cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.93229.v1/t47
title: "Table 47" of "Jet-hadron correlations measured relative to the second order event plane in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Correlation functions in signal plus background region for $4.0
description: CERN-LHC. The Quark Gluon Plasma (QGP) produced in ultra relativistic heavy-ion collisions at the Large Hadron Collider (LHC) can be studied by measuring the modifications of jets formed by hard scattered partons which interact with the medium. We studied these modifications via angular correlations of jets with charged hadrons for jets with momenta $20
DOI: 10.17182/hepdata.93229.v1/t48
title: "Table 48" of "Jet-hadron correlations measured relative to the second order event plane in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Correlation functions in signal plus background region for $4.0
description: CERN-LHC. The Quark Gluon Plasma (QGP) produced in ultra relativistic heavy-ion collisions at the Large Hadron Collider (LHC) can be studied by measuring the modifications of jets formed by hard scattered partons which interact with the medium. We studied these modifications via angular correlations of jets with charged hadrons for jets with momenta $20
DOI: 10.17182/hepdata.93229.v1/t50
title: "Table 50" of "Jet-hadron correlations measured relative to the second order event plane in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Correlation functions in signal plus background region for $4.0
description: CERN-LHC. The Quark Gluon Plasma (QGP) produced in ultra relativistic heavy-ion collisions at the Large Hadron Collider (LHC) can be studied by measuring the modifications of jets formed by hard scattered partons which interact with the medium. We studied these modifications via angular correlations of jets with charged hadrons for jets with momenta $20
DOI: 10.17182/hepdata.93229.v1/t49
title: "Table 49" of "Jet-hadron correlations measured relative to the second order event plane in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Correlation functions in signal plus background region for $4.0
description: CERN-LHC. The Quark Gluon Plasma (QGP) produced in ultra relativistic heavy-ion collisions at the Large Hadron Collider (LHC) can be studied by measuring the modifications of jets formed by hard scattered partons which interact with the medium. We studied these modifications via angular correlations of jets with charged hadrons for jets with momenta $20
DOI: 10.17182/hepdata.93229.v1/t51
title: "Table 51" of "Jet-hadron correlations measured relative to the second order event plane in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Correlation functions in signal plus background region for $5.0
description: CERN-LHC. The Quark Gluon Plasma (QGP) produced in ultra relativistic heavy-ion collisions at the Large Hadron Collider (LHC) can be studied by measuring the modifications of jets formed by hard scattered partons which interact with the medium. We studied these modifications via angular correlations of jets with charged hadrons for jets with momenta $20
DOI: 10.17182/hepdata.93229.v1/t52
title: "Table 52" of "Jet-hadron correlations measured relative to the second order event plane in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Correlation functions in signal plus background region for $5.0
description: CERN-LHC. The Quark Gluon Plasma (QGP) produced in ultra relativistic heavy-ion collisions at the Large Hadron Collider (LHC) can be studied by measuring the modifications of jets formed by hard scattered partons which interact with the medium. We studied these modifications via angular correlations of jets with charged hadrons for jets with momenta $20
DOI: 10.17182/hepdata.93229.v1/t53
title: "Table 53" of "Jet-hadron correlations measured relative to the second order event plane in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Correlation functions in signal plus background region for $5.0
description: CERN-LHC. The Quark Gluon Plasma (QGP) produced in ultra relativistic heavy-ion collisions at the Large Hadron Collider (LHC) can be studied by measuring the modifications of jets formed by hard scattered partons which interact with the medium. We studied these modifications via angular correlations of jets with charged hadrons for jets with momenta $20
DOI: 10.17182/hepdata.93229.v1/t54
title: "Table 54" of "Jet-hadron correlations measured relative to the second order event plane in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Correlation functions in signal plus background region for $5.0
description: CERN-LHC. The Quark Gluon Plasma (QGP) produced in ultra relativistic heavy-ion collisions at the Large Hadron Collider (LHC) can be studied by measuring the modifications of jets formed by hard scattered partons which interact with the medium. We studied these modifications via angular correlations of jets with charged hadrons for jets with momenta $20
DOI: 10.17182/hepdata.93229.v1/t55
title: "Table 55" of "Jet-hadron correlations measured relative to the second order event plane in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Correlation functions in signal plus background region for $6.0
description: CERN-LHC. The Quark Gluon Plasma (QGP) produced in ultra relativistic heavy-ion collisions at the Large Hadron Collider (LHC) can be studied by measuring the modifications of jets formed by hard scattered partons which interact with the medium. We studied these modifications via angular correlations of jets with charged hadrons for jets with momenta $20
DOI: 10.17182/hepdata.93229.v1/t56
title: "Table 56" of "Jet-hadron correlations measured relative to the second order event plane in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Correlation functions in signal plus background region for $6.0
description: CERN-LHC. The Quark Gluon Plasma (QGP) produced in ultra relativistic heavy-ion collisions at the Large Hadron Collider (LHC) can be studied by measuring the modifications of jets formed by hard scattered partons which interact with the medium. We studied these modifications via angular correlations of jets with charged hadrons for jets with momenta $20
DOI: 10.17182/hepdata.93229.v1/t57
title: "Table 57" of "Jet-hadron correlations measured relative to the second order event plane in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Correlation functions in signal plus background region for $6.0
description: CERN-LHC. The Quark Gluon Plasma (QGP) produced in ultra relativistic heavy-ion collisions at the Large Hadron Collider (LHC) can be studied by measuring the modifications of jets formed by hard scattered partons which interact with the medium. We studied these modifications via angular correlations of jets with charged hadrons for jets with momenta $20
DOI: 10.17182/hepdata.93229.v1/t58
title: "Table 58" of "Jet-hadron correlations measured relative to the second order event plane in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV"

description: Correlation functions in signal plus background region for $6.0
description: CERN-LHC. The Quark Gluon Plasma (QGP) produced in ultra relativistic heavy-ion collisions at the Large Hadron Collider (LHC) can be studied by measuring the modifications of jets formed by hard scattered partons which interact with the medium. We studied these modifications via angular correlations of jets with charged hadrons for jets with momenta $20
DOI: 10.17182/hepdata.93232.v1/t1
title: "Table 1" of "Elliptic flow in Au + Au collisions at s(N N)**(1/2) = 130-GeV."

description: Elliptic flow as a function of centrality defined as nch/nmax. Also given is epsilon, the initial space eccentricity of the overlap region, as well as the cumulative fraction of events starting with the most central. From the results of the study of non-flow contributions by different subevent selections and the maximum magnitudes of the first and higher-order harmonics, we estimate a systematic error for v2 of about 0.007, with somewhat smaller uncertainty for the mid-centralities where the resolution of the event plane is high.
description: No data abstract available.
DOI: 10.17182/hepdata.93232.v1/t2
title: "Table 2" of "Elliptic flow in Au + Au collisions at s(N N)**(1/2) = 130-GeV."

description: Elliptic flow as a function of transverse momen-tum for minimum bias events
description: No data abstract available.
DOI: 10.17182/hepdata.93260.v1/t1
title: "Table 1.1" of "Particle dependence of azimuthal anisotropy and nuclear modification of particle production at moderate p(T) in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The minimum bias (0-80% of the collision cross-section) v2(pT) of K0s. Errors listed include statistical and point-to-point systematic uncertainties from the background. Additional non-flow systematic uncertainties are approximately -20%.
description: No data abstract available.
DOI: 10.17182/hepdata.93260.v1/t2
title: "Table 1.2" of "Particle dependence of azimuthal anisotropy and nuclear modification of particle production at moderate p(T) in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The minimum bias (0-80% of the collision cross-section) v2(pT) of Lambda+Lambdabar. Errors listed include statistical and point-to-point systematic uncertainties from the background. Additional non-flow systematic uncertainties are approximately -20%.
description: No data abstract available.
DOI: 10.17182/hepdata.93260.v1/t3
title: "Table 1.3" of "Particle dependence of azimuthal anisotropy and nuclear modification of particle production at moderate p(T) in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The minimum bias (0-80% of the collision cross-section) v2(pT) of charged hadrons. Errors listed include statistical and point-to-point systematic uncertainties from the background. Additional non-flow systematic uncertainties are approximately -20%.
description: No data abstract available.
DOI: 10.17182/hepdata.93260.v1/t4
title: "Table 2.1" of "Particle dependence of azimuthal anisotropy and nuclear modification of particle production at moderate p(T) in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The v2 of KS0 as a function of pT for 30%–70%, 5%–30%, and 0%–5% of the collision cross section. The error bars represent statistical errors only. The nonflow systematic errors for the 30%–70%, 5%– 30%, and 0%–5% centralities are 25%, 20%, and 80%, respectively.
description: No data abstract available.
DOI: 10.15468/dl.qzqdtt
title: Occurrence Download

description: A dataset containing 568 species occurrences available in GBIF matching the query:
{
 "and" : [
 "Geometry POLYGON((-71.34184 41.85657,-71.34184 41.89971,-71.42174 41.89971,-71.42174 41.85657,-71.34184 41.85657))",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "OccurrenceStatus is Present",
 "TaxonKey is Magnoliopsida"
 ]
}

 The dataset includes 568 records from 15 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015779-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.93260.v1/t5
title: "Table 2.2" of "Particle dependence of azimuthal anisotropy and nuclear modification of particle production at moderate p(T) in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The v2 of Lambda+Lambdabar as a function of pT for 30%–70%, 5%–30%, and 0%–5% of the collision cross section. The error bars represent statistical errors only. The nonflow systematic errors for the 30%–70%, 5%– 30%, and 0%–5% centralities are 25%, 20%, and 80%, respectively.
description: No data abstract available.
DOI: 10.17182/hepdata.93260.v1/t6
title: "Table 3.1" of "Particle dependence of azimuthal anisotropy and nuclear modification of particle production at moderate p(T) in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The ratio RCP for KS0 at midrapidity calculated using centrality intervals, 0%–5% vs 40%–60% and 0%–5% vs 60%–80% of the collision cross section. The error bars shown on the points include both statistical and systematic errors.
description: No data abstract available.
DOI: 10.17182/hepdata.93260.v1/t7
title: "Table 3.2" of "Particle dependence of azimuthal anisotropy and nuclear modification of particle production at moderate p(T) in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The ratio RCP for Lambda+Lambdabar at midrapidity calculated using centrality intervals, 0%–5% vs 40%–60% and 0%–5% vs 60%–80% of the collision cross section. The error bars shown on the points include both statistical and systematic errors.
description: No data abstract available.
DOI: 10.17182/hepdata.93260.v1/t8
title: "Table 4.1" of "Particle dependence of azimuthal anisotropy and nuclear modification of particle production at moderate p(T) in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The v2 parameter for KS0 scaled by the number of constituent quarks (n) and plotted versus pT/n. The error bars shown include statistical and point-to-point systematic uncertainties from the background. The additional nonflow systematic uncertainties are approximately 20%.
description: No data abstract available.
DOI: 10.17182/hepdata.93260.v1/t9
title: "Table 4.2" of "Particle dependence of azimuthal anisotropy and nuclear modification of particle production at moderate p(T) in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The v2 parameter for Lambda+Lambdabar scaled by the number of constituent quarks (n) and plotted versus pT/n. The error bars shown include statistical and point-to-point systematic uncertainties from the background. The additional nonflow systematic uncertainties are approximately 20%.
description: No data abstract available.
DOI: 10.17182/hepdata.93261.v1/t2
title: "Table 1.2" of "Identified particle elliptic flow in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: Differential elliptic flow for protons + antiprotons for minimum-bias events, the systematic uncertainty for minimum-bias data is 13%.
description: No data abstract available.
DOI: 10.17182/hepdata.93261.v1/t1
title: "Table 1.1" of "Identified particle elliptic flow in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: Differential elliptic flow for pions for minimum-bias events, the systematic uncertainty for minimum-bias data is 13%.
description: No data abstract available.
DOI: 10.17182/hepdata.93261.v1/t3
title: "Table 1.3" of "Identified particle elliptic flow in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: Differential elliptic flow for kaons for minimum-bias events, the systematic uncertainty for minimum-bias data is 13%.
description: No data abstract available.
DOI: 10.17182/hepdata.93261.v1/t4
title: "Table 2.1" of "Identified particle elliptic flow in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: Differential elliptic flow of pions for different centrality bins. The systematic uncertainty is smallest for the centrality region with the best reaction plane resolution and is estimated to be 20% for the most central bin, 8% for the mid-central bin, and 22% for the most peripheral bin.
description: No data abstract available.
DOI: 10.17182/hepdata.93261.v1/t5
title: "Table 2.2" of "Identified particle elliptic flow in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: Differential elliptic flow of protons + antiprotons for different centrality bins. The systematic uncertainty is smallest for the centrality region with the best reaction plane resolution and is estimated to be 20% for the most central bin, 8% for the mid-central bin, and 22% for the most peripheral bin.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t1
title: "Figure 2_1" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Directed flow of charged hadrons v1{3} as a function of pseudorapidity for 10–70% centrality.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t2
title: "Figure 2_2" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Directed flow of charged hadrons v1 {EP1,EP2} as a function of pseudorapidity for 20–60% centrality.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t3
title: "Figure 4" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Charged hadron v2 for the centrality bins 5 to 10% and in steps of 10% starting at 10, 20, 30, 40, 50, 60, and 70 up to 80% along with min. bias as a function of p_T.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t4
title: "Figure 5" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Charged hadron v2 for the centrality bin 0-50%.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t5
title: "Figure 6_1" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: v2(4) vs. p_T for pions for 20 - 60% centrality
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t6
title: "Figure 6_2" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: v2(4) vs. p_T for kaons for 20 - 60% centrality
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t7
title: "Figure 6_3" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: v2(4) vs. p_T for anti-protons for 20 - 60% centrality
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t8
title: "Figure 7a" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: v2(2) vs. centrality for pions
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t10
title: "Figure 7c" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: v2(2) vs. centrality for anti-protons
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t11
title: "Figure 8" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: v2 vs. p_T for particles identified in the RICH (min. bias) for pions+kaons and protons/antiprotons
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t12
title: "Figure 9_1" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: v2 for Kshort for min. bias
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t13
title: "Figure 9_2" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: v2 for kaons from kinks for min. bias
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t14
title: "Figure 9_3" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: v2 for kaons from dE/dx for min. bias
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t15
title: "Figure 10" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: v2 for Lambda+Lambdabar for min. bias [PRL/92/052302/2004]. The PHENIX data are from [PRL/91/182301/2003]. The hydro calculations are from [P. Huovinen/private communication].
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t16
title: "Figure 11_1" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: v2 for charged pions for min. bias. kaon data points are from Figure 9.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t9
title: "Figure 7b" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: v2(2) vs. centrality for kaons
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t17
title: "Figure 11_2" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: v2 for anti-protons for min. bias. kaon data points are from Figure 9.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t18
title: "Figure 12_1" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Azimuthal correlations (\sum_i cos(2(\phi_pT -\phi_i))) in Au+Au collisions as a function of p_T along with results from p+p collisions.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t19
title: "Figure 12_2" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Azimuthal correlations (\sum_i cos(2(\phi_pT -\phi_i))) from d+Au as a function of p_T for min bias collisions.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t20
title: "Figure 13" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Azimuthal correlations (\sum_i cos(2(\phi_pT -\phi_i))) from d+Au as a function of p_T for three centralities.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t21
title: "Figure 15 and Figure 27 - 1" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Charged hadron v2 and v4{EP_2} as a function of pseudorapidity for minimum bias.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t22
title: "Figure 16_1" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: v2(2) and v2(4) vs. pseudorapidity
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t23
title: "Figure 16_2" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: v2(2) and v2(4) vs. pseudorapidity,FTPC only
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t24
title: "Figure 17_1" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: v2(4) 20-70% in TPC+FTPC and v2(2) 20-70% in FTPC.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t25
title: "Figure 17_2" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: MC v2 with FTPC momentum resolution.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t26
title: "Figure 18_1" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Charged hadron v2 for the centrality bin 0-5% in standard and modified event plane methods.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t27
title: "Figure 18_2" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Charged hadron v2 for the centrality bin 5-10% in standard and modified event plane methods.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t28
title: "Figure 18_3" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Charged hadron v2 for the centrality bin 10-20% in standard and modified event plane methods.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t29
title: "Figure 18_4" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Charged hadron v2 for the centrality bin 20-30% in standard and modified event plane methods.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t30
title: "Figure 18_5" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Charged hadron v2 for the centrality bin 30-40% in standard and modified event plane methods.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t31
title: "Figure 18_6" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Charged hadron v2 for the centrality bin 40-60% in standard and modified event plane methods.
description: No data abstract available.
DOI: 10.17182/hepdata.93262.v1/t32
title: "Figure 20" of "Azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Charged hadron v2{2} from modified reaction plane method and two-particle cumulant results (after subtracting the correlations measured in p+p collisions) for centrality bin 20-60% .
description: No data abstract available.