cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.77015.v2/t9
title: "Table 9" of "Suppression and azimuthal anisotropy of prompt and nonprompt J/psi production in PbPb collisions at sqrt(s[NN]) = 2.76 TeV"

description: Nonprompt J/$\psi$ $v_{2}$ as a function of $p_{\rm T}$.
description: CERN-LHC. The nuclear modification factor $R_{AA}$ and the azimuthal anisotropy coefficient $v_{2}$ of prompt and nonprompt (i.e. those from decays of b hadrons) J/$\psi$ mesons, measured from PbPb and pp collisions at $\sqrt{\mathrm{s_{NN}}}$=2.76 TeV at the LHC, are reported. The results are presented in several event centrality intervals and several kinematic regions, for transverse momenta $p_{T}&gt;$6.5 GeV/c and rapidity $|y|&lt;$2.4, extending down to $p_{T}$=3 GeV/c in the 1.6$&lt;|y|&lt;$2.4 range. The $v_{2}$ of prompt J/$\psi$ is found to be nonzero and constant over the full kinematic range studied, while the measured $v_{2}$ of nonprompt J/$\psi$ is consistent with zero. The $R_{AA}$ of prompt J/$\psi$ exhibits a suppression that increases with centrality but does not vary as a function of either y or $p_{T}$ in the fiducial range. The nonprompt J/$\psi$ $R_{AA}$ shows a suppression which becomes stronger as rapidity or $p_{T}$ increase. The $v_{2}$ and nuclear suppression of open and hidden charm, and of open charm and beauty, are compared. 

See arXiv:1610.00613 for more details.
DOI: 10.5281/zenodo.18267876
title: Data and Code for "Mountain Resonance Control on Earthquake-Induced Landslides"
DOI: 10.5281/zenodo.18267877
title: Data and Code for "Mountain Resonance Control on Earthquake-Induced Landslides"
DOI: 10.17182/hepdata.77015.v2/t10
title: "Table 10" of "Suppression and azimuthal anisotropy of prompt and nonprompt J/psi production in PbPb collisions at sqrt(s[NN]) = 2.76 TeV"

description: Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.
description: CERN-LHC. The nuclear modification factor $R_{AA}$ and the azimuthal anisotropy coefficient $v_{2}$ of prompt and nonprompt (i.e. those from decays of b hadrons) J/$\psi$ mesons, measured from PbPb and pp collisions at $\sqrt{\mathrm{s_{NN}}}$=2.76 TeV at the LHC, are reported. The results are presented in several event centrality intervals and several kinematic regions, for transverse momenta $p_{T}&gt;$6.5 GeV/c and rapidity $|y|&lt;$2.4, extending down to $p_{T}$=3 GeV/c in the 1.6$&lt;|y|&lt;$2.4 range. The $v_{2}$ of prompt J/$\psi$ is found to be nonzero and constant over the full kinematic range studied, while the measured $v_{2}$ of nonprompt J/$\psi$ is consistent with zero. The $R_{AA}$ of prompt J/$\psi$ exhibits a suppression that increases with centrality but does not vary as a function of either y or $p_{T}$ in the fiducial range. The nonprompt J/$\psi$ $R_{AA}$ shows a suppression which becomes stronger as rapidity or $p_{T}$ increase. The $v_{2}$ and nuclear suppression of open and hidden charm, and of open charm and beauty, are compared. 

See arXiv:1610.00613 for more details.
DOI: 10.17182/hepdata.77015.v2/t11
title: "Table 11" of "Suppression and azimuthal anisotropy of prompt and nonprompt J/psi production in PbPb collisions at sqrt(s[NN]) = 2.76 TeV"

description: Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of rapidity.
description: CERN-LHC. The nuclear modification factor $R_{AA}$ and the azimuthal anisotropy coefficient $v_{2}$ of prompt and nonprompt (i.e. those from decays of b hadrons) J/$\psi$ mesons, measured from PbPb and pp collisions at $\sqrt{\mathrm{s_{NN}}}$=2.76 TeV at the LHC, are reported. The results are presented in several event centrality intervals and several kinematic regions, for transverse momenta $p_{T}&gt;$6.5 GeV/c and rapidity $|y|&lt;$2.4, extending down to $p_{T}$=3 GeV/c in the 1.6$&lt;|y|&lt;$2.4 range. The $v_{2}$ of prompt J/$\psi$ is found to be nonzero and constant over the full kinematic range studied, while the measured $v_{2}$ of nonprompt J/$\psi$ is consistent with zero. The $R_{AA}$ of prompt J/$\psi$ exhibits a suppression that increases with centrality but does not vary as a function of either y or $p_{T}$ in the fiducial range. The nonprompt J/$\psi$ $R_{AA}$ shows a suppression which becomes stronger as rapidity or $p_{T}$ increase. The $v_{2}$ and nuclear suppression of open and hidden charm, and of open charm and beauty, are compared. 

See arXiv:1610.00613 for more details.
DOI: 10.17182/hepdata.77015.v2/t12
title: "Table 12" of "Suppression and azimuthal anisotropy of prompt and nonprompt J/psi production in PbPb collisions at sqrt(s[NN]) = 2.76 TeV"

description: Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of $p_{\rm T}$.
description: CERN-LHC. The nuclear modification factor $R_{AA}$ and the azimuthal anisotropy coefficient $v_{2}$ of prompt and nonprompt (i.e. those from decays of b hadrons) J/$\psi$ mesons, measured from PbPb and pp collisions at $\sqrt{\mathrm{s_{NN}}}$=2.76 TeV at the LHC, are reported. The results are presented in several event centrality intervals and several kinematic regions, for transverse momenta $p_{T}&gt;$6.5 GeV/c and rapidity $|y|&lt;$2.4, extending down to $p_{T}$=3 GeV/c in the 1.6$&lt;|y|&lt;$2.4 range. The $v_{2}$ of prompt J/$\psi$ is found to be nonzero and constant over the full kinematic range studied, while the measured $v_{2}$ of nonprompt J/$\psi$ is consistent with zero. The $R_{AA}$ of prompt J/$\psi$ exhibits a suppression that increases with centrality but does not vary as a function of either y or $p_{T}$ in the fiducial range. The nonprompt J/$\psi$ $R_{AA}$ shows a suppression which becomes stronger as rapidity or $p_{T}$ increase. The $v_{2}$ and nuclear suppression of open and hidden charm, and of open charm and beauty, are compared. 

See arXiv:1610.00613 for more details.
DOI: 10.17182/hepdata.77015.v2/t13
title: "Table 13" of "Suppression and azimuthal anisotropy of prompt and nonprompt J/psi production in PbPb collisions at sqrt(s[NN]) = 2.76 TeV"

description: Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.
description: CERN-LHC. The nuclear modification factor $R_{AA}$ and the azimuthal anisotropy coefficient $v_{2}$ of prompt and nonprompt (i.e. those from decays of b hadrons) J/$\psi$ mesons, measured from PbPb and pp collisions at $\sqrt{\mathrm{s_{NN}}}$=2.76 TeV at the LHC, are reported. The results are presented in several event centrality intervals and several kinematic regions, for transverse momenta $p_{T}&gt;$6.5 GeV/c and rapidity $|y|&lt;$2.4, extending down to $p_{T}$=3 GeV/c in the 1.6$&lt;|y|&lt;$2.4 range. The $v_{2}$ of prompt J/$\psi$ is found to be nonzero and constant over the full kinematic range studied, while the measured $v_{2}$ of nonprompt J/$\psi$ is consistent with zero. The $R_{AA}$ of prompt J/$\psi$ exhibits a suppression that increases with centrality but does not vary as a function of either y or $p_{T}$ in the fiducial range. The nonprompt J/$\psi$ $R_{AA}$ shows a suppression which becomes stronger as rapidity or $p_{T}$ increase. The $v_{2}$ and nuclear suppression of open and hidden charm, and of open charm and beauty, are compared. 

See arXiv:1610.00613 for more details.
DOI: 10.17182/hepdata.77015.v2/t14
title: "Table 14" of "Suppression and azimuthal anisotropy of prompt and nonprompt J/psi production in PbPb collisions at sqrt(s[NN]) = 2.76 TeV"

description: Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.
description: CERN-LHC. The nuclear modification factor $R_{AA}$ and the azimuthal anisotropy coefficient $v_{2}$ of prompt and nonprompt (i.e. those from decays of b hadrons) J/$\psi$ mesons, measured from PbPb and pp collisions at $\sqrt{\mathrm{s_{NN}}}$=2.76 TeV at the LHC, are reported. The results are presented in several event centrality intervals and several kinematic regions, for transverse momenta $p_{T}&gt;$6.5 GeV/c and rapidity $|y|&lt;$2.4, extending down to $p_{T}$=3 GeV/c in the 1.6$&lt;|y|&lt;$2.4 range. The $v_{2}$ of prompt J/$\psi$ is found to be nonzero and constant over the full kinematic range studied, while the measured $v_{2}$ of nonprompt J/$\psi$ is consistent with zero. The $R_{AA}$ of prompt J/$\psi$ exhibits a suppression that increases with centrality but does not vary as a function of either y or $p_{T}$ in the fiducial range. The nonprompt J/$\psi$ $R_{AA}$ shows a suppression which becomes stronger as rapidity or $p_{T}$ increase. The $v_{2}$ and nuclear suppression of open and hidden charm, and of open charm and beauty, are compared. 

See arXiv:1610.00613 for more details.
DOI: 10.17182/hepdata.77015.v2/t8
title: "Table 8" of "Suppression and azimuthal anisotropy of prompt and nonprompt J/psi production in PbPb collisions at sqrt(s[NN]) = 2.76 TeV"

description: Prompt J/$\psi$ $R_{\rm AA}$ as a function of centrality, at forward rapidity, 1.6$&lt;|y|&lt;$2.4, for two different $p_{\rm T}$ regions.
description: CERN-LHC. The nuclear modification factor $R_{AA}$ and the azimuthal anisotropy coefficient $v_{2}$ of prompt and nonprompt (i.e. those from decays of b hadrons) J/$\psi$ mesons, measured from PbPb and pp collisions at $\sqrt{\mathrm{s_{NN}}}$=2.76 TeV at the LHC, are reported. The results are presented in several event centrality intervals and several kinematic regions, for transverse momenta $p_{T}&gt;$6.5 GeV/c and rapidity $|y|&lt;$2.4, extending down to $p_{T}$=3 GeV/c in the 1.6$&lt;|y|&lt;$2.4 range. The $v_{2}$ of prompt J/$\psi$ is found to be nonzero and constant over the full kinematic range studied, while the measured $v_{2}$ of nonprompt J/$\psi$ is consistent with zero. The $R_{AA}$ of prompt J/$\psi$ exhibits a suppression that increases with centrality but does not vary as a function of either y or $p_{T}$ in the fiducial range. The nonprompt J/$\psi$ $R_{AA}$ shows a suppression which becomes stronger as rapidity or $p_{T}$ increase. The $v_{2}$ and nuclear suppression of open and hidden charm, and of open charm and beauty, are compared. 

See arXiv:1610.00613 for more details.
DOI: 10.17182/hepdata.82637.v1/t1
title: "Table 1" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 2nd order event plane from Pb-going side in pPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t2
title: "Table 2" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 2nd order event plane from p-going side in pPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t3
title: "Table 3" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 2nd order event plane in PbPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t4
title: "Table 4" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 3rd order event plane from Pb-going side in pPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t5
title: "Table 5" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 3rd order event plane from p-going side in pPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t6
title: "Table 6" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 3rd order event plane in PbPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t7
title: "Table 7" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Two-particle correlation in pPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t8
title: "Table 8" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Two-particle correlation in PbPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t10
title: "Table 10" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 2nd order event plane from p-going side in pPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t11
title: "Table 11" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 2nd order event plane in PbPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t12
title: "Table 12" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 3rd order event plane from Pb-going side in pPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t13
title: "Table 13" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 3rd order event plane from p-going side in pPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t14
title: "Table 14" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 3rd order event plane in PbPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t15
title: "Table 15" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Two-particle correlation in pPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t9
title: "Table 9" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 2nd order event plane from Pb-going side in pPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.66548.v1/t1
title: "Table 1" of "Measurement of prompt psi(2S) to J/psi yield ratios in PbPb and pp collisions at sqrt(s[NN]) = 2.76 TeV"

description: Double ratio of measured yields, $(N_{\psi\mathrm{(2S)}} / N_{J/\psi})_{\mathrm{PbPb}} / (N_{\psi\mathrm{(2S)}} / N_{J/\psi})_{pp}$, as a function of centrality, for the midrapidity analysis bin.
description: CERN-LHC. The ratio between the prompt psi(2S) and J/psi yields, reconstructed via their decays into muon pairs, is measured in lead-lead and proton-proton collisions at a centre-of-mass energy per nucleon-nucleon pair of 2.76 TeV. The analysis is based on lead-lead and proton-proton data samples collected by CMS at the LHC, corresponding to integrated luminosities of 150 mub^-1 and 5.4 pb^-1, respectively. The double ratio of measured yields, $(N_{\psi\mathrm{(2S)}} / N_{J/\psi})_{\mathrm{PbPb}} / (N_{\psi\mathrm{(2S)}} / N_{J/\psi})_{pp}$, is computed in three lead-lead collision centrality bins and two kinematic ranges: one at midrapidity, |y|&lt;1.6, covering the transverse momentum range 6.5
DOI: 10.17182/hepdata.66548.v1/t2
title: "Table 2" of "Measurement of prompt psi(2S) to J/psi yield ratios in PbPb and pp collisions at sqrt(s[NN]) = 2.76 TeV"

description: Double ratio of measured yields, $(N_{\psi\mathrm{(2S)}} / N_{J/\psi})_{\mathrm{PbPb}} / (N_{\psi\mathrm{(2S)}} / N_{J/\psi})_{pp}$, as a function of centrality, for the forward rapidity analysis bin.
description: CERN-LHC. The ratio between the prompt psi(2S) and J/psi yields, reconstructed via their decays into muon pairs, is measured in lead-lead and proton-proton collisions at a centre-of-mass energy per nucleon-nucleon pair of 2.76 TeV. The analysis is based on lead-lead and proton-proton data samples collected by CMS at the LHC, corresponding to integrated luminosities of 150 mub^-1 and 5.4 pb^-1, respectively. The double ratio of measured yields, $(N_{\psi\mathrm{(2S)}} / N_{J/\psi})_{\mathrm{PbPb}} / (N_{\psi\mathrm{(2S)}} / N_{J/\psi})_{pp}$, is computed in three lead-lead collision centrality bins and two kinematic ranges: one at midrapidity, |y|&lt;1.6, covering the transverse momentum range 6.5
DOI: 10.17182/hepdata.66548.v1/t3
title: "Table 3" of "Measurement of prompt psi(2S) to J/psi yield ratios in PbPb and pp collisions at sqrt(s[NN]) = 2.76 TeV"

description: Double ratio of measured yields, $(N_{\psi\mathrm{(2S)}} / N_{J/\psi})_{\mathrm{PbPb}} / (N_{\psi\mathrm{(2S)}} / N_{J/\psi})_{pp}$, integrated over centrality, for the midrapidity and forward rapidity analysis bins.
description: CERN-LHC. The ratio between the prompt psi(2S) and J/psi yields, reconstructed via their decays into muon pairs, is measured in lead-lead and proton-proton collisions at a centre-of-mass energy per nucleon-nucleon pair of 2.76 TeV. The analysis is based on lead-lead and proton-proton data samples collected by CMS at the LHC, corresponding to integrated luminosities of 150 mub^-1 and 5.4 pb^-1, respectively. The double ratio of measured yields, $(N_{\psi\mathrm{(2S)}} / N_{J/\psi})_{\mathrm{PbPb}} / (N_{\psi\mathrm{(2S)}} / N_{J/\psi})_{pp}$, is computed in three lead-lead collision centrality bins and two kinematic ranges: one at midrapidity, |y|&lt;1.6, covering the transverse momentum range 6.5
DOI: 10.17182/hepdata.66548.v1/t4
title: "Table 4" of "Measurement of prompt psi(2S) to J/psi yield ratios in PbPb and pp collisions at sqrt(s[NN]) = 2.76 TeV"

description: Nuclear modification factor RAA of psi(2S) integrated over centrality, for the midrapidity and forward rapidity analysis bins.
description: CERN-LHC. The ratio between the prompt psi(2S) and J/psi yields, reconstructed via their decays into muon pairs, is measured in lead-lead and proton-proton collisions at a centre-of-mass energy per nucleon-nucleon pair of 2.76 TeV. The analysis is based on lead-lead and proton-proton data samples collected by CMS at the LHC, corresponding to integrated luminosities of 150 mub^-1 and 5.4 pb^-1, respectively. The double ratio of measured yields, $(N_{\psi\mathrm{(2S)}} / N_{J/\psi})_{\mathrm{PbPb}} / (N_{\psi\mathrm{(2S)}} / N_{J/\psi})_{pp}$, is computed in three lead-lead collision centrality bins and two kinematic ranges: one at midrapidity, |y|&lt;1.6, covering the transverse momentum range 6.5
DOI: 10.17182/hepdata.82637.v1/t16
title: "Table 16" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Two-particle correlation in PbPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t17
title: "Table 17" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 2nd order event plane from Pb-going side in pPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t18
title: "Table 18" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 2nd order event plane from p-going side in pPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t19
title: "Table 19" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 2nd order event plane in PbPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t20
title: "Table 20" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 3rd order event plane from Pb-going side in pPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t21
title: "Table 21" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 3rd order event plane from p-going side in pPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.
DOI: 10.17182/hepdata.82637.v1/t22
title: "Table 22" of "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC"

description: Three-particle correlation with respect to the 3rd order event plane in PbPb collisions.
description: CERN-LHC. Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the LHC.