cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.64272.v1/t73
title: "Table 73" of "Measurement of inclusive jet charged-particle fragmentation functions in Pb+Pb collisions at sqrt(s_NN) = 2.76 TeV with the ATLAS detector"

description: Ratio of D(pt) distributions for R=0.3 jets for central to peripheral events.
description: CERN-LHC. Measurements of charged-particle fragmentation functions of jets produced in ultra-relativistic nuclear collisions can provide insight into the modification of parton showers in the hot, dense medium created in the collisions. ATLAS has measured jets in sqrt(sNN) = 2.76 TeV PB PB collisions at the LHC using a data set recorded in 2011 with an integrated luminosity of 0.14 nb^{-1}. Jets were reconstructed using the anti-kt algorithm with distance parameter values R = 0.2, 0.3, and 0.4. 

Here is the summary of results for the charged particle (CH) longitudinal momentum fraction, Z = PT(CH).PT(JET)/ABS(PT(JET))**2, distributions, D(Z) = (1/N(JET))*D(N(CH))/DZ and distributions of transverse momenta of particles in jets, D(PT(CH)) = (1/N(JET))*D(N(CH))/DPT(CH). The jets have PT&gt;100 GeV, |ETA|&lt;2.1, and the particle to jet association is done using geometrical matching with DELTA R &lt;= 0.4 for all three different R values.
DOI: 10.17182/hepdata.64272.v1/t74
title: "Table 74" of "Measurement of inclusive jet charged-particle fragmentation functions in Pb+Pb collisions at sqrt(s_NN) = 2.76 TeV with the ATLAS detector"

description: Ratio of D(pt) distributions for R=0.3 jets for central to peripheral events.
description: CERN-LHC. Measurements of charged-particle fragmentation functions of jets produced in ultra-relativistic nuclear collisions can provide insight into the modification of parton showers in the hot, dense medium created in the collisions. ATLAS has measured jets in sqrt(sNN) = 2.76 TeV PB PB collisions at the LHC using a data set recorded in 2011 with an integrated luminosity of 0.14 nb^{-1}. Jets were reconstructed using the anti-kt algorithm with distance parameter values R = 0.2, 0.3, and 0.4. 

Here is the summary of results for the charged particle (CH) longitudinal momentum fraction, Z = PT(CH).PT(JET)/ABS(PT(JET))**2, distributions, D(Z) = (1/N(JET))*D(N(CH))/DZ and distributions of transverse momenta of particles in jets, D(PT(CH)) = (1/N(JET))*D(N(CH))/DPT(CH). The jets have PT&gt;100 GeV, |ETA|&lt;2.1, and the particle to jet association is done using geometrical matching with DELTA R &lt;= 0.4 for all three different R values.
DOI: 10.17182/hepdata.64272.v1/t75
title: "Table 75" of "Measurement of inclusive jet charged-particle fragmentation functions in Pb+Pb collisions at sqrt(s_NN) = 2.76 TeV with the ATLAS detector"

description: Ratio of D(pt) distributions for R=0.2 jets for central to peripheral events.
description: CERN-LHC. Measurements of charged-particle fragmentation functions of jets produced in ultra-relativistic nuclear collisions can provide insight into the modification of parton showers in the hot, dense medium created in the collisions. ATLAS has measured jets in sqrt(sNN) = 2.76 TeV PB PB collisions at the LHC using a data set recorded in 2011 with an integrated luminosity of 0.14 nb^{-1}. Jets were reconstructed using the anti-kt algorithm with distance parameter values R = 0.2, 0.3, and 0.4. 

Here is the summary of results for the charged particle (CH) longitudinal momentum fraction, Z = PT(CH).PT(JET)/ABS(PT(JET))**2, distributions, D(Z) = (1/N(JET))*D(N(CH))/DZ and distributions of transverse momenta of particles in jets, D(PT(CH)) = (1/N(JET))*D(N(CH))/DPT(CH). The jets have PT&gt;100 GeV, |ETA|&lt;2.1, and the particle to jet association is done using geometrical matching with DELTA R &lt;= 0.4 for all three different R values.
DOI: 10.17182/hepdata.64272.v1/t76
title: "Table 76" of "Measurement of inclusive jet charged-particle fragmentation functions in Pb+Pb collisions at sqrt(s_NN) = 2.76 TeV with the ATLAS detector"

description: Ratio of D(pt) distributions for R=0.2 jets for central to peripheral events.
description: CERN-LHC. Measurements of charged-particle fragmentation functions of jets produced in ultra-relativistic nuclear collisions can provide insight into the modification of parton showers in the hot, dense medium created in the collisions. ATLAS has measured jets in sqrt(sNN) = 2.76 TeV PB PB collisions at the LHC using a data set recorded in 2011 with an integrated luminosity of 0.14 nb^{-1}. Jets were reconstructed using the anti-kt algorithm with distance parameter values R = 0.2, 0.3, and 0.4. 

Here is the summary of results for the charged particle (CH) longitudinal momentum fraction, Z = PT(CH).PT(JET)/ABS(PT(JET))**2, distributions, D(Z) = (1/N(JET))*D(N(CH))/DZ and distributions of transverse momenta of particles in jets, D(PT(CH)) = (1/N(JET))*D(N(CH))/DPT(CH). The jets have PT&gt;100 GeV, |ETA|&lt;2.1, and the particle to jet association is done using geometrical matching with DELTA R &lt;= 0.4 for all three different R values.
DOI: 10.17182/hepdata.64272.v1/t77
title: "Table 77" of "Measurement of inclusive jet charged-particle fragmentation functions in Pb+Pb collisions at sqrt(s_NN) = 2.76 TeV with the ATLAS detector"

description: Ratio of D(pt) distributions for R=0.2 jets for central to peripheral events.
description: CERN-LHC. Measurements of charged-particle fragmentation functions of jets produced in ultra-relativistic nuclear collisions can provide insight into the modification of parton showers in the hot, dense medium created in the collisions. ATLAS has measured jets in sqrt(sNN) = 2.76 TeV PB PB collisions at the LHC using a data set recorded in 2011 with an integrated luminosity of 0.14 nb^{-1}. Jets were reconstructed using the anti-kt algorithm with distance parameter values R = 0.2, 0.3, and 0.4. 

Here is the summary of results for the charged particle (CH) longitudinal momentum fraction, Z = PT(CH).PT(JET)/ABS(PT(JET))**2, distributions, D(Z) = (1/N(JET))*D(N(CH))/DZ and distributions of transverse momenta of particles in jets, D(PT(CH)) = (1/N(JET))*D(N(CH))/DPT(CH). The jets have PT&gt;100 GeV, |ETA|&lt;2.1, and the particle to jet association is done using geometrical matching with DELTA R &lt;= 0.4 for all three different R values.
DOI: 10.17182/hepdata.64272.v1/t78
title: "Table 78" of "Measurement of inclusive jet charged-particle fragmentation functions in Pb+Pb collisions at sqrt(s_NN) = 2.76 TeV with the ATLAS detector"

description: Ratio of D(pt) distributions for R=0.2 jets for central to peripheral events.
description: CERN-LHC. Measurements of charged-particle fragmentation functions of jets produced in ultra-relativistic nuclear collisions can provide insight into the modification of parton showers in the hot, dense medium created in the collisions. ATLAS has measured jets in sqrt(sNN) = 2.76 TeV PB PB collisions at the LHC using a data set recorded in 2011 with an integrated luminosity of 0.14 nb^{-1}. Jets were reconstructed using the anti-kt algorithm with distance parameter values R = 0.2, 0.3, and 0.4. 

Here is the summary of results for the charged particle (CH) longitudinal momentum fraction, Z = PT(CH).PT(JET)/ABS(PT(JET))**2, distributions, D(Z) = (1/N(JET))*D(N(CH))/DZ and distributions of transverse momenta of particles in jets, D(PT(CH)) = (1/N(JET))*D(N(CH))/DPT(CH). The jets have PT&gt;100 GeV, |ETA|&lt;2.1, and the particle to jet association is done using geometrical matching with DELTA R &lt;= 0.4 for all three different R values.
DOI: 10.17182/hepdata.64272.v1/t79
title: "Table 79" of "Measurement of inclusive jet charged-particle fragmentation functions in Pb+Pb collisions at sqrt(s_NN) = 2.76 TeV with the ATLAS detector"

description: Ratio of D(pt) distributions for R=0.2 jets for central to peripheral events.
description: CERN-LHC. Measurements of charged-particle fragmentation functions of jets produced in ultra-relativistic nuclear collisions can provide insight into the modification of parton showers in the hot, dense medium created in the collisions. ATLAS has measured jets in sqrt(sNN) = 2.76 TeV PB PB collisions at the LHC using a data set recorded in 2011 with an integrated luminosity of 0.14 nb^{-1}. Jets were reconstructed using the anti-kt algorithm with distance parameter values R = 0.2, 0.3, and 0.4. 

Here is the summary of results for the charged particle (CH) longitudinal momentum fraction, Z = PT(CH).PT(JET)/ABS(PT(JET))**2, distributions, D(Z) = (1/N(JET))*D(N(CH))/DZ and distributions of transverse momenta of particles in jets, D(PT(CH)) = (1/N(JET))*D(N(CH))/DPT(CH). The jets have PT&gt;100 GeV, |ETA|&lt;2.1, and the particle to jet association is done using geometrical matching with DELTA R &lt;= 0.4 for all three different R values.
DOI: 10.17182/hepdata.43089.v1/t1
title: "Table 1" of "K*0 and phi Meson Production in Proton-Nucleus Interactions at sqrt(s) = 41.6 GeV"

description: Measured rapidity distribution for K*0 production in the accessible phase space.
description: DESY-HERA. Measurement of the inclusive production cross sections for the strange vector mesons K*0, K*BAR0 and PHI in the interaction of GeV protons with C, TI and WT targets. Differential cross sections in YRAP and PT**2 are given together with total cross sections and atomic number dependance both within the available, and extrapolated to full phase space.
DOI: 10.17182/hepdata.43089.v1/t2
title: "Table 2" of "K*0 and phi Meson Production in Proton-Nucleus Interactions at sqrt(s) = 41.6 GeV"

description: Measured rapidity distribution for K*BAR0 production in the accessible phase space.
description: DESY-HERA. Measurement of the inclusive production cross sections for the strange vector mesons K*0, K*BAR0 and PHI in the interaction of GeV protons with C, TI and WT targets. Differential cross sections in YRAP and PT**2 are given together with total cross sections and atomic number dependance both within the available, and extrapolated to full phase space.
DOI: 10.17182/hepdata.43089.v1/t3
title: "Table 3" of "K*0 and phi Meson Production in Proton-Nucleus Interactions at sqrt(s) = 41.6 GeV"

description: Measured rapidity distribution for PHI production in the accessible phase space.
description: DESY-HERA. Measurement of the inclusive production cross sections for the strange vector mesons K*0, K*BAR0 and PHI in the interaction of GeV protons with C, TI and WT targets. Differential cross sections in YRAP and PT**2 are given together with total cross sections and atomic number dependance both within the available, and extrapolated to full phase space.
DOI: 10.17182/hepdata.43089.v1/t5
title: "Table 5" of "K*0 and phi Meson Production in Proton-Nucleus Interactions at sqrt(s) = 41.6 GeV"

description: Measured transverse momentum distribution for K*BAR0 production in the accessible phase space.
description: DESY-HERA. Measurement of the inclusive production cross sections for the strange vector mesons K*0, K*BAR0 and PHI in the interaction of GeV protons with C, TI and WT targets. Differential cross sections in YRAP and PT**2 are given together with total cross sections and atomic number dependance both within the available, and extrapolated to full phase space.
DOI: 10.17182/hepdata.43089.v1/t6
title: "Table 6" of "K*0 and phi Meson Production in Proton-Nucleus Interactions at sqrt(s) = 41.6 GeV"

description: Measured transverse momentum distribution for PHI production in the accessible phase space.
description: DESY-HERA. Measurement of the inclusive production cross sections for the strange vector mesons K*0, K*BAR0 and PHI in the interaction of GeV protons with C, TI and WT targets. Differential cross sections in YRAP and PT**2 are given together with total cross sections and atomic number dependance both within the available, and extrapolated to full phase space.
DOI: 10.17182/hepdata.64272.v1/t80
title: "Table 80" of "Measurement of inclusive jet charged-particle fragmentation functions in Pb+Pb collisions at sqrt(s_NN) = 2.76 TeV with the ATLAS detector"

description: Ratio of D(pt) distributions for R=0.2 jets for central to peripheral events.
description: CERN-LHC. Measurements of charged-particle fragmentation functions of jets produced in ultra-relativistic nuclear collisions can provide insight into the modification of parton showers in the hot, dense medium created in the collisions. ATLAS has measured jets in sqrt(sNN) = 2.76 TeV PB PB collisions at the LHC using a data set recorded in 2011 with an integrated luminosity of 0.14 nb^{-1}. Jets were reconstructed using the anti-kt algorithm with distance parameter values R = 0.2, 0.3, and 0.4. 

Here is the summary of results for the charged particle (CH) longitudinal momentum fraction, Z = PT(CH).PT(JET)/ABS(PT(JET))**2, distributions, D(Z) = (1/N(JET))*D(N(CH))/DZ and distributions of transverse momenta of particles in jets, D(PT(CH)) = (1/N(JET))*D(N(CH))/DPT(CH). The jets have PT&gt;100 GeV, |ETA|&lt;2.1, and the particle to jet association is done using geometrical matching with DELTA R &lt;= 0.4 for all three different R values.
DOI: 10.17182/hepdata.43089.v1/t4
title: "Table 4" of "K*0 and phi Meson Production in Proton-Nucleus Interactions at sqrt(s) = 41.6 GeV"

description: Measured transverse momentum distribution for K*0 production in the accessible phase space.
description: DESY-HERA. Measurement of the inclusive production cross sections for the strange vector mesons K*0, K*BAR0 and PHI in the interaction of GeV protons with C, TI and WT targets. Differential cross sections in YRAP and PT**2 are given together with total cross sections and atomic number dependance both within the available, and extrapolated to full phase space.
DOI: 10.17182/hepdata.43089.v1/t7
title: "Table 7" of "K*0 and phi Meson Production in Proton-Nucleus Interactions at sqrt(s) = 41.6 GeV"

description: Cross sections for K*0 and K*BAR0 production integrated over the accessiblephase space.
description: DESY-HERA. Measurement of the inclusive production cross sections for the strange vector mesons K*0, K*BAR0 and PHI in the interaction of GeV protons with C, TI and WT targets. Differential cross sections in YRAP and PT**2 are given together with total cross sections and atomic number dependance both within the available, and extrapolated to full phase space.
DOI: 10.17182/hepdata.43089.v1/t8
title: "Table 8" of "K*0 and phi Meson Production in Proton-Nucleus Interactions at sqrt(s) = 41.6 GeV"

description: Cross sections for K*0 and K*BAR0 production extrapolated to full phase space.
description: DESY-HERA. Measurement of the inclusive production cross sections for the strange vector mesons K*0, K*BAR0 and PHI in the interaction of GeV protons with C, TI and WT targets. Differential cross sections in YRAP and PT**2 are given together with total cross sections and atomic number dependance both within the available, and extrapolated to full phase space.
DOI: 10.17182/hepdata.43089.v1/t9
title: "Table 9" of "K*0 and phi Meson Production in Proton-Nucleus Interactions at sqrt(s) = 41.6 GeV"

description: Cross sections for PHI production integrated over the accessible phase space.
description: DESY-HERA. Measurement of the inclusive production cross sections for the strange vector mesons K*0, K*BAR0 and PHI in the interaction of GeV protons with C, TI and WT targets. Differential cross sections in YRAP and PT**2 are given together with total cross sections and atomic number dependance both within the available, and extrapolated to full phase space.
DOI: 10.17182/hepdata.43089.v1/t10
title: "Table 10" of "K*0 and phi Meson Production in Proton-Nucleus Interactions at sqrt(s) = 41.6 GeV"

description: Cross sections for PHI production extrapolated to full phase space.
description: DESY-HERA. Measurement of the inclusive production cross sections for the strange vector mesons K*0, K*BAR0 and PHI in the interaction of GeV protons with C, TI and WT targets. Differential cross sections in YRAP and PT**2 are given together with total cross sections and atomic number dependance both within the available, and extrapolated to full phase space.
DOI: 10.17182/hepdata.43089.v1/t11
title: "Table 11" of "K*0 and phi Meson Production in Proton-Nucleus Interactions at sqrt(s) = 41.6 GeV"

description: Measured A dependence of K*0 production in the accessible phase space.
description: DESY-HERA. Measurement of the inclusive production cross sections for the strange vector mesons K*0, K*BAR0 and PHI in the interaction of GeV protons with C, TI and WT targets. Differential cross sections in YRAP and PT**2 are given together with total cross sections and atomic number dependance both within the available, and extrapolated to full phase space.
DOI: 10.17182/hepdata.43089.v1/t13
title: "Table 13" of "K*0 and phi Meson Production in Proton-Nucleus Interactions at sqrt(s) = 41.6 GeV"

description: Measured A dependence of PHI production in the accessible phase space.
description: DESY-HERA. Measurement of the inclusive production cross sections for the strange vector mesons K*0, K*BAR0 and PHI in the interaction of GeV protons with C, TI and WT targets. Differential cross sections in YRAP and PT**2 are given together with total cross sections and atomic number dependance both within the available, and extrapolated to full phase space.
DOI: 10.17182/hepdata.43089.v1/t12
title: "Table 12" of "K*0 and phi Meson Production in Proton-Nucleus Interactions at sqrt(s) = 41.6 GeV"

description: Measured A dependence of K*BAR0 production in the accessible phase space.
description: DESY-HERA. Measurement of the inclusive production cross sections for the strange vector mesons K*0, K*BAR0 and PHI in the interaction of GeV protons with C, TI and WT targets. Differential cross sections in YRAP and PT**2 are given together with total cross sections and atomic number dependance both within the available, and extrapolated to full phase space.
DOI: 10.6084/m9.figshare.28369472.v5
title: Evolution in response to an abiotic stress shapes species coexistence - Data and scripts

description: # evolution_cadmium_coexistenceThis material is a companion to the paper "Evolution in response to an abiotic stress shapes species coexistence"This information is also available in the git repository: https://github.com/irfragata/evolution_cadmium_coexistenceThe scripts available allow with the data set provided to replicate all the analyses done in the paper, as well as the figures.Inside each folder there is a ReadMe file explaining the different files and folder available. The general description of the folder is as follows:The Data folder contains the raw dataThe Code folder contains the scripts to perform the analysesThe Analyses folder contains intermediate outputs required for the analyses.The Plots folder contains the figures used in the manuscript (output from the code)Given that running the cxr package requires sometime, we provided the intermediate files used to generate the figure, but we also provide the code done to generate the files, to ensure the total reproducibility analyses.For the purpose of Open Access, a CC-BY 4.0 public copyright licence has been applied to the contents of this repository.<br>
DOI: 10.17182/hepdata.89325.v1/t1
title: "Figure1_Panel1" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: NchRec v.s. Et
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t2
title: "Figure1_Panel2" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: w.r.t. Et
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t3
title: "Figure1_Panel3" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: w.r.t. NchRec
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t4
title: "Figure2_Panel1" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: Et distribution
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t5
title: "Figure2_Panel2" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: NchRec distribution
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t6
title: "Figure3_Panel1_pt0" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: v_2{2}, 3-subevent, 0.5
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t7
title: "Figure3_Panel1_pt1" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: v_2{2}, 3-subevent, 1.0
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t8
title: "Figure3_Panel1_pt2" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: v_2{2}, 3-subevent, 1.5
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t9
title: "Figure3_Panel1_pt3" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: v_2{2}, 3-subevent, 2.0
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t10
title: "Figure3_Panel2_pt0" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: v_3{2}, 3-subevent, 0.5
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t11
title: "Figure3_Panel2_pt1" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: v_3{2}, 3-subevent, 1.0
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t12
title: "Figure3_Panel2_pt2" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: v_3{2}, 3-subevent, 1.5
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t13
title: "Figure3_Panel2_pt3" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: v_3{2}, 3-subevent, 2.0
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t17
title: "Figure3_Panel3_pt3" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: v_4{2}, 3-subevent, 2.0
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t14
title: "Figure3_Panel3_pt0" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: v_4{2}, 3-subevent, 0.5
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t15
title: "Figure3_Panel3_pt1" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: v_4{2}, 3-subevent, 1.0
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t16
title: "Figure3_Panel3_pt2" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: v_4{2}, 3-subevent, 1.5
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t18
title: "Figure4_Panel1_pt0" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: nc_2{4}, standard, 0.5
description: No data abstract available.
DOI: 10.17182/hepdata.89325.v1/t19
title: "Figure4_Panel1_pt1" of "Fluctuations of anisotropic flow in Pb+Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}} $ = 5.02 TeV with the ATLAS detector"

description: nc_2{4}, standard, 1.0
description: No data abstract available.