentum $j_T$. The extracted value, $\sqrt{}$ = 585 +/- 6(stat.) +/- 15(syst.) MeV/$c$, is constant with respect to the trigger particle transverse momentum, and comparable to the previous lower $\sqrt{s}$ measurements. The width of the away-side peak is shown to be a convolution of $j_T$ with the fragmentation variable, $z$, and the partonic transverse momentum, $k_T$. The $$ is determined through a combined analysis of the measured $\pi^0$ inclusive and associated spectra using jet fragmentation functions measured in $e^+$$e^-$ collisions. The final extracted values of $k_T$ are then determined to also be independent of the trigger particle transverse momentum, over the range measured, with value of $\sqrt{}$ = 2.68 +/- 0.07(stat.) +/- 0.34(syst.) GeV/$c$.