cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.66180.v1/t18
title: "Table 18" of "Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at sqrt(s_NN)=2.76 TeV with the ATLAS detector"

description: Elliptic flow $v_{2}$ integrated over transverse momentum $p_{T}&gt;p_{T,0}$ as a function of $p_{T,0}$ for 20-30% centrality interval, obtained with different charged-particle reconstruction methods: the tracklet (TKT) method with $p_{T,0}=0.07$ GeV, the pixel track (PXT) method with $p_{T,0} \geq 0.1$ GeV and the ID track (IDT) method with $p_{T,0}=0.5$ GeV. Error bars indicate statistical and systematic uncertainties added in quadrature.
description: CERN-LHC. The integrated elliptic flow of charged particles produced in Pb+Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV has been measured with the ATLAS detector using data collected at the Large Hadron Collider. The anisotropy parameter, $v_{2}$, was measured in the pseudorapidity range $|\eta| \leq 2.5$ with the event-plane method. In order to include tracks with very low transverse momentum $p_{T}$, thus reducing the uncertainty in $v_{2}$ integrated over $p_{T}$, a 1$\mu b^{-1}$ data sample recorded without a magnetic field in the tracking detectors is used. The centrality dependence of the integrated $v_{2}$ is compared to other measurements obtained with higher $p_{T}$ thresholds. The integrated $v_{2}$ transformed to the rest frame of one of the colliding nuclei is compared to the lower-energy RHIC data.
For more details see the paper.
DOI: 10.17182/hepdata.66180.v1/t19
title: "Table 19" of "Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at sqrt(s_NN)=2.76 TeV with the ATLAS detector"

description: Elliptic flow $v_{2}$ integrated over transverse momentum $p_{T}&gt;p_{T,0}$ as a function of $p_{T,0}$ for 30-40% centrality interval, obtained with different charged-particle reconstruction methods: the tracklet (TKT) method with $p_{T,0}=0.07$ GeV, the pixel track (PXT) method with $p_{T,0} \geq 0.1$ GeV and the ID track (IDT) method with $p_{T,0}=0.5$ GeV. Error bars indicate statistical and systematic uncertainties added in quadrature.
description: CERN-LHC. The integrated elliptic flow of charged particles produced in Pb+Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV has been measured with the ATLAS detector using data collected at the Large Hadron Collider. The anisotropy parameter, $v_{2}$, was measured in the pseudorapidity range $|\eta| \leq 2.5$ with the event-plane method. In order to include tracks with very low transverse momentum $p_{T}$, thus reducing the uncertainty in $v_{2}$ integrated over $p_{T}$, a 1$\mu b^{-1}$ data sample recorded without a magnetic field in the tracking detectors is used. The centrality dependence of the integrated $v_{2}$ is compared to other measurements obtained with higher $p_{T}$ thresholds. The integrated $v_{2}$ transformed to the rest frame of one of the colliding nuclei is compared to the lower-energy RHIC data.
For more details see the paper.
DOI: 10.17182/hepdata.66180.v1/t20
title: "Table 20" of "Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at sqrt(s_NN)=2.76 TeV with the ATLAS detector"

description: Elliptic flow $v_{2}$ integrated over transverse momentum $p_{T}&gt;p_{T,0}$ as a function of $p_{T,0}$ for 40-50% centrality interval, obtained with different charged-particle reconstruction methods: the tracklet (TKT) method with $p_{T,0}=0.07$ GeV, the pixel track (PXT) method with $p_{T,0} \geq 0.1$ GeV and the ID track (IDT) method with $p_{T,0}=0.5$ GeV. Error bars indicate statistical and systematic uncertainties added in quadrature.
description: CERN-LHC. The integrated elliptic flow of charged particles produced in Pb+Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV has been measured with the ATLAS detector using data collected at the Large Hadron Collider. The anisotropy parameter, $v_{2}$, was measured in the pseudorapidity range $|\eta| \leq 2.5$ with the event-plane method. In order to include tracks with very low transverse momentum $p_{T}$, thus reducing the uncertainty in $v_{2}$ integrated over $p_{T}$, a 1$\mu b^{-1}$ data sample recorded without a magnetic field in the tracking detectors is used. The centrality dependence of the integrated $v_{2}$ is compared to other measurements obtained with higher $p_{T}$ thresholds. The integrated $v_{2}$ transformed to the rest frame of one of the colliding nuclei is compared to the lower-energy RHIC data.
For more details see the paper.
DOI: 10.17182/hepdata.66180.v1/t21
title: "Table 21" of "Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at sqrt(s_NN)=2.76 TeV with the ATLAS detector"

description: Elliptic flow $v_{2}$ integrated over transverse momentum $p_{T}&gt;p_{T,0}$ as a function of $p_{T,0}$ for 50-60% centrality interval, obtained with different charged-particle reconstruction methods: the tracklet (TKT) method with $p_{T,0}=0.07$ GeV, the pixel track (PXT) method with $p_{T,0} \geq 0.1$ GeV and the ID track (IDT) method with $p_{T,0}=0.5$ GeV. Error bars indicate statistical and systematic uncertainties added in quadrature.
description: CERN-LHC. The integrated elliptic flow of charged particles produced in Pb+Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV has been measured with the ATLAS detector using data collected at the Large Hadron Collider. The anisotropy parameter, $v_{2}$, was measured in the pseudorapidity range $|\eta| \leq 2.5$ with the event-plane method. In order to include tracks with very low transverse momentum $p_{T}$, thus reducing the uncertainty in $v_{2}$ integrated over $p_{T}$, a 1$\mu b^{-1}$ data sample recorded without a magnetic field in the tracking detectors is used. The centrality dependence of the integrated $v_{2}$ is compared to other measurements obtained with higher $p_{T}$ thresholds. The integrated $v_{2}$ transformed to the rest frame of one of the colliding nuclei is compared to the lower-energy RHIC data.
For more details see the paper.
DOI: 10.17182/hepdata.66180.v1/t22
title: "Table 22" of "Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at sqrt(s_NN)=2.76 TeV with the ATLAS detector"

description: Elliptic flow $v_{2}$ integrated over transverse momentum $p_{T}&gt;p_{T,0}$ as a function of $p_{T,0}$ for 60-70% centrality interval, obtained with different charged-particle reconstruction methods: the tracklet (TKT) method with $p_{T,0}=0.07$ GeV, the pixel track (PXT) method with $p_{T,0} \geq 0.1$ GeV and the ID track (IDT) method with $p_{T,0}=0.5$ GeV. Error bars indicate statistical and systematic uncertainties added in quadrature.
description: CERN-LHC. The integrated elliptic flow of charged particles produced in Pb+Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV has been measured with the ATLAS detector using data collected at the Large Hadron Collider. The anisotropy parameter, $v_{2}$, was measured in the pseudorapidity range $|\eta| \leq 2.5$ with the event-plane method. In order to include tracks with very low transverse momentum $p_{T}$, thus reducing the uncertainty in $v_{2}$ integrated over $p_{T}$, a 1$\mu b^{-1}$ data sample recorded without a magnetic field in the tracking detectors is used. The centrality dependence of the integrated $v_{2}$ is compared to other measurements obtained with higher $p_{T}$ thresholds. The integrated $v_{2}$ transformed to the rest frame of one of the colliding nuclei is compared to the lower-energy RHIC data.
For more details see the paper.
DOI: 10.17182/hepdata.66180.v1/t23
title: "Table 23" of "Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at sqrt(s_NN)=2.76 TeV with the ATLAS detector"

description: Elliptic flow $v_{2}$ integrated over transverse momentum $p_{T}&gt;p_{T,0}$ as a function of $p_{T,0}$ for 70-80% centrality interval, obtained with different charged-particle reconstruction methods: the tracklet (TKT) method with $p_{T,0}=0.07$ GeV, the pixel track (PXT) method with $p_{T,0} \geq 0.1$ GeV and the ID track (IDT) method with $p_{T,0}=0.5$ GeV. Error bars indicate statistical and systematic uncertainties added in quadrature.
description: CERN-LHC. The integrated elliptic flow of charged particles produced in Pb+Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV has been measured with the ATLAS detector using data collected at the Large Hadron Collider. The anisotropy parameter, $v_{2}$, was measured in the pseudorapidity range $|\eta| \leq 2.5$ with the event-plane method. In order to include tracks with very low transverse momentum $p_{T}$, thus reducing the uncertainty in $v_{2}$ integrated over $p_{T}$, a 1$\mu b^{-1}$ data sample recorded without a magnetic field in the tracking detectors is used. The centrality dependence of the integrated $v_{2}$ is compared to other measurements obtained with higher $p_{T}$ thresholds. The integrated $v_{2}$ transformed to the rest frame of one of the colliding nuclei is compared to the lower-energy RHIC data.
For more details see the paper.
DOI: 10.17182/hepdata.66180.v1/t24
title: "Table 24" of "Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at sqrt(s_NN)=2.76 TeV with the ATLAS detector"

description: Pseudorapidity dependence of elliptic flow, $v_{2}$, integrated over transverse momentum, $p_{T}$, for different charged particle reconstruction methods and different low-$p_{T}$ thresholds for the 0-10% centrality interval. Error bars indicate statistical and systematic uncertainties added in quadrature.
description: CERN-LHC. The integrated elliptic flow of charged particles produced in Pb+Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV has been measured with the ATLAS detector using data collected at the Large Hadron Collider. The anisotropy parameter, $v_{2}$, was measured in the pseudorapidity range $|\eta| \leq 2.5$ with the event-plane method. In order to include tracks with very low transverse momentum $p_{T}$, thus reducing the uncertainty in $v_{2}$ integrated over $p_{T}$, a 1$\mu b^{-1}$ data sample recorded without a magnetic field in the tracking detectors is used. The centrality dependence of the integrated $v_{2}$ is compared to other measurements obtained with higher $p_{T}$ thresholds. The integrated $v_{2}$ transformed to the rest frame of one of the colliding nuclei is compared to the lower-energy RHIC data.
For more details see the paper.
DOI: 10.17182/hepdata.66180.v1/t25
title: "Table 25" of "Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at sqrt(s_NN)=2.76 TeV with the ATLAS detector"

description: Pseudorapidity dependence of elliptic flow, $v_{2}$, integrated over transverse momentum, $p_{T}$, for different charged particle reconstruction methods and different low-$p_{T}$ thresholds for the 10-20% centrality interval. Error bars indicate statistical and systematic uncertainties added in quadrature.
description: CERN-LHC. The integrated elliptic flow of charged particles produced in Pb+Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV has been measured with the ATLAS detector using data collected at the Large Hadron Collider. The anisotropy parameter, $v_{2}$, was measured in the pseudorapidity range $|\eta| \leq 2.5$ with the event-plane method. In order to include tracks with very low transverse momentum $p_{T}$, thus reducing the uncertainty in $v_{2}$ integrated over $p_{T}$, a 1$\mu b^{-1}$ data sample recorded without a magnetic field in the tracking detectors is used. The centrality dependence of the integrated $v_{2}$ is compared to other measurements obtained with higher $p_{T}$ thresholds. The integrated $v_{2}$ transformed to the rest frame of one of the colliding nuclei is compared to the lower-energy RHIC data.
For more details see the paper.
DOI: 10.17182/hepdata.66180.v1/t26
title: "Table 26" of "Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at sqrt(s_NN)=2.76 TeV with the ATLAS detector"

description: Pseudorapidity dependence of elliptic flow, $v_{2}$, integrated over transverse momentum, $p_{T}$, for different charged particle reconstruction methods and different low-$p_{T}$ thresholds for the 20-30% centrality interval. Error bars indicate statistical and systematic uncertainties added in quadrature.
description: CERN-LHC. The integrated elliptic flow of charged particles produced in Pb+Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV has been measured with the ATLAS detector using data collected at the Large Hadron Collider. The anisotropy parameter, $v_{2}$, was measured in the pseudorapidity range $|\eta| \leq 2.5$ with the event-plane method. In order to include tracks with very low transverse momentum $p_{T}$, thus reducing the uncertainty in $v_{2}$ integrated over $p_{T}$, a 1$\mu b^{-1}$ data sample recorded without a magnetic field in the tracking detectors is used. The centrality dependence of the integrated $v_{2}$ is compared to other measurements obtained with higher $p_{T}$ thresholds. The integrated $v_{2}$ transformed to the rest frame of one of the colliding nuclei is compared to the lower-energy RHIC data.
For more details see the paper.
DOI: 10.17182/hepdata.66180.v1/t27
title: "Table 27" of "Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at sqrt(s_NN)=2.76 TeV with the ATLAS detector"

description: Pseudorapidity dependence of elliptic flow, $v_{2}$, integrated over transverse momentum, $p_{T}$, for different charged particle reconstruction methods and different low-$p_{T}$ thresholds for the 30-40% centrality interval. Error bars indicate statistical and systematic uncertainties added in quadrature.
description: CERN-LHC. The integrated elliptic flow of charged particles produced in Pb+Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV has been measured with the ATLAS detector using data collected at the Large Hadron Collider. The anisotropy parameter, $v_{2}$, was measured in the pseudorapidity range $|\eta| \leq 2.5$ with the event-plane method. In order to include tracks with very low transverse momentum $p_{T}$, thus reducing the uncertainty in $v_{2}$ integrated over $p_{T}$, a 1$\mu b^{-1}$ data sample recorded without a magnetic field in the tracking detectors is used. The centrality dependence of the integrated $v_{2}$ is compared to other measurements obtained with higher $p_{T}$ thresholds. The integrated $v_{2}$ transformed to the rest frame of one of the colliding nuclei is compared to the lower-energy RHIC data.
For more details see the paper.
DOI: 10.17182/hepdata.66180.v1/t28
title: "Table 28" of "Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at sqrt(s_NN)=2.76 TeV with the ATLAS detector"

description: Pseudorapidity dependence of elliptic flow, $v_{2}$, integrated over transverse momentum, $p_{T}$, for different charged particle reconstruction methods and different low-$p_{T}$ thresholds for the 40-50% centrality interval. Error bars indicate statistical and systematic uncertainties added in quadrature.
description: CERN-LHC. The integrated elliptic flow of charged particles produced in Pb+Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV has been measured with the ATLAS detector using data collected at the Large Hadron Collider. The anisotropy parameter, $v_{2}$, was measured in the pseudorapidity range $|\eta| \leq 2.5$ with the event-plane method. In order to include tracks with very low transverse momentum $p_{T}$, thus reducing the uncertainty in $v_{2}$ integrated over $p_{T}$, a 1$\mu b^{-1}$ data sample recorded without a magnetic field in the tracking detectors is used. The centrality dependence of the integrated $v_{2}$ is compared to other measurements obtained with higher $p_{T}$ thresholds. The integrated $v_{2}$ transformed to the rest frame of one of the colliding nuclei is compared to the lower-energy RHIC data.
For more details see the paper.
DOI: 10.17182/hepdata.66180.v1/t29
title: "Table 29" of "Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at sqrt(s_NN)=2.76 TeV with the ATLAS detector"

description: Pseudorapidity dependence of elliptic flow, $v_{2}$, integrated over transverse momentum, $p_{T}$, for different charged particle reconstruction methods and different low-$p_{T}$ thresholds for the 50-60% centrality interval. Error bars indicate statistical and systematic uncertainties added in quadrature.
description: CERN-LHC. The integrated elliptic flow of charged particles produced in Pb+Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV has been measured with the ATLAS detector using data collected at the Large Hadron Collider. The anisotropy parameter, $v_{2}$, was measured in the pseudorapidity range $|\eta| \leq 2.5$ with the event-plane method. In order to include tracks with very low transverse momentum $p_{T}$, thus reducing the uncertainty in $v_{2}$ integrated over $p_{T}$, a 1$\mu b^{-1}$ data sample recorded without a magnetic field in the tracking detectors is used. The centrality dependence of the integrated $v_{2}$ is compared to other measurements obtained with higher $p_{T}$ thresholds. The integrated $v_{2}$ transformed to the rest frame of one of the colliding nuclei is compared to the lower-energy RHIC data.
For more details see the paper.
DOI: 10.17182/hepdata.66180.v1/t30
title: "Table 30" of "Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at sqrt(s_NN)=2.76 TeV with the ATLAS detector"

description: Pseudorapidity dependence of elliptic flow, $v_{2}$, integrated over transverse momentum, $p_{T}$, for different charged particle reconstruction methods and different low-$p_{T}$ thresholds for the 60-70% centrality interval. Error bars indicate statistical and systematic uncertainties added in quadrature.
description: CERN-LHC. The integrated elliptic flow of charged particles produced in Pb+Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV has been measured with the ATLAS detector using data collected at the Large Hadron Collider. The anisotropy parameter, $v_{2}$, was measured in the pseudorapidity range $|\eta| \leq 2.5$ with the event-plane method. In order to include tracks with very low transverse momentum $p_{T}$, thus reducing the uncertainty in $v_{2}$ integrated over $p_{T}$, a 1$\mu b^{-1}$ data sample recorded without a magnetic field in the tracking detectors is used. The centrality dependence of the integrated $v_{2}$ is compared to other measurements obtained with higher $p_{T}$ thresholds. The integrated $v_{2}$ transformed to the rest frame of one of the colliding nuclei is compared to the lower-energy RHIC data.
For more details see the paper.
DOI: 10.17182/hepdata.66180.v1/t31
title: "Table 31" of "Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at sqrt(s_NN)=2.76 TeV with the ATLAS detector"

description: Pseudorapidity dependence of elliptic flow, $v_{2}$, integrated over transverse momentum, $p_{T}$, for different charged particle reconstruction methods and different low-$p_{T}$ thresholds for the 70-80% centrality interval. Error bars indicate statistical and systematic uncertainties added in quadrature.
description: CERN-LHC. The integrated elliptic flow of charged particles produced in Pb+Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV has been measured with the ATLAS detector using data collected at the Large Hadron Collider. The anisotropy parameter, $v_{2}$, was measured in the pseudorapidity range $|\eta| \leq 2.5$ with the event-plane method. In order to include tracks with very low transverse momentum $p_{T}$, thus reducing the uncertainty in $v_{2}$ integrated over $p_{T}$, a 1$\mu b^{-1}$ data sample recorded without a magnetic field in the tracking detectors is used. The centrality dependence of the integrated $v_{2}$ is compared to other measurements obtained with higher $p_{T}$ thresholds. The integrated $v_{2}$ transformed to the rest frame of one of the colliding nuclei is compared to the lower-energy RHIC data.
For more details see the paper.
DOI: 10.17182/hepdata.66180.v1/t32
title: "Table 32" of "Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at sqrt(s_NN)=2.76 TeV with the ATLAS detector"

description: Integrated elliptic flow, $v_{2}$, as a function of $|\eta| - y_{beam}$ for three centrality intervals Error bars indicate statistical and systematic uncertainties added in quadrature.
description: CERN-LHC. The integrated elliptic flow of charged particles produced in Pb+Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV has been measured with the ATLAS detector using data collected at the Large Hadron Collider. The anisotropy parameter, $v_{2}$, was measured in the pseudorapidity range $|\eta| \leq 2.5$ with the event-plane method. In order to include tracks with very low transverse momentum $p_{T}$, thus reducing the uncertainty in $v_{2}$ integrated over $p_{T}$, a 1$\mu b^{-1}$ data sample recorded without a magnetic field in the tracking detectors is used. The centrality dependence of the integrated $v_{2}$ is compared to other measurements obtained with higher $p_{T}$ thresholds. The integrated $v_{2}$ transformed to the rest frame of one of the colliding nuclei is compared to the lower-energy RHIC data.
For more details see the paper.
DOI: 10.17182/hepdata.66180.v1/t33
title: "Table 33" of "Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at sqrt(s_NN)=2.76 TeV with the ATLAS detector"

description: The transverse momentum, $p_{T}$, dependence of the TKT track reconstruction efficiency for $\pi^{\pm}$, $K^{\pm}$ and $p^{\pm}$ in the pseudorapidity range $|\eta| &lt; 1$ for 0-10% centrality interval.
description: CERN-LHC. The integrated elliptic flow of charged particles produced in Pb+Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV has been measured with the ATLAS detector using data collected at the Large Hadron Collider. The anisotropy parameter, $v_{2}$, was measured in the pseudorapidity range $|\eta| \leq 2.5$ with the event-plane method. In order to include tracks with very low transverse momentum $p_{T}$, thus reducing the uncertainty in $v_{2}$ integrated over $p_{T}$, a 1$\mu b^{-1}$ data sample recorded without a magnetic field in the tracking detectors is used. The centrality dependence of the integrated $v_{2}$ is compared to other measurements obtained with higher $p_{T}$ thresholds. The integrated $v_{2}$ transformed to the rest frame of one of the colliding nuclei is compared to the lower-energy RHIC data.
For more details see the paper.