cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.77601.v1/t5
title: "Table 4" of "Measurement of inclusive jet cross-sections in pp and PbPb collisions at sqrt(s[NN])=2.76 TeV"

description: Inclusive jet cross section in pp collisions, for anti-k$_T$ jets with a distance parameter $R=0.2, 0.3, 0.4$, reconstructed in $|\eta|&lt;0.2$. The '3.7%' luminosity uncertainty is a fully correlated uncertainty, and not included in the point-to-point uncertainty.
description: CERN-LHC. Inclusive jet spectra from pp and PbPb collisions at 2.76 TeV collected by the CMS experiment. Jets are reconstructed with three different distance parameters (R=0.2, 0.3, and 0.4) for transverse momentum pT&gt;70GeV/c and pseudorapidity |eta|&lt;2. The production cross sections and nuclear modification factor RAA is presented as function of pT and event centrality, for each R.
DOI: 10.17182/hepdata.77601.v1/t6
title: "Table 5" of "Measurement of inclusive jet cross-sections in pp and PbPb collisions at sqrt(s[NN])=2.76 TeV"

description: Inclusive jet spectra in different centrality bins of PbPb collisions, for anti-k$_T$ jets of distance parameter $R=0.2$, reconstructed in $|\eta|&lt;0.2$. The PbPb spectra in each case are scaled by TAA. The uncertainty on the TAA is considered as global uncertainty (common to all points for a given centrality), and it is not included in the point-to-point uncertainties.
description: CERN-LHC. Inclusive jet spectra from pp and PbPb collisions at 2.76 TeV collected by the CMS experiment. Jets are reconstructed with three different distance parameters (R=0.2, 0.3, and 0.4) for transverse momentum pT&gt;70GeV/c and pseudorapidity |eta|&lt;2. The production cross sections and nuclear modification factor RAA is presented as function of pT and event centrality, for each R.
DOI: 10.17182/hepdata.77601.v1/t7
title: "Table 6" of "Measurement of inclusive jet cross-sections in pp and PbPb collisions at sqrt(s[NN])=2.76 TeV"

description: Inclusive jet spectra in different centrality bins of PbPb collisions, for anti-k$_T$ jets of distance parameter $R=0.3$, reconstructed in $|\eta|&lt;0.2$. The PbPb spectra in each case are scaled by TAA. The uncertainty on the TAA is considered as global uncertainty (common to all points for a given centrality), and it is not included in the point-to-point uncertainties.
description: CERN-LHC. Inclusive jet spectra from pp and PbPb collisions at 2.76 TeV collected by the CMS experiment. Jets are reconstructed with three different distance parameters (R=0.2, 0.3, and 0.4) for transverse momentum pT&gt;70GeV/c and pseudorapidity |eta|&lt;2. The production cross sections and nuclear modification factor RAA is presented as function of pT and event centrality, for each R.
DOI: 10.17182/hepdata.77601.v1/t8
title: "Table 7" of "Measurement of inclusive jet cross-sections in pp and PbPb collisions at sqrt(s[NN])=2.76 TeV"

description: Inclusive jet spectra in different centrality bins of PbPb collisions, for anti-k$_T$ jets of distance parameter $R=0.4$, reconstructed in $|\eta|&lt;0.2$. The PbPb spectra in each case are scaled by TAA. The uncertainty on the TAA is considered as global uncertainty (common to all points for a given centrality), and it is not included in the point-to-point uncertainties.
description: CERN-LHC. Inclusive jet spectra from pp and PbPb collisions at 2.76 TeV collected by the CMS experiment. Jets are reconstructed with three different distance parameters (R=0.2, 0.3, and 0.4) for transverse momentum pT&gt;70GeV/c and pseudorapidity |eta|&lt;2. The production cross sections and nuclear modification factor RAA is presented as function of pT and event centrality, for each R.
DOI: 10.17182/hepdata.88289.v1/t89
title: "Table 89" of "Mixed higher-order anisotropic flow and nonlinear response coefficients of charged particles in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 2.76 and 5.02 TeV"

description: Nonlinear response coefficient $\chi_{633}$ from the scalar-product method at 2.76 TeV as a function of centrality.
description: Anisotropies in the initial energy density distribution of the quark-gluon plasma created in high energy heavy ion collisions lead to anisotropies in the azimuthal distributions of the final-state particles known as collective anisotropic flow. Fourier harmonic decomposition is used to quantify these anisotropies. The higher-order harmonics can be induced by the same order anisotropies (linear response) or by the combined influence of several lower order anisotropies (nonlinear response) in the initial state. The mixed higher-order anisotropic flow and nonlinear response coefficients of charged particles are measured as functions of transverse momentum and centrality in PbPb collisions at nucleon-nucleon center-of-mass energies $\sqrt{\smash[b]{s_{_{\mathrm{NN}}}}} = 2.76$ and $5.02$ TeV with the CMS detector. The results are compared with viscous hydrodynamic calculations using several different initial conditions, as well as microscopic transport model calculations. None of the models provides a simultaneous description of the mixed higher-order flow harmonics and nonlinear response coefficients.
DOI: 10.17182/hepdata.88289.v1/t90
title: "Table 90" of "Mixed higher-order anisotropic flow and nonlinear response coefficients of charged particles in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 2.76 and 5.02 TeV"

description: Nonlinear response coefficient $\chi_{7223}$ from the scalar-product method at 2.76 TeV as a function of centrality.
description: Anisotropies in the initial energy density distribution of the quark-gluon plasma created in high energy heavy ion collisions lead to anisotropies in the azimuthal distributions of the final-state particles known as collective anisotropic flow. Fourier harmonic decomposition is used to quantify these anisotropies. The higher-order harmonics can be induced by the same order anisotropies (linear response) or by the combined influence of several lower order anisotropies (nonlinear response) in the initial state. The mixed higher-order anisotropic flow and nonlinear response coefficients of charged particles are measured as functions of transverse momentum and centrality in PbPb collisions at nucleon-nucleon center-of-mass energies $\sqrt{\smash[b]{s_{_{\mathrm{NN}}}}} = 2.76$ and $5.02$ TeV with the CMS detector. The results are compared with viscous hydrodynamic calculations using several different initial conditions, as well as microscopic transport model calculations. None of the models provides a simultaneous description of the mixed higher-order flow harmonics and nonlinear response coefficients.
DOI: 10.17182/hepdata.77015.v2/t1
title: "Table 1" 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/$\psi$ $v_{2}$ 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.77601.v1/t10
title: "Table 8b" of "Measurement of inclusive jet cross-sections in pp and PbPb collisions at sqrt(s[NN])=2.76 TeV"

description: Inclusive jet RAA as a function of jet $p_T$, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3, 0.4$, with $|\eta|&lt;2$, for 5-10\% PbPb centrality. The '5.9%' combined uncertainty on the pp luminosity and PbPb TAA is considered as global uncertainty (common to all points), and it is not included in the point-to-point uncertainties.
description: CERN-LHC. Inclusive jet spectra from pp and PbPb collisions at 2.76 TeV collected by the CMS experiment. Jets are reconstructed with three different distance parameters (R=0.2, 0.3, and 0.4) for transverse momentum pT&gt;70GeV/c and pseudorapidity |eta|&lt;2. The production cross sections and nuclear modification factor RAA is presented as function of pT and event centrality, for each R.
DOI: 10.17182/hepdata.77601.v1/t11
title: "Table 8c" of "Measurement of inclusive jet cross-sections in pp and PbPb collisions at sqrt(s[NN])=2.76 TeV"

description: Inclusive jet RAA as a function of jet $p_T$, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3, 0.4$, with $|\eta|&lt;2$, for 10-30\% PbPb centrality. The '6.9%' combined uncertainty on the pp luminosity and PbPb TAA is considered as global uncertainty (common to all points), and it is not included in the point-to-point uncertainties.
description: CERN-LHC. Inclusive jet spectra from pp and PbPb collisions at 2.76 TeV collected by the CMS experiment. Jets are reconstructed with three different distance parameters (R=0.2, 0.3, and 0.4) for transverse momentum pT&gt;70GeV/c and pseudorapidity |eta|&lt;2. The production cross sections and nuclear modification factor RAA is presented as function of pT and event centrality, for each R.
DOI: 10.17182/hepdata.77601.v1/t12
title: "Table 8d" of "Measurement of inclusive jet cross-sections in pp and PbPb collisions at sqrt(s[NN])=2.76 TeV"

description: Inclusive jet RAA as a function of jet $p_T$, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3, 0.4$, with $|\eta|&lt;2$, for 30-50\% PbPb centrality. The '10%' combined uncertainty on the pp luminosity and PbPb TAA is considered as global uncertainty (common to all points), and it is not included in the point-to-point uncertainties.
description: CERN-LHC. Inclusive jet spectra from pp and PbPb collisions at 2.76 TeV collected by the CMS experiment. Jets are reconstructed with three different distance parameters (R=0.2, 0.3, and 0.4) for transverse momentum pT&gt;70GeV/c and pseudorapidity |eta|&lt;2. The production cross sections and nuclear modification factor RAA is presented as function of pT and event centrality, for each R.
DOI: 10.17182/hepdata.77601.v1/t13
title: "Table 8e" of "Measurement of inclusive jet cross-sections in pp and PbPb collisions at sqrt(s[NN])=2.76 TeV"

description: Inclusive jet RAA as a function of jet $p_T$, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3, 0.4$, with $|\eta|&lt;2$, for 50-70\% PbPb centrality. The '15%' combined uncertainty on the pp luminosity and PbPb TAA is considered as global uncertainty (common to all points), and it is not included in the point-to-point uncertainties.
description: CERN-LHC. Inclusive jet spectra from pp and PbPb collisions at 2.76 TeV collected by the CMS experiment. Jets are reconstructed with three different distance parameters (R=0.2, 0.3, and 0.4) for transverse momentum pT&gt;70GeV/c and pseudorapidity |eta|&lt;2. The production cross sections and nuclear modification factor RAA is presented as function of pT and event centrality, for each R.
DOI: 10.17182/hepdata.77601.v1/t14
title: "Table 8f" of "Measurement of inclusive jet cross-sections in pp and PbPb collisions at sqrt(s[NN])=2.76 TeV"

description: Inclusive jet RAA as a function of jet $p_T$, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3, 0.4$, with $|\eta|&lt;2$, for 70-90\% PbPb centrality. The '18%' combined uncertainty on the pp luminosity and PbPb TAA is considered as global uncertainty (common to all points), and it is not included in the point-to-point uncertainties.
description: CERN-LHC. Inclusive jet spectra from pp and PbPb collisions at 2.76 TeV collected by the CMS experiment. Jets are reconstructed with three different distance parameters (R=0.2, 0.3, and 0.4) for transverse momentum pT&gt;70GeV/c and pseudorapidity |eta|&lt;2. The production cross sections and nuclear modification factor RAA is presented as function of pT and event centrality, for each R.
DOI: 10.17182/hepdata.77601.v1/t15
title: "Table 9a" of "Measurement of inclusive jet cross-sections in pp and PbPb collisions at sqrt(s[NN])=2.76 TeV"

description: Inclusive jet RAA as a function of average Npart, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3, 0.4$, reconstructed in the range $80&lt; p_T &lt; 90$GeV/c and $|\eta|&lt;2$.
description: CERN-LHC. Inclusive jet spectra from pp and PbPb collisions at 2.76 TeV collected by the CMS experiment. Jets are reconstructed with three different distance parameters (R=0.2, 0.3, and 0.4) for transverse momentum pT&gt;70GeV/c and pseudorapidity |eta|&lt;2. The production cross sections and nuclear modification factor RAA is presented as function of pT and event centrality, for each R.
DOI: 10.17182/hepdata.77601.v1/t16
title: "Table 9b" of "Measurement of inclusive jet cross-sections in pp and PbPb collisions at sqrt(s[NN])=2.76 TeV"

description: Inclusive jet RAA as a function of average Npart, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3, 0.4$, reconstructed in the range $130&lt; p_T &lt; 150$GeV/c and $|\eta|&lt;2$.
description: CERN-LHC. Inclusive jet spectra from pp and PbPb collisions at 2.76 TeV collected by the CMS experiment. Jets are reconstructed with three different distance parameters (R=0.2, 0.3, and 0.4) for transverse momentum pT&gt;70GeV/c and pseudorapidity |eta|&lt;2. The production cross sections and nuclear modification factor RAA is presented as function of pT and event centrality, for each R.
DOI: 10.17182/hepdata.77601.v1/t17
title: "Table 10" of "Measurement of inclusive jet cross-sections in pp and PbPb collisions at sqrt(s[NN])=2.76 TeV"

description: Inclusive jet RAA as a function of jet $p_T$, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3$, reconstructed in the range $|\eta|&lt;2$, for 0-10\% PbPb centrality. The '5.7%' combined uncertainty on the pp luminosity and PbPb TAA is considered as global uncertainty (common to all points), and it is not included in the point-to-point uncertainties.
description: CERN-LHC. Inclusive jet spectra from pp and PbPb collisions at 2.76 TeV collected by the CMS experiment. Jets are reconstructed with three different distance parameters (R=0.2, 0.3, and 0.4) for transverse momentum pT&gt;70GeV/c and pseudorapidity |eta|&lt;2. The production cross sections and nuclear modification factor RAA is presented as function of pT and event centrality, for each R.
DOI: 10.17182/hepdata.77601.v1/t9
title: "Table 8a" of "Measurement of inclusive jet cross-sections in pp and PbPb collisions at sqrt(s[NN])=2.76 TeV"

description: Inclusive jet RAA as a function of jet $p_T$, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3, 0.4$, with $|\eta|&lt;2$, for 0-5\% PbPb centrality. The '5.5%' combined uncertainty on the pp luminosity and PbPb TAA is considered as global uncertainty (common to all points), and it is not included in the point-to-point uncertainties.
description: CERN-LHC. Inclusive jet spectra from pp and PbPb collisions at 2.76 TeV collected by the CMS experiment. Jets are reconstructed with three different distance parameters (R=0.2, 0.3, and 0.4) for transverse momentum pT&gt;70GeV/c and pseudorapidity |eta|&lt;2. The production cross sections and nuclear modification factor RAA is presented as function of pT and event centrality, for each R.
DOI: 10.17182/hepdata.77015.v2/t2
title: "Table 2" 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/$\psi$ $v_{2}$ 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/t3
title: "Table 3" 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/$\psi$ $v_{2}$ as a function of $p_{T}$.
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/t4
title: "Table 4" 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. 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/t5
title: "Table 5" 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 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/t6
title: "Table 6" 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 $p_{\rm T}$.
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/t7
title: "Table 7" 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 high $p_{\rm T}$, 6.5$
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.