cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.73094.v1/t8
title: "Table 8" of "Differential studies of inclusive J/$\psi$ and $\psi$(2S) production at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{{\textit s}_{_{NN}}}}$ = 2.76 TeV"

description: Inclusive J/$\psi$ $R_{\rm AA}$ and Pb-Pb yields as a function of $p_{\rm T}$ for the 20-40% centrality class and $2.5
description: CERN-LHC. The production of J/$\psi$ and $\psi$(2S) was studied with the ALICE detector in Pb-Pb collisions at the LHC. The measurement was performed at forward rapidity ($2.5
DOI: 10.17182/hepdata.73094.v1/t9
title: "Table 9" of "Differential studies of inclusive J/$\psi$ and $\psi$(2S) production at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{{\textit s}_{_{NN}}}}$ = 2.76 TeV"

description: Inclusive J/$\psi$ $R_{\rm AA}$ and Pb-Pb yields as a function of $p_{\rm T}$ for the 0-40% centrality class and $2.5
description: CERN-LHC. The production of J/$\psi$ and $\psi$(2S) was studied with the ALICE detector in Pb-Pb collisions at the LHC. The measurement was performed at forward rapidity ($2.5
DOI: 10.5064/f6g2petf/gfpd2l
title: Moore-et-al_ME_1220_20201212-Public-Safety-Vaccination-Plan.pdf
DOI: 10.17182/hepdata.68483.v1/t1
title: "Table 1" of "Measurement of jet suppression in central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: The $\delta{p}_{\mathrm{T}}$ distribution for $R=0.2$ with the random-cone and the embedded-track methods in the 10% most central events, with $p_{\mathrm{T}}^{\mathrm{probe}}=60$ GeV/$c$ for the embedded-track method.
description: CERN-LHC. The transverse momentum ($p_{\mathrm{T}}$) spectrum and nuclear modification factor (${R}_{\mathrm{AA}}$) of reconstructed jets in $0$-$10$% and $10$-$30$% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$ TeV were measured. Jets were reconstructed from charged and neutral particles, utilizing the ALICE tracking detectors and Electromagnetic Calorimeter (EMCal), with the anti-$k_{\mathrm{T}}$ jet algorithm with a resolution parameter of $R=0.2$. The jet $p_{\mathrm{T}}$ spectra are reported in the pseudorapidity interval of $|{\eta}_{\rm jet}|&lt;0.5$ for $40&lt;{p}_{\mathrm{T,~jet}}&lt;120$ GeV/$c$ in $0$-$10$% and for $30&lt;{p}_{\mathrm{T,~jet}}&lt;100$ GeV/$c$ in $10$-$30$% collisions. Reconstructed jets were required to contain a leading charged particle with $p_{\mathrm{T}}&gt;5$ GeV/$c$ to suppress jets constructed from the combinatorial background in Pb--Pb collisions. The nuclear modification factor is obtained by dividing the jet spectrum measured in Pb--Pb by that in pp collisions scaled by the number of independent nucleon--nucleon collisions estimated using a Glauber model. ${R}_{\mathrm{AA}}$ is found to be $0.28\pm0.04$ in $0$-$10$% and $0.35\pm0.04$ in $10$-$30$% collisions, independent of ${p}_{\mathrm{T,~jet}}$ within the uncertainties of the measurement.
DOI: 10.17182/hepdata.73094.v1/t12
title: "Table 12" of "Differential studies of inclusive J/$\psi$ and $\psi$(2S) production at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{{\textit s}_{_{NN}}}}$ = 2.76 TeV"

description: Inclusive J/$\psi$ $R_{\rm AA}$ and Pb-Pb yields as a function of $y$ for the 0-90% centrality class and $p_{\rm T}&lt;8$ GeV/$c$. Statistical and systematic uncertainties are also reported. A global systematic uncertainty of 8% (4%) affects all the $R_{\rm AA}$ (yields) values.
description: CERN-LHC. The production of J/$\psi$ and $\psi$(2S) was studied with the ALICE detector in Pb-Pb collisions at the LHC. The measurement was performed at forward rapidity ($2.5
DOI: 10.17182/hepdata.73094.v1/t13
title: "Table 13" of "Differential studies of inclusive J/$\psi$ and $\psi$(2S) production at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{{\textit s}_{_{NN}}}}$ = 2.76 TeV"

description: Inclusive J/$\psi$ $R_{\rm AA}$ as a function of centrality, $0.3
description: CERN-LHC. The production of J/$\psi$ and $\psi$(2S) was studied with the ALICE detector in Pb-Pb collisions at the LHC. The measurement was performed at forward rapidity ($2.5
DOI: 10.17182/hepdata.73094.v1/t14
title: "Table 14" of "Differential studies of inclusive J/$\psi$ and $\psi$(2S) production at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{{\textit s}_{_{NN}}}}$ = 2.76 TeV"

description: Inclusive J/$\psi$ $R_{\rm AA}$ for $2.5
description: CERN-LHC. The production of J/$\psi$ and $\psi$(2S) was studied with the ALICE detector in Pb-Pb collisions at the LHC. The measurement was performed at forward rapidity ($2.5
DOI: 10.17182/hepdata.73094.v1/t15
title: "Table 15" of "Differential studies of inclusive J/$\psi$ and $\psi$(2S) production at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{{\textit s}_{_{NN}}}}$ = 2.76 TeV"

description: Inclusive $[\psi\text{(2S)/J/}\psi]_{\rm Pb-Pb}$ and $[\psi\text{(2S)/J/}\psi]_{\rm Pb-Pb}\;/\;[\psi\text{(2S)/J/}\psi]_{\rm pp}$ ratios as a function of centrality for $p_{\rm T}&lt;3$ GeV/$c$. Statistical and systematic uncertainties are reported when the value is not given as an upper limit.
description: CERN-LHC. The production of J/$\psi$ and $\psi$(2S) was studied with the ALICE detector in Pb-Pb collisions at the LHC. The measurement was performed at forward rapidity ($2.5
DOI: 10.17182/hepdata.73094.v1/t16
title: "Table 16" of "Differential studies of inclusive J/$\psi$ and $\psi$(2S) production at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{{\textit s}_{_{NN}}}}$ = 2.76 TeV"

description: Inclusive $[\psi\text{(2S)/J/}\psi]_{\rm Pb-Pb}$ and $[\psi\text{(2S)/J/}\psi]_{\rm Pb-Pb}\;/\;[\psi\text{(2S)/J/}\psi]_{\rm pp}$ ratios as a function of centrality for $3
description: CERN-LHC. The production of J/$\psi$ and $\psi$(2S) was studied with the ALICE detector in Pb-Pb collisions at the LHC. The measurement was performed at forward rapidity ($2.5
DOI: 10.17182/hepdata.68483.v1/t2
title: "Table 2" of "Measurement of jet suppression in central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: The spectra of $R=0.2$ jets with a leading track requirement of $5$ GeV/$c$ in inelastic pp collisions at $\sqrt{s}=2.76$ TeV.
description: CERN-LHC. The transverse momentum ($p_{\mathrm{T}}$) spectrum and nuclear modification factor (${R}_{\mathrm{AA}}$) of reconstructed jets in $0$-$10$% and $10$-$30$% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$ TeV were measured. Jets were reconstructed from charged and neutral particles, utilizing the ALICE tracking detectors and Electromagnetic Calorimeter (EMCal), with the anti-$k_{\mathrm{T}}$ jet algorithm with a resolution parameter of $R=0.2$. The jet $p_{\mathrm{T}}$ spectra are reported in the pseudorapidity interval of $|{\eta}_{\rm jet}|&lt;0.5$ for $40&lt;{p}_{\mathrm{T,~jet}}&lt;120$ GeV/$c$ in $0$-$10$% and for $30&lt;{p}_{\mathrm{T,~jet}}&lt;100$ GeV/$c$ in $10$-$30$% collisions. Reconstructed jets were required to contain a leading charged particle with $p_{\mathrm{T}}&gt;5$ GeV/$c$ to suppress jets constructed from the combinatorial background in Pb--Pb collisions. The nuclear modification factor is obtained by dividing the jet spectrum measured in Pb--Pb by that in pp collisions scaled by the number of independent nucleon--nucleon collisions estimated using a Glauber model. ${R}_{\mathrm{AA}}$ is found to be $0.28\pm0.04$ in $0$-$10$% and $0.35\pm0.04$ in $10$-$30$% collisions, independent of ${p}_{\mathrm{T,~jet}}$ within the uncertainties of the measurement.
DOI: 10.17182/hepdata.68483.v1/t3
title: "Table 3" of "Measurement of jet suppression in central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: The spectra of $R=0.2$ jets with a leading track requirement of $5$ GeV/$c$ in 0-10% and 10-30% most central Pb-Pb collisions scaled by 1/$N_{\mathrm{coll}}$ at $\sqrt{s_{\mathrm{NN}}}=2.76$ TeV.
description: CERN-LHC. The transverse momentum ($p_{\mathrm{T}}$) spectrum and nuclear modification factor (${R}_{\mathrm{AA}}$) of reconstructed jets in $0$-$10$% and $10$-$30$% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$ TeV were measured. Jets were reconstructed from charged and neutral particles, utilizing the ALICE tracking detectors and Electromagnetic Calorimeter (EMCal), with the anti-$k_{\mathrm{T}}$ jet algorithm with a resolution parameter of $R=0.2$. The jet $p_{\mathrm{T}}$ spectra are reported in the pseudorapidity interval of $|{\eta}_{\rm jet}|&lt;0.5$ for $40&lt;{p}_{\mathrm{T,~jet}}&lt;120$ GeV/$c$ in $0$-$10$% and for $30&lt;{p}_{\mathrm{T,~jet}}&lt;100$ GeV/$c$ in $10$-$30$% collisions. Reconstructed jets were required to contain a leading charged particle with $p_{\mathrm{T}}&gt;5$ GeV/$c$ to suppress jets constructed from the combinatorial background in Pb--Pb collisions. The nuclear modification factor is obtained by dividing the jet spectrum measured in Pb--Pb by that in pp collisions scaled by the number of independent nucleon--nucleon collisions estimated using a Glauber model. ${R}_{\mathrm{AA}}$ is found to be $0.28\pm0.04$ in $0$-$10$% and $0.35\pm0.04$ in $10$-$30$% collisions, independent of ${p}_{\mathrm{T,~jet}}$ within the uncertainties of the measurement.
DOI: 10.17182/hepdata.68483.v1/t4
title: "Table 4" of "Measurement of jet suppression in central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: Ratio of the jet spectrum with a leading track $p_{\mathrm{T}}$ &gt; 5 GeV/$c$ over the inclusive jet spectrum for $R=0.2$ in pp collisions at $\sqrt{s}=2.76$ TeV.
description: CERN-LHC. The transverse momentum ($p_{\mathrm{T}}$) spectrum and nuclear modification factor (${R}_{\mathrm{AA}}$) of reconstructed jets in $0$-$10$% and $10$-$30$% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$ TeV were measured. Jets were reconstructed from charged and neutral particles, utilizing the ALICE tracking detectors and Electromagnetic Calorimeter (EMCal), with the anti-$k_{\mathrm{T}}$ jet algorithm with a resolution parameter of $R=0.2$. The jet $p_{\mathrm{T}}$ spectra are reported in the pseudorapidity interval of $|{\eta}_{\rm jet}|&lt;0.5$ for $40&lt;{p}_{\mathrm{T,~jet}}&lt;120$ GeV/$c$ in $0$-$10$% and for $30&lt;{p}_{\mathrm{T,~jet}}&lt;100$ GeV/$c$ in $10$-$30$% collisions. Reconstructed jets were required to contain a leading charged particle with $p_{\mathrm{T}}&gt;5$ GeV/$c$ to suppress jets constructed from the combinatorial background in Pb--Pb collisions. The nuclear modification factor is obtained by dividing the jet spectrum measured in Pb--Pb by that in pp collisions scaled by the number of independent nucleon--nucleon collisions estimated using a Glauber model. ${R}_{\mathrm{AA}}$ is found to be $0.28\pm0.04$ in $0$-$10$% and $0.35\pm0.04$ in $10$-$30$% collisions, independent of ${p}_{\mathrm{T,~jet}}$ within the uncertainties of the measurement.
DOI: 10.17182/hepdata.68483.v1/t5
title: "Table 5" of "Measurement of jet suppression in central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: Ratios of jet spectra with different leading track $p_{\mathrm{T}}$ requirements ("$0$ over $5$", "$3$ over $5$", "$7$ over $5$" and "$10$ over $5$") for $R=0.2$ jets in 0-10% most central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$ TeV.
description: CERN-LHC. The transverse momentum ($p_{\mathrm{T}}$) spectrum and nuclear modification factor (${R}_{\mathrm{AA}}$) of reconstructed jets in $0$-$10$% and $10$-$30$% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$ TeV were measured. Jets were reconstructed from charged and neutral particles, utilizing the ALICE tracking detectors and Electromagnetic Calorimeter (EMCal), with the anti-$k_{\mathrm{T}}$ jet algorithm with a resolution parameter of $R=0.2$. The jet $p_{\mathrm{T}}$ spectra are reported in the pseudorapidity interval of $|{\eta}_{\rm jet}|&lt;0.5$ for $40&lt;{p}_{\mathrm{T,~jet}}&lt;120$ GeV/$c$ in $0$-$10$% and for $30&lt;{p}_{\mathrm{T,~jet}}&lt;100$ GeV/$c$ in $10$-$30$% collisions. Reconstructed jets were required to contain a leading charged particle with $p_{\mathrm{T}}&gt;5$ GeV/$c$ to suppress jets constructed from the combinatorial background in Pb--Pb collisions. The nuclear modification factor is obtained by dividing the jet spectrum measured in Pb--Pb by that in pp collisions scaled by the number of independent nucleon--nucleon collisions estimated using a Glauber model. ${R}_{\mathrm{AA}}$ is found to be $0.28\pm0.04$ in $0$-$10$% and $0.35\pm0.04$ in $10$-$30$% collisions, independent of ${p}_{\mathrm{T,~jet}}$ within the uncertainties of the measurement.
DOI: 10.17182/hepdata.68483.v1/t6
title: "Table 6" of "Measurement of jet suppression in central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: $R_{\mathrm{AA}}$ for $R=0.2$ jets with the leading track requirement of $5$ GeV/$c$ in 0-10% most central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$ TeV.
description: CERN-LHC. The transverse momentum ($p_{\mathrm{T}}$) spectrum and nuclear modification factor (${R}_{\mathrm{AA}}$) of reconstructed jets in $0$-$10$% and $10$-$30$% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$ TeV were measured. Jets were reconstructed from charged and neutral particles, utilizing the ALICE tracking detectors and Electromagnetic Calorimeter (EMCal), with the anti-$k_{\mathrm{T}}$ jet algorithm with a resolution parameter of $R=0.2$. The jet $p_{\mathrm{T}}$ spectra are reported in the pseudorapidity interval of $|{\eta}_{\rm jet}|&lt;0.5$ for $40&lt;{p}_{\mathrm{T,~jet}}&lt;120$ GeV/$c$ in $0$-$10$% and for $30&lt;{p}_{\mathrm{T,~jet}}&lt;100$ GeV/$c$ in $10$-$30$% collisions. Reconstructed jets were required to contain a leading charged particle with $p_{\mathrm{T}}&gt;5$ GeV/$c$ to suppress jets constructed from the combinatorial background in Pb--Pb collisions. The nuclear modification factor is obtained by dividing the jet spectrum measured in Pb--Pb by that in pp collisions scaled by the number of independent nucleon--nucleon collisions estimated using a Glauber model. ${R}_{\mathrm{AA}}$ is found to be $0.28\pm0.04$ in $0$-$10$% and $0.35\pm0.04$ in $10$-$30$% collisions, independent of ${p}_{\mathrm{T,~jet}}$ within the uncertainties of the measurement.
DOI: 10.17182/hepdata.68483.v1/t7
title: "Table 7" of "Measurement of jet suppression in central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: $R_{\mathrm{AA}}$ for $R=0.2$ jets with the leading track requirement of $5$ GeV/$c$ in 10-30% most central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$ TeV.
description: CERN-LHC. The transverse momentum ($p_{\mathrm{T}}$) spectrum and nuclear modification factor (${R}_{\mathrm{AA}}$) of reconstructed jets in $0$-$10$% and $10$-$30$% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$ TeV were measured. Jets were reconstructed from charged and neutral particles, utilizing the ALICE tracking detectors and Electromagnetic Calorimeter (EMCal), with the anti-$k_{\mathrm{T}}$ jet algorithm with a resolution parameter of $R=0.2$. The jet $p_{\mathrm{T}}$ spectra are reported in the pseudorapidity interval of $|{\eta}_{\rm jet}|&lt;0.5$ for $40&lt;{p}_{\mathrm{T,~jet}}&lt;120$ GeV/$c$ in $0$-$10$% and for $30&lt;{p}_{\mathrm{T,~jet}}&lt;100$ GeV/$c$ in $10$-$30$% collisions. Reconstructed jets were required to contain a leading charged particle with $p_{\mathrm{T}}&gt;5$ GeV/$c$ to suppress jets constructed from the combinatorial background in Pb--Pb collisions. The nuclear modification factor is obtained by dividing the jet spectrum measured in Pb--Pb by that in pp collisions scaled by the number of independent nucleon--nucleon collisions estimated using a Glauber model. ${R}_{\mathrm{AA}}$ is found to be $0.28\pm0.04$ in $0$-$10$% and $0.35\pm0.04$ in $10$-$30$% collisions, independent of ${p}_{\mathrm{T,~jet}}$ within the uncertainties of the measurement.
DOI: 10.17182/hepdata.78924.v2/t1
title: "Table 1" of "Systematic studies of correlations between different order flow harmonics in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: Centrality dependence of observables SC(5,2) in Pb-Pb collisions at 2.76 TeV.
description: CERN-LHC. Measurements of correlations between event-by-event fluctuations of amplitudes of anisotropic flow harmonics in nucleus-nucleus collisions at $\sqrt{s_{_{\rm NN}}}=2.76$ TeV. Data was recorded in November 2010 with the ALICE detector at the CERN Large Hadron Collider. The measurements are performed in the central pseudorapidity region (|$\eta$| &lt; 0.8) and transverse momentum range 0.2 &lt; $p_T$ &lt; 5.0 GeV/c. The data for SC(3,2), SC(4,2), NSC(3,2) and NSC(4,2) in Figure 1 can be found at http://dx.doi.org/10.17182/hepdata.74142. The lower order $v_n$ for n&lt;4 in Figure 3 can be found at http://dx.doi.org/10.17182/hepdata.72886.v2 (Table 3 and 4).
DOI: 10.17182/hepdata.78924.v2/t3
title: "Table 3" of "Systematic studies of correlations between different order flow harmonics in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: Centrality dependence of observables SC(4,3) in Pb-Pb collisions at 2.76 TeV.
description: CERN-LHC. Measurements of correlations between event-by-event fluctuations of amplitudes of anisotropic flow harmonics in nucleus-nucleus collisions at $\sqrt{s_{_{\rm NN}}}=2.76$ TeV. Data was recorded in November 2010 with the ALICE detector at the CERN Large Hadron Collider. The measurements are performed in the central pseudorapidity region (|$\eta$| &lt; 0.8) and transverse momentum range 0.2 &lt; $p_T$ &lt; 5.0 GeV/c. The data for SC(3,2), SC(4,2), NSC(3,2) and NSC(4,2) in Figure 1 can be found at http://dx.doi.org/10.17182/hepdata.74142. The lower order $v_n$ for n&lt;4 in Figure 3 can be found at http://dx.doi.org/10.17182/hepdata.72886.v2 (Table 3 and 4).
DOI: 10.17182/hepdata.78924.v2/t5
title: "Table 5" of "Systematic studies of correlations between different order flow harmonics in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: Centrality dependence of observables NSC(5,3) in Pb-Pb collisions at 2.76 TeV.
description: CERN-LHC. Measurements of correlations between event-by-event fluctuations of amplitudes of anisotropic flow harmonics in nucleus-nucleus collisions at $\sqrt{s_{_{\rm NN}}}=2.76$ TeV. Data was recorded in November 2010 with the ALICE detector at the CERN Large Hadron Collider. The measurements are performed in the central pseudorapidity region (|$\eta$| &lt; 0.8) and transverse momentum range 0.2 &lt; $p_T$ &lt; 5.0 GeV/c. The data for SC(3,2), SC(4,2), NSC(3,2) and NSC(4,2) in Figure 1 can be found at http://dx.doi.org/10.17182/hepdata.74142. The lower order $v_n$ for n&lt;4 in Figure 3 can be found at http://dx.doi.org/10.17182/hepdata.72886.v2 (Table 3 and 4).
DOI: 10.5064/f6g2petf/8xkqs5
title: Moore-et-al_MD_0921_Pages - PHOTO RELEASE-Maryland Department of Health provides free COVID-19 vaccinations at the Maryland Renaissa.pdf
DOI: 10.17182/hepdata.78924.v2/t11
title: "Table 11" of "Systematic studies of correlations between different order flow harmonics in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.
description: CERN-LHC. Measurements of correlations between event-by-event fluctuations of amplitudes of anisotropic flow harmonics in nucleus-nucleus collisions at $\sqrt{s_{_{\rm NN}}}=2.76$ TeV. Data was recorded in November 2010 with the ALICE detector at the CERN Large Hadron Collider. The measurements are performed in the central pseudorapidity region (|$\eta$| &lt; 0.8) and transverse momentum range 0.2 &lt; $p_T$ &lt; 5.0 GeV/c. The data for SC(3,2), SC(4,2), NSC(3,2) and NSC(4,2) in Figure 1 can be found at http://dx.doi.org/10.17182/hepdata.74142. The lower order $v_n$ for n&lt;4 in Figure 3 can be found at http://dx.doi.org/10.17182/hepdata.72886.v2 (Table 3 and 4).
DOI: 10.17182/hepdata.78924.v2/t2
title: "Table 2" of "Systematic studies of correlations between different order flow harmonics in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: Centrality dependence of observables SC(5,3) in Pb-Pb collisions at 2.76 TeV.
description: CERN-LHC. Measurements of correlations between event-by-event fluctuations of amplitudes of anisotropic flow harmonics in nucleus-nucleus collisions at $\sqrt{s_{_{\rm NN}}}=2.76$ TeV. Data was recorded in November 2010 with the ALICE detector at the CERN Large Hadron Collider. The measurements are performed in the central pseudorapidity region (|$\eta$| &lt; 0.8) and transverse momentum range 0.2 &lt; $p_T$ &lt; 5.0 GeV/c. The data for SC(3,2), SC(4,2), NSC(3,2) and NSC(4,2) in Figure 1 can be found at http://dx.doi.org/10.17182/hepdata.74142. The lower order $v_n$ for n&lt;4 in Figure 3 can be found at http://dx.doi.org/10.17182/hepdata.72886.v2 (Table 3 and 4).
DOI: 10.17182/hepdata.78924.v2/t4
title: "Table 4" of "Systematic studies of correlations between different order flow harmonics in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: Centrality dependence of observables NSC(5,2) in Pb-Pb collisions at 2.76 TeV.
description: CERN-LHC. Measurements of correlations between event-by-event fluctuations of amplitudes of anisotropic flow harmonics in nucleus-nucleus collisions at $\sqrt{s_{_{\rm NN}}}=2.76$ TeV. Data was recorded in November 2010 with the ALICE detector at the CERN Large Hadron Collider. The measurements are performed in the central pseudorapidity region (|$\eta$| &lt; 0.8) and transverse momentum range 0.2 &lt; $p_T$ &lt; 5.0 GeV/c. The data for SC(3,2), SC(4,2), NSC(3,2) and NSC(4,2) in Figure 1 can be found at http://dx.doi.org/10.17182/hepdata.74142. The lower order $v_n$ for n&lt;4 in Figure 3 can be found at http://dx.doi.org/10.17182/hepdata.72886.v2 (Table 3 and 4).
DOI: 10.17182/hepdata.78924.v2/t6
title: "Table 6" of "Systematic studies of correlations between different order flow harmonics in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: Centrality dependence of observables NSC(4,3) in Pb-Pb collisions at 2.76 TeV.
description: CERN-LHC. Measurements of correlations between event-by-event fluctuations of amplitudes of anisotropic flow harmonics in nucleus-nucleus collisions at $\sqrt{s_{_{\rm NN}}}=2.76$ TeV. Data was recorded in November 2010 with the ALICE detector at the CERN Large Hadron Collider. The measurements are performed in the central pseudorapidity region (|$\eta$| &lt; 0.8) and transverse momentum range 0.2 &lt; $p_T$ &lt; 5.0 GeV/c. The data for SC(3,2), SC(4,2), NSC(3,2) and NSC(4,2) in Figure 1 can be found at http://dx.doi.org/10.17182/hepdata.74142. The lower order $v_n$ for n&lt;4 in Figure 3 can be found at http://dx.doi.org/10.17182/hepdata.72886.v2 (Table 3 and 4).
DOI: 10.17182/hepdata.78924.v2/t7
title: "Table 7" of "Systematic studies of correlations between different order flow harmonics in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.
description: CERN-LHC. Measurements of correlations between event-by-event fluctuations of amplitudes of anisotropic flow harmonics in nucleus-nucleus collisions at $\sqrt{s_{_{\rm NN}}}=2.76$ TeV. Data was recorded in November 2010 with the ALICE detector at the CERN Large Hadron Collider. The measurements are performed in the central pseudorapidity region (|$\eta$| &lt; 0.8) and transverse momentum range 0.2 &lt; $p_T$ &lt; 5.0 GeV/c. The data for SC(3,2), SC(4,2), NSC(3,2) and NSC(4,2) in Figure 1 can be found at http://dx.doi.org/10.17182/hepdata.74142. The lower order $v_n$ for n&lt;4 in Figure 3 can be found at http://dx.doi.org/10.17182/hepdata.72886.v2 (Table 3 and 4).