cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.102321.v1/t12
title: "Figure 3.0" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: Kinetic freeze-out temperature and transverse flow velocity obtained from the fits to $m_T$ spectra for 0-10% centrality.
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102321.v1/t13
title: "Figure 3.1" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: Kinetic freeze-out temperature and transverse flow velocity of $\Xi^-+\bar{\Xi}^+$ (1$\sigma$ contour).
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102321.v1/t14
title: "Figure 3.2" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: Kinetic freeze-out temperature and transverse flow velocity of $\Xi^-+\bar{\Xi}^+$ (2$\sigma$ contour).
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102321.v1/t15
title: "Figure 3.3" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: Kinetic freeze-out temperature and transverse flow velocity of $\Xi^-+\bar{\Xi}^+$ (3$\sigma$ contour).
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102321.v1/t16
title: "Figure 3.4" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: Kinetic freeze-out temperature and transverse flow velocity of $\pi$, $K$, $p$, $\Lambda$ (1$\sigma$ contour).
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102321.v1/t17
title: "Figure 3.5" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: Kinetic freeze-out temperature and transverse flow velocity of $\pi$, $K$, $p$, $\Lambda$ (2$\sigma$ contour).
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102321.v1/t18
title: "Figure 3.6" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: Kinetic freeze-out temperature and transverse flow velocity of $\pi$, $K$, $p$, $\Lambda$ (3$\sigma$ contour).
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102321.v1/t19
title: "Figure 3.7" of "Multi-strange baryon production in Au Au collisions at s(NN)**(1/2) = 130-GeV."

description: Mean transverse momentum $\langle p_T \rangle$. Results from best fits to spectra, Bose-Einstein for $\pi$, exponential for $K$, hydrodynamically-inspired function for $p$, and Boltzmann for $\Lambda$, $\Xi$, and $\Omega$.
description: The transverse mass spectra and midrapidity yields for $\Xi$s and $\Omega$s are presented. For the 10% most central collisions, the $\bar{\Xi}^+/h^-$ ratio increases from the Super Proton Synchrotron to the Relativistic Heavy Ion Collider energies while the $\Xi^-/h^-$ stays approximately constant. A hydrodynamically inspired model fit to the $\Xi$ spectra, which assumes a thermalized source, seems to indicate that these multistrange particles experience a significant transverse flow effect, but are emitted when the system is hotter and the flow is smaller than values obtained from a combined fit to $\pi$, $K$, $p$, and $\Lambda$s.
DOI: 10.17182/hepdata.102322.v1/t1
title: "Figure 1.0" of "Azimuthal anisotropy at RHIC: The first and fourth harmonics."

description: $v_1$ of charged particles as a function of pseudorapidity for 10-70% centrality. Non-flow systematic uncertainties are approximately 20%.
description: We report the first observations of the first harmonic (directed flow, $v_1$) and the fourth harmonic ($v_4$), in the azimuthal distribution of particles with respect to the reaction plane in Au+Au collisions at the BNL Relativistic Heavy Ion Collider (RHIC). Both measurements were done taking advantage of the large elliptic flow ($v_2$) generated at RHIC. From the correlation of $v_2$ with $v_1$ it is demonstrated that $v_2$ is positive, or $in$-$plane$. The integrated $v_4$ is is about a factor of 10 smaller than $v_2$. For the sixth ($v_6$) and eighth ($v_8$) harmonics upper limits on the magnitudes are reported. An erratum of this paper can be found in Phys.Rev.Lett.127.069901 (2021).
DOI: 10.17182/hepdata.102322.v1/t2
title: "Figure 2.0" of "Azimuthal anisotropy at RHIC: The first and fourth harmonics."

description: $v_2$ with respect to the second harmonic event plane as a function of $p_T$ for the minimum bias Au+Au collisions. Background from secondary particles is expected to be less than 15%. Non-flow systematic uncertainties are approximately 20%. Fluctuations in initial geometry can lead to an effect of about a factor of 1.2 to 1.5.
description: We report the first observations of the first harmonic (directed flow, $v_1$) and the fourth harmonic ($v_4$), in the azimuthal distribution of particles with respect to the reaction plane in Au+Au collisions at the BNL Relativistic Heavy Ion Collider (RHIC). Both measurements were done taking advantage of the large elliptic flow ($v_2$) generated at RHIC. From the correlation of $v_2$ with $v_1$ it is demonstrated that $v_2$ is positive, or $in$-$plane$. The integrated $v_4$ is is about a factor of 10 smaller than $v_2$. For the sixth ($v_6$) and eighth ($v_8$) harmonics upper limits on the magnitudes are reported. An erratum of this paper can be found in Phys.Rev.Lett.127.069901 (2021).
DOI: 10.17182/hepdata.102322.v1/t3
title: "Figure 2.1" of "Azimuthal anisotropy at RHIC: The first and fourth harmonics."

description: $v_4$ with respect to the second harmonic event plane as a function of $p_T$ for the minimum bias Au+Au collisions. Background from secondary particles is expected to be less than 15%. Non-flow systematic uncertainties are approximately 20%. Fluctuations in initial geometry can lead to an effect of about a factor of 1.2 to 1.5.
description: We report the first observations of the first harmonic (directed flow, $v_1$) and the fourth harmonic ($v_4$), in the azimuthal distribution of particles with respect to the reaction plane in Au+Au collisions at the BNL Relativistic Heavy Ion Collider (RHIC). Both measurements were done taking advantage of the large elliptic flow ($v_2$) generated at RHIC. From the correlation of $v_2$ with $v_1$ it is demonstrated that $v_2$ is positive, or $in$-$plane$. The integrated $v_4$ is is about a factor of 10 smaller than $v_2$. For the sixth ($v_6$) and eighth ($v_8$) harmonics upper limits on the magnitudes are reported. An erratum of this paper can be found in Phys.Rev.Lett.127.069901 (2021).
DOI: 10.17182/hepdata.102322.v1/t4
title: "Figure 2.2" of "Azimuthal anisotropy at RHIC: The first and fourth harmonics."

description: $v_4$ from three particle cumulant as a function of $p_T$ for the minimum bias Au+Au collisions. Background from secondary particles is expected to be less than 15%. Non-flow systematic uncertainties are approximately 20%. Fluctuations in initial geometry can lead to an effect of about a factor of 1.2 to 1.5.
description: We report the first observations of the first harmonic (directed flow, $v_1$) and the fourth harmonic ($v_4$), in the azimuthal distribution of particles with respect to the reaction plane in Au+Au collisions at the BNL Relativistic Heavy Ion Collider (RHIC). Both measurements were done taking advantage of the large elliptic flow ($v_2$) generated at RHIC. From the correlation of $v_2$ with $v_1$ it is demonstrated that $v_2$ is positive, or $in$-$plane$. The integrated $v_4$ is is about a factor of 10 smaller than $v_2$. For the sixth ($v_6$) and eighth ($v_8$) harmonics upper limits on the magnitudes are reported. An erratum of this paper can be found in Phys.Rev.Lett.127.069901 (2021).
DOI: 10.17182/hepdata.102322.v1/t5
title: "Figure 2.3" of "Azimuthal anisotropy at RHIC: The first and fourth harmonics."

description: $v_6$ with respect to the second harmonic event plane as a function of $p_T$ for the minimum bias Au+Au collisions. Background from secondary particles is expected to be less than 15%. Non-flow systematic uncertainties are approximately 20%. Fluctuations in initial geometry can lead to an effect of about a factor of 1.2 to 1.5.
description: We report the first observations of the first harmonic (directed flow, $v_1$) and the fourth harmonic ($v_4$), in the azimuthal distribution of particles with respect to the reaction plane in Au+Au collisions at the BNL Relativistic Heavy Ion Collider (RHIC). Both measurements were done taking advantage of the large elliptic flow ($v_2$) generated at RHIC. From the correlation of $v_2$ with $v_1$ it is demonstrated that $v_2$ is positive, or $in$-$plane$. The integrated $v_4$ is is about a factor of 10 smaller than $v_2$. For the sixth ($v_6$) and eighth ($v_8$) harmonics upper limits on the magnitudes are reported. An erratum of this paper can be found in Phys.Rev.Lett.127.069901 (2021).
DOI: 10.17182/hepdata.102322.v1/t6
title: "Figure 3.0" of "Azimuthal anisotropy at RHIC: The first and fourth harmonics."

description: $p_T$- and $\eta$-integrated $v_2$, $v_4$, $v_6$ as a function of centrality. Background from secondary particles is expected to be less than 15%. Non-flow systematic uncertainties are approximately 20%. Fluctuations in initial geometry can lead to an effect of about a factor of 1.2 to 1.5.
description: We report the first observations of the first harmonic (directed flow, $v_1$) and the fourth harmonic ($v_4$), in the azimuthal distribution of particles with respect to the reaction plane in Au+Au collisions at the BNL Relativistic Heavy Ion Collider (RHIC). Both measurements were done taking advantage of the large elliptic flow ($v_2$) generated at RHIC. From the correlation of $v_2$ with $v_1$ it is demonstrated that $v_2$ is positive, or $in$-$plane$. The integrated $v_4$ is is about a factor of 10 smaller than $v_2$. For the sixth ($v_6$) and eighth ($v_8$) harmonics upper limits on the magnitudes are reported. An erratum of this paper can be found in Phys.Rev.Lett.127.069901 (2021).
DOI: 10.17182/hepdata.102351.v1/t1
title: "data table 0" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: red data points
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t2
title: "data table 1" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: black histogram
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t4
title: "data table 3" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with default flow Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t5
title: "data table 4" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with default flow Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t7
title: "data table 6" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with default flow Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t8
title: "data table 7" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with default flow Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t9
title: "data table 8" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with default flow Au+Au 20-60%, 3
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t10
title: "data table 9" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with default flow Au+Au 20-60%, 3
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t11
title: "data table 10" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with default flow Au+Au 20-60%, 3
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t3
title: "data table 2" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with default flow Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t6
title: "data table 5" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with default flow Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t12
title: "data table 11" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with default flow Au+Au 20-60%, 3
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t13
title: "data table 12" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with default flow Au+Au 20-60%, 3
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t14
title: "data table 13" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with default flow Au+Au 20-60%, 3
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t15
title: "data table 14" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with upper flow systematic uncertainty Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t16
title: "data table 15" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with upper flow systematic uncertainty Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t17
title: "data table 16" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with upper flow systematic uncertainty Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t18
title: "data table 17" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with upper flow systematic uncertainty Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t19
title: "data table 18" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with upper flow systematic uncertainty Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t20
title: "data table 19" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with upper flow systematic uncertainty Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t22
title: "data table 21" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with upper flow systematic uncertainty Au+Au 20-60%, 3
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t23
title: "data table 22" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with upper flow systematic uncertainty Au+Au 20-60%, 3
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t26
title: "data table 25" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with upper flow systematic uncertainty Au+Au 20-60%, 3
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t27
title: "data table 26" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with lower flow systematic uncertainty Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t28
title: "data table 27" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with lower flow systematic uncertainty Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t24
title: "data table 23" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with upper flow systematic uncertainty Au+Au 20-60%, 3
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t25
title: "data table 24" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with upper flow systematic uncertainty Au+Au 20-60%, 3
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t29
title: "data table 28" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with lower flow systematic uncertainty Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t30
title: "data table 29" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with lower flow systematic uncertainty Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t21
title: "data table 20" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with upper flow systematic uncertainty Au+Au 20-60%, 3
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t31
title: "data table 30" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with lower flow systematic uncertainty Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t32
title: "data table 31" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with lower flow systematic uncertainty Au+Au 20-60%, 4
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t33
title: "data table 32" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with lower flow systematic uncertainty Au+Au 20-60%, 3
description: No data abstract available.
DOI: 10.17182/hepdata.102351.v1/t34
title: "data table 33" of "Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV"

description: flow background with lower flow systematic uncertainty Au+Au 20-60%, 3
description: No data abstract available.