cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.165764.v1/t13
title: "Table 13" of "D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV"

description: $\Delta R_{\rm axis}$ distribution for $\rm STD-SD$ with grooming setting ($z_{\rm cut} = 0.1, \beta = 0$) for $\rm D^0$-tagged jets of $R=0.4$, in the intervals $10
description: Heavy-flavor quarks produced in proton$\mathrm{-}$proton (pp) collisions provide a unique opportunity to investigate the evolution of quark-initiated parton showers from initial hard scatterings to final-state hadrons. By examining jets that contain heavy-flavor hadrons, this study explores the effects of both perturbative and non-perturbative QCD on jet formation and structure. The angular differences between various jet axes, $\Delta R_{\rm axis}$, offer insight into the radiation patterns and fragmentation of charm quarks. The first measurement of D$^{0}$-tagged jet axes differences in pp collisions at $\sqrt{s}=5.02$ TeV by the ALICE experiment at the LHC is presented for jets with transverse momentum $p_{\rm T}^{\rm ch~jet} \geq 10$ ${\rm GeV}/c$ and D$^0$ mesons with $p_{\rm T}^{\rm D^{0}} \geq 5$ ${\rm GeV}/c$. In this D$^0$-meson-tagged jet measurement, three jet axis definitions, each with different sensitivities to soft, wide-angle radiation, are used -- the Standard axis, Soft Drop groomed axis, and Winner-Takes-All axis. Measurements of the radial distributions of D$^0$ mesons with respect to the jet axes, $\Delta R_{\mathrm{axis-D^0}}$, are reported, along with the angle, $\Delta R_{\mathrm{axis}}$, between the three jet axes. The D$^{0}$ meson emerges as the leading particle in these jets, closely aligning with the Winner-Takes-All axis and diverging from the Standard jet axis. The results also examine how varying the sensitivity to soft radiation with grooming influences the orientation of the Soft Drop jet axis, and uncover that charm-jet structure is more likely to survive grooming when the Soft Drop axis is further from the D$^{0}$ direction, providing further evidence of the dead-cone effect recently measured by ALICE.
DOI: 10.17182/hepdata.165764.v1/t14
title: "Table 14" of "D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV"

description: $\Delta R_{\rm axis}$ distribution for $\rm STD-SD$ with grooming setting ($z_{\rm cut} = 0.2, \beta = 0$) for $\rm D^0$-tagged jets of $R=0.4$, in the intervals $10
description: Heavy-flavor quarks produced in proton$\mathrm{-}$proton (pp) collisions provide a unique opportunity to investigate the evolution of quark-initiated parton showers from initial hard scatterings to final-state hadrons. By examining jets that contain heavy-flavor hadrons, this study explores the effects of both perturbative and non-perturbative QCD on jet formation and structure. The angular differences between various jet axes, $\Delta R_{\rm axis}$, offer insight into the radiation patterns and fragmentation of charm quarks. The first measurement of D$^{0}$-tagged jet axes differences in pp collisions at $\sqrt{s}=5.02$ TeV by the ALICE experiment at the LHC is presented for jets with transverse momentum $p_{\rm T}^{\rm ch~jet} \geq 10$ ${\rm GeV}/c$ and D$^0$ mesons with $p_{\rm T}^{\rm D^{0}} \geq 5$ ${\rm GeV}/c$. In this D$^0$-meson-tagged jet measurement, three jet axis definitions, each with different sensitivities to soft, wide-angle radiation, are used -- the Standard axis, Soft Drop groomed axis, and Winner-Takes-All axis. Measurements of the radial distributions of D$^0$ mesons with respect to the jet axes, $\Delta R_{\mathrm{axis-D^0}}$, are reported, along with the angle, $\Delta R_{\mathrm{axis}}$, between the three jet axes. The D$^{0}$ meson emerges as the leading particle in these jets, closely aligning with the Winner-Takes-All axis and diverging from the Standard jet axis. The results also examine how varying the sensitivity to soft radiation with grooming influences the orientation of the Soft Drop jet axis, and uncover that charm-jet structure is more likely to survive grooming when the Soft Drop axis is further from the D$^{0}$ direction, providing further evidence of the dead-cone effect recently measured by ALICE.
DOI: 10.17182/hepdata.165764.v1/t16
title: "Table 16" of "D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV"

description: $\Delta R_{\rm axis}$ distribution for the ratio of $\rm SD-D^0$ ($z_{\rm cut} = 0.2, \beta=0$) over $\rm SD-D^0$ ($z_{\rm cut} = 0.1, \beta=0$) for $\rm D^0$-tagged jets of $R=0.4$, in the intervals $10
description: Heavy-flavor quarks produced in proton$\mathrm{-}$proton (pp) collisions provide a unique opportunity to investigate the evolution of quark-initiated parton showers from initial hard scatterings to final-state hadrons. By examining jets that contain heavy-flavor hadrons, this study explores the effects of both perturbative and non-perturbative QCD on jet formation and structure. The angular differences between various jet axes, $\Delta R_{\rm axis}$, offer insight into the radiation patterns and fragmentation of charm quarks. The first measurement of D$^{0}$-tagged jet axes differences in pp collisions at $\sqrt{s}=5.02$ TeV by the ALICE experiment at the LHC is presented for jets with transverse momentum $p_{\rm T}^{\rm ch~jet} \geq 10$ ${\rm GeV}/c$ and D$^0$ mesons with $p_{\rm T}^{\rm D^{0}} \geq 5$ ${\rm GeV}/c$. In this D$^0$-meson-tagged jet measurement, three jet axis definitions, each with different sensitivities to soft, wide-angle radiation, are used -- the Standard axis, Soft Drop groomed axis, and Winner-Takes-All axis. Measurements of the radial distributions of D$^0$ mesons with respect to the jet axes, $\Delta R_{\mathrm{axis-D^0}}$, are reported, along with the angle, $\Delta R_{\mathrm{axis}}$, between the three jet axes. The D$^{0}$ meson emerges as the leading particle in these jets, closely aligning with the Winner-Takes-All axis and diverging from the Standard jet axis. The results also examine how varying the sensitivity to soft radiation with grooming influences the orientation of the Soft Drop jet axis, and uncover that charm-jet structure is more likely to survive grooming when the Soft Drop axis is further from the D$^{0}$ direction, providing further evidence of the dead-cone effect recently measured by ALICE.
DOI: 10.17182/hepdata.165764.v1/t9
title: "Table 9" of "D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV"

description: $\Delta R_{\rm axis}$ distribution for $\rm WTA-SD$ with grooming setting ($z_{\rm cut} = 0.1, \beta = 0$) for $\rm D^0$-tagged jets of $R=0.4$, in the intervals $10
description: Heavy-flavor quarks produced in proton$\mathrm{-}$proton (pp) collisions provide a unique opportunity to investigate the evolution of quark-initiated parton showers from initial hard scatterings to final-state hadrons. By examining jets that contain heavy-flavor hadrons, this study explores the effects of both perturbative and non-perturbative QCD on jet formation and structure. The angular differences between various jet axes, $\Delta R_{\rm axis}$, offer insight into the radiation patterns and fragmentation of charm quarks. The first measurement of D$^{0}$-tagged jet axes differences in pp collisions at $\sqrt{s}=5.02$ TeV by the ALICE experiment at the LHC is presented for jets with transverse momentum $p_{\rm T}^{\rm ch~jet} \geq 10$ ${\rm GeV}/c$ and D$^0$ mesons with $p_{\rm T}^{\rm D^{0}} \geq 5$ ${\rm GeV}/c$. In this D$^0$-meson-tagged jet measurement, three jet axis definitions, each with different sensitivities to soft, wide-angle radiation, are used -- the Standard axis, Soft Drop groomed axis, and Winner-Takes-All axis. Measurements of the radial distributions of D$^0$ mesons with respect to the jet axes, $\Delta R_{\mathrm{axis-D^0}}$, are reported, along with the angle, $\Delta R_{\mathrm{axis}}$, between the three jet axes. The D$^{0}$ meson emerges as the leading particle in these jets, closely aligning with the Winner-Takes-All axis and diverging from the Standard jet axis. The results also examine how varying the sensitivity to soft radiation with grooming influences the orientation of the Soft Drop jet axis, and uncover that charm-jet structure is more likely to survive grooming when the Soft Drop axis is further from the D$^{0}$ direction, providing further evidence of the dead-cone effect recently measured by ALICE.
DOI: 10.17182/hepdata.101355.v1/t1
title: "Figure 2" of "Constraining the initial conditions and temperature dependent transport with three-particle correlations in Au+Au collisions"

description: Dependence of mixed harmonic correlators $C_{1,2,3}$ and $C_{2,2,4}$ on relative pseudorapidity.
description: No data abstract available.
DOI: 10.17182/hepdata.105868.v1/t1
title: "Table 1" of "Transverse spin-dependent azimuthal correlations of charged pion pairs measured in p$^\uparrow$+p collisions at $\sqrt{s}$ = 500 GeV"

description: Squared 4-momentum transfer $Q^2$ vs x coverage of STAR .
description: No data abstract available.
DOI: 10.17182/hepdata.128137.v1/t1
title: "Table 1" of "Measurement of the groomed jet radius and momentum splitting fraction in pp and Pb$-$Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Groomed jet momentum splitting fraction $z_{{\mathrm{g}}}$ in pp collisions.
$60
description: No data abstract available.
DOI: 10.17182/hepdata.128137.v1/t2
title: "Table 2" of "Measurement of the groomed jet radius and momentum splitting fraction in pp and Pb$-$Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Groomed jet momentum splitting fraction $z_{{\mathrm{g}}}$ in Pb-Pb collisions.
$60
description: No data abstract available.
DOI: 10.17182/hepdata.128137.v1/t3
title: "Table 3" of "Measurement of the groomed jet radius and momentum splitting fraction in pp and Pb$-$Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Groomed jet momentum splitting fraction $z_{{\mathrm{g}}}$ $-$ ratio of Pb-Pb to pp collisions.
$60
description: No data abstract available.
DOI: 10.17182/hepdata.128137.v1/t4
title: "Table 13" of "Measurement of the groomed jet radius and momentum splitting fraction in pp and Pb$-$Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Groomed jet momentum splitting fraction $z_{{\mathrm{g}}}$ in pp collisions.
$80
description: No data abstract available.
DOI: 10.17182/hepdata.165764.v1/t15
title: "Table 15" of "D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV"

description: $\Delta R_{\rm axis}$ distribution for the ratio of $\rm STD-SD$ ($z_{\rm cut} = 0.2, \beta=0$) over $\rm STD-SD$ ($z_{\rm cut} = 0.1, \beta=0$) for $\rm D^0$-tagged jets of $R=0.4$, in the intervals $10
description: Heavy-flavor quarks produced in proton$\mathrm{-}$proton (pp) collisions provide a unique opportunity to investigate the evolution of quark-initiated parton showers from initial hard scatterings to final-state hadrons. By examining jets that contain heavy-flavor hadrons, this study explores the effects of both perturbative and non-perturbative QCD on jet formation and structure. The angular differences between various jet axes, $\Delta R_{\rm axis}$, offer insight into the radiation patterns and fragmentation of charm quarks. The first measurement of D$^{0}$-tagged jet axes differences in pp collisions at $\sqrt{s}=5.02$ TeV by the ALICE experiment at the LHC is presented for jets with transverse momentum $p_{\rm T}^{\rm ch~jet} \geq 10$ ${\rm GeV}/c$ and D$^0$ mesons with $p_{\rm T}^{\rm D^{0}} \geq 5$ ${\rm GeV}/c$. In this D$^0$-meson-tagged jet measurement, three jet axis definitions, each with different sensitivities to soft, wide-angle radiation, are used -- the Standard axis, Soft Drop groomed axis, and Winner-Takes-All axis. Measurements of the radial distributions of D$^0$ mesons with respect to the jet axes, $\Delta R_{\mathrm{axis-D^0}}$, are reported, along with the angle, $\Delta R_{\mathrm{axis}}$, between the three jet axes. The D$^{0}$ meson emerges as the leading particle in these jets, closely aligning with the Winner-Takes-All axis and diverging from the Standard jet axis. The results also examine how varying the sensitivity to soft radiation with grooming influences the orientation of the Soft Drop jet axis, and uncover that charm-jet structure is more likely to survive grooming when the Soft Drop axis is further from the D$^{0}$ direction, providing further evidence of the dead-cone effect recently measured by ALICE.
DOI: 10.17182/hepdata.105868.v1/t2
title: "Table 2" of "Transverse spin-dependent azimuthal correlations of charged pion pairs measured in p$^\uparrow$+p collisions at $\sqrt{s}$ = 500 GeV"

description: $A_{UT}$ as a function of $\eta$ for $$ = 13 GeV/c and $$ = 1 GeV/($c^2$) (Upper panel of the fig. 3). Kinematic variables $$, $$ as a function of $\eta$ for $$ = 13 GeV/c and $$ = 1 GeV/($c^2$) (Lower panel of the fig. 3). In addition to statistical uncertainties, systematic uncertainties originating from PID and trigger bias systematic uncertainties are also mentioned for $A_{UT}$.
description: No data abstract available.
DOI: 10.17182/hepdata.105868.v1/t3
title: "Table 3" of "Transverse spin-dependent azimuthal correlations of charged pion pairs measured in p$^\uparrow$+p collisions at $\sqrt{s}$ = 500 GeV"

description: $A_{UT}$ as a function of $$ for pT bin $$ = 4 GeV/c for $\eta &gt; 0$ and $\eta &lt; 0$. In addition to statistical uncertainties, systematic uncertainties originating from PID and trigger bias systematic uncertainties are also mentioned.
description: No data abstract available.
DOI: 10.17182/hepdata.128137.v1/t5
title: "Table 14" of "Measurement of the groomed jet radius and momentum splitting fraction in pp and Pb$-$Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Groomed jet momentum splitting fraction $z_{{\mathrm{g}}}$ in Pb-Pb collisions.
$80
description: No data abstract available.
DOI: 10.17182/hepdata.128137.v1/t6
title: "Table 15" of "Measurement of the groomed jet radius and momentum splitting fraction in pp and Pb$-$Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Groomed jet momentum splitting fraction $z_{{\mathrm{g}}}$ $-$ ratio of Pb-Pb to pp collisions.
$80
description: No data abstract available.
DOI: 10.17182/hepdata.128137.v1/t7
title: "Table 7" of "Measurement of the groomed jet radius and momentum splitting fraction in pp and Pb$-$Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Groomed jet radius (scaled) $\theta_{{\mathrm{g}}}$ in pp collisions.
$60
description: No data abstract available.
DOI: 10.17182/hepdata.105868.v1/t4
title: "Table 4" of "Transverse spin-dependent azimuthal correlations of charged pion pairs measured in p$^\uparrow$+p collisions at $\sqrt{s}$ = 500 GeV"

description: $A_{UT}$ as a function of $$ for pT bin $$ = 5 GeV/c for $\eta &gt; 0$ and $\eta &lt; 0$. In addition to statistical uncertainties, systematic uncertainties originating from PID and trigger bias systematic uncertainties are also mentioned.
description: No data abstract available.
DOI: 10.17182/hepdata.105868.v1/t5
title: "Table 5" of "Transverse spin-dependent azimuthal correlations of charged pion pairs measured in p$^\uparrow$+p collisions at $\sqrt{s}$ = 500 GeV"

description: $A_{UT}$ as a function of $$ for pT bin $$ = 6 GeV/c for $\eta &gt; 0$ and $\eta &lt; 0$. In addition to statistical uncertainties, systematic uncertainties originating from PID and trigger bias systematic uncertainties are also mentioned.
description: No data abstract available.
DOI: 10.17182/hepdata.105868.v1/t6
title: "Table 6" of "Transverse spin-dependent azimuthal correlations of charged pion pairs measured in p$^\uparrow$+p collisions at $\sqrt{s}$ = 500 GeV"

description: $A_{UT}$ as a function of $$ for pT bin $$ = 8 GeV/c for $\eta &gt; 0$ and $\eta &lt; 0$. In addition to statistical uncertainties, systematic uncertainties originating from PID and trigger bias systematic uncertainties are also mentioned.
description: No data abstract available.
DOI: 10.17182/hepdata.128137.v1/t10
title: "Table 4" of "Measurement of the groomed jet radius and momentum splitting fraction in pp and Pb$-$Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Groomed jet momentum splitting fraction $z_{{\mathrm{g}}}$ in pp collisions.
$60
description: No data abstract available.
DOI: 10.17182/hepdata.128137.v1/t11
title: "Table 5" of "Measurement of the groomed jet radius and momentum splitting fraction in pp and Pb$-$Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Groomed jet momentum splitting fraction $z_{{\mathrm{g}}}$ in Pb-Pb collisions.
$60
description: No data abstract available.
DOI: 10.17182/hepdata.128137.v1/t12
title: "Table 6" of "Measurement of the groomed jet radius and momentum splitting fraction in pp and Pb$-$Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Groomed jet momentum splitting fraction $z_{{\mathrm{g}}}$ $-$ ratio of Pb-Pb to pp collisions.
$60
description: No data abstract available.
DOI: 10.17182/hepdata.128137.v1/t8
title: "Table 8" of "Measurement of the groomed jet radius and momentum splitting fraction in pp and Pb$-$Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Groomed jet radius (scaled) $\theta_{{\mathrm{g}}}$ in Pb-Pb collisions.
$60
description: No data abstract available.
DOI: 10.17182/hepdata.105868.v1/t7
title: "Table 7" of "Transverse spin-dependent azimuthal correlations of charged pion pairs measured in p$^\uparrow$+p collisions at $\sqrt{s}$ = 500 GeV"

description: $A_{UT}$ as a function of $$ for pT bin $$ = 13 GeV/c for $\eta &gt; 0$ and $\eta &lt; 0$. In addition to statistical uncertainties, systematic uncertainties originating from PID and trigger bias systematic uncertainties are also mentioned.
description: No data abstract available.
DOI: 10.17182/hepdata.105868.v1/t8
title: "Table 8" of "Transverse spin-dependent azimuthal correlations of charged pion pairs measured in p$^\uparrow$+p collisions at $\sqrt{s}$ = 500 GeV"

description: Same-charge, momentum ordered asymmetry $A_{UT}$ as a function of $$ for pT bin $$ = 4 GeV/c for $\eta &gt; 0$. In addition to statistical uncertainties, systematic uncertainties originating from PID and trigger bias systematic uncertainties are also mentioned.
description: No data abstract available.
DOI: 10.17182/hepdata.105868.v1/t9
title: "Table 9" of "Transverse spin-dependent azimuthal correlations of charged pion pairs measured in p$^\uparrow$+p collisions at $\sqrt{s}$ = 500 GeV"

description: Same-charge, momentum ordered asymmetry $A_{UT}$ as a function of $$ for pT bin $$ = 6 GeV/c for $\eta &gt; 0$. In addition to statistical uncertainties, systematic uncertainties originating from PID and trigger bias systematic uncertainties are also mentioned.
description: No data abstract available.
DOI: 10.17182/hepdata.128137.v1/t9
title: "Table 9" of "Measurement of the groomed jet radius and momentum splitting fraction in pp and Pb$-$Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Groomed jet radius (scaled) $\theta_{{\mathrm{g}}}$ $-$ ratio of Pb-Pb to pp collisions.
$60
description: No data abstract available.
DOI: 10.17182/hepdata.105868.v1/t10
title: "Table 10" of "Transverse spin-dependent azimuthal correlations of charged pion pairs measured in p$^\uparrow$+p collisions at $\sqrt{s}$ = 500 GeV"

description: Same-charge, momentum ordered asymmetry $A_{UT}$ as a function of $$ for pT bin $$ = 13 GeV/c for $\eta &gt; 0$. In addition to statistical uncertainties, systematic uncertainties originating from PID and trigger bias systematic uncertainties are also mentioned.
description: No data abstract available.
DOI: 10.17182/hepdata.105868.v1/t11
title: "Table 11" of "Transverse spin-dependent azimuthal correlations of charged pion pairs measured in p$^\uparrow$+p collisions at $\sqrt{s}$ = 500 GeV"

description: $A_{UT}$ as a function of $$ for $$ = 0.4 GeV/$c^{2}$ for $\eta &gt; 0$. In addition to statistical uncertainties, systematic uncertainties originating from PID and trigger bias systematic uncertainties are also mentioned. The systematic uncertainty numbers marked with (*) are based on marker size, and may not reflect actual experimental uncertainties.
description: No data abstract available.
DOI: 10.17182/hepdata.105868.v1/t12
title: "Table 12" of "Transverse spin-dependent azimuthal correlations of charged pion pairs measured in p$^\uparrow$+p collisions at $\sqrt{s}$ = 500 GeV"

description: $A_{UT}$ as a function of $$ for $$ = 0.5 GeV/$c^{2}$ for $\eta &gt; 0$. In addition to statistical uncertainties, systematic uncertainties originating from PID and trigger bias systematic uncertainties are also mentioned. The systematic uncertainty numbers marked with (*) are based on marker size, and may not reflect actual experimental uncertainties.
description: No data abstract available.
DOI: 10.17182/hepdata.128137.v1/t13
title: "Table 10" of "Measurement of the groomed jet radius and momentum splitting fraction in pp and Pb$-$Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Groomed jet radius (scaled) $\theta_{{\mathrm{g}}}$ in pp collisions.
$60
description: No data abstract available.
DOI: 10.17182/hepdata.128137.v1/t14
title: "Table 11" of "Measurement of the groomed jet radius and momentum splitting fraction in pp and Pb$-$Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Groomed jet radius (scaled) $\theta_{{\mathrm{g}}}$ in Pb-Pb collisions.
$60
description: No data abstract available.
DOI: 10.17182/hepdata.128137.v1/t15
title: "Table 12" of "Measurement of the groomed jet radius and momentum splitting fraction in pp and Pb$-$Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Groomed jet radius (scaled) $\theta_{{\mathrm{g}}}$ $-$ ratio of Pb-Pb to pp collisions.
$60
description: No data abstract available.
DOI: 10.17182/hepdata.128137.v1/t16
title: "Table 16" of "Measurement of the groomed jet radius and momentum splitting fraction in pp and Pb$-$Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Groomed jet radius (scaled) $\theta_{{\mathrm{g}}}$ in pp collisions.
$60
description: No data abstract available.
DOI: 10.17182/hepdata.128137.v1/t17
title: "Table 17" of "Measurement of the groomed jet radius and momentum splitting fraction in pp and Pb$-$Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Groomed jet radius (scaled) $\theta_{{\mathrm{g}}}$ in Pb-Pb collisions.
$60
description: No data abstract available.
DOI: 10.17182/hepdata.105868.v1/t13
title: "Table 13" of "Transverse spin-dependent azimuthal correlations of charged pion pairs measured in p$^\uparrow$+p collisions at $\sqrt{s}$ = 500 GeV"

description: $A_{UT}$ as a function of $$ for $$ = 0.6 GeV/$c^{2}$ for $\eta &gt; 0$. In addition to statistical uncertainties, systematic uncertainties originating from PID and trigger bias systematic uncertainties are also mentioned. The systematic uncertainty numbers marked with (*) are based on marker size, and may not reflect actual experimental uncertainties.
description: No data abstract available.
DOI: 10.17182/hepdata.105868.v1/t14
title: "Table 14" of "Transverse spin-dependent azimuthal correlations of charged pion pairs measured in p$^\uparrow$+p collisions at $\sqrt{s}$ = 500 GeV"

description: $A_{UT}$ as a function of $$ for $$ = 0.7 GeV/$c^{2}$ for $\eta &gt; 0$. In addition to statistical uncertainties, systematic uncertainties originating from PID and trigger bias systematic uncertainties are also mentioned. The systematic uncertainty numbers marked with (*) are based on marker size, and may not reflect actual experimental uncertainties.
description: No data abstract available.