Differential production cross sections of psi(2S) as a function of pT.

Differential production cross sections of psi(2S) as a function of rapidity.

integrated production cross section of psi(2S).

psi(2S) over J/psi ratio as a function of pt.

psi(2S) over J/psi ratio as a function of rapidity.

integrated psi(2S) over J/psi production cross section ratio.

Differential production cross sections of Upsilon(1S) as a function of pT.

Differential production cross sections of Upsilon(1S) as a function of rapidity.

integrated production cross section of Upsilon (1S).

integrated production cross section of Upsilon (2S).

integrated Upsilon(1S) over Upsilon(2s) production cross section ratio.

D$^{0}$-meson relative yields for the sum of particle and antiparticle in several multiplicity and PT intervals for pp collisions at $\sqrt{s}=7$ TeV as a function of the relative average multiplicity in the V0 detector, $N_{V0} \big/ \langle N_{V0} \rangle$. The yields reported here are not corrected by the trigger selection efficiency, they are normalised to the visible cross section.

Fraction of non-prompt JPSI measured for PT > 1.3 GeV/c, $f_{\rm B}$(%), and extrapolated down to PT > 0, $f_{\rm B}^{\rm extr}$(%) in the various multiplicity intervals. The first and second uncertainties correspond to the statistical and systematic uncertainties, respectively.

Prompt and non-prompt relative JPSI relative yields for PT > 0 in the in different multiplicity bins. The first and second uncertainties correspond to the statistical and systematic uncertainties respectively. The yields reported here are normalised to the inelastic cross section.

Prompt and non-prompt relative JPSI relative yields for PT > 0 in the in different multiplicity bins. The first and second uncertainties correspond to the statistical and systematic uncertainties respectively. The yields reported here are not corrected by the trigger selection efficiency, they are normalised to the visible cross section.

psi(2S) double-differential cross section times branching fraction and the corresponding scaling factors to obtain the cross sections for different polarization scenarios (azimuthal polarization parameter in the center of mass helicity frame lambda_theta^HX = +1, -1, +0.03) as a function of pT for |y| < 1.2.

Ratio of psi(2S) to J/psi differential cross section times branching fractions assuming unpolarized productions as a function of pT for |y| < 1.2.

Prompt J/$\psi$ $v_{2}$ as a function of rapidity.

Prompt J/$\psi$ $v_{2}$ as a function of $p_{T}$.

Prompt J/$\psi$ $v_{2}$ as a function of $p_{T}$.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of rapidity.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of rapidity.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of $p_{\rm T}$.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of $p_{\rm T}$.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of centrality at high $p_{\rm T}$, 6.5$<p_{\rm T}<$30 GeV/c, in three different $|y|$ regions.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of centrality at high $p_{\rm T}$, 6.5$<p_{\rm T}<$30 GeV/c, in three different $|y|$ regions.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of centrality, at forward rapidity, 1.6$<|y|<$2.4, for two different $p_{\rm T}$ regions.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of centrality, at forward rapidity, 1.6$<|y|<$2.4, for two different $p_{\rm T}$ regions.

Nonprompt J/$\psi$ $v_{2}$ as a function of $p_{\rm T}$.

Nonprompt J/$\psi$ $v_{2}$ as a function of $p_{\rm T}$.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of rapidity.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of rapidity.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of $p_{\rm T}$.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of $p_{\rm T}$.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.

95% CL intervals on the 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 pT, for the forward rapidity analysis bin.

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.

95% CL intervals on the 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.

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.

95% CL intervals on the 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.

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.

95% CL interval on the 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.

Differential cross section of J/psi mesons from b hadrons as a function of dimuon pT in pp and PbPb collisions. The PbPb cross sections are normalised by TAA for direct comparison. Global uncertainties arise from the integrated luminosity uncertainty in pp collisions, and the number of minimum bias events and TAA uncertainties for PbPb collisions.

Differential cross section of prompt J/psi mesons as a function of dimuon rapidty in pp and PbPb collisions. The PbPb cross sections are normalised by TAA for direct comparison. Global uncertainties arise from the integrated luminosity uncertainty in pp collisions, and the number of minimum bias events and TAA uncertainties for PbPb collisions.

Differential cross section of J/psi mesons from b hadrons as a function of dimuon rapidty in pp and PbPb collisions. The PbPb cross sections are normalised by TAA for direct comparison. Global uncertainties arise from the integrated luminosity uncertainty in pp collisions, and the number of minimum bias events and TAA uncertainties for PbPb collisions.

Nuclear modification factor of prompt J/psi mesons as a function of dimuon rapidity. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of collision centrality. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of dimuon pT. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of dimuon pT in the mid-rapidity interval. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of dimuon pT in the most forward rapidity interval. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of collision centrality in the mid- and most forward rapidity intervals. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of pT in three centrality bins. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of collision centrality in the most forward rapidity range at moderate and high pT. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of collision centrality in the mid-rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt psi(2S) mesons as a function of collision centrality in the mid-rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

95% CL intervals on the nuclear modification factor of prompt psi(2S) mesons as a function of collision centrality in the mid-rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt J/psi and psi(2S) mesons as a function of dimuon pT in the mid-rapidity range. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of collision centrality in the forward rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt psi(2S) mesons as a function of collision centrality in the forward rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

95% CL intervals on the nuclear modification factor of prompt psi(2S) mesons as a function of collision centrality in the forward rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of dimuon pT in the forward rapidity range. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt psi(2S) mesons as a function of dimuon pT in the forward rapidity range. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

95% CL intervals on the nuclear modification factor of prompt psi(2S) mesons as a function of dimuon pT in the forward rapidity range. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of dimuon rapidity. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of collision centrality. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of dimuon pT. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of dimuon pT in the mid-rapidity interval. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of dimuon pT in the most forward rapidity interval. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of collision centrality in the mid- and most forward rapidity intervals. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of pT in three centrality bins. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of collision centrality in the most forward rapidity range at moderate and high pT. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Differential cross-section for non-prompt chi_c2 production, measured in bins of J/psi pT, assuming unpolarised chi_c production. The measurements are not corrected for the branching fractions of the decays chi_c --> J/psi + gamma and J/psi --> mu+ mu-. The uncertainty envelope associated with the unknown chi_c spin alignment is also shown.

Differential cross-section for prompt chi_c1 production, measured in bins of chi_c1 pT, assuming unpolarised chi_c production. The measurements are not corrected for the branching fractions of the decays chi_c --> J/psi + gamma and J/psi --> mu+ mu-. The uncertainty envelope associated with the unknown chi_c spin alignment is also shown.

Differential cross-section for prompt chi_c2 production, measured in bins of chi_c2 pT, assuming unpolarised chi_c production. The measurements are not corrected for the branching fractions of the decays chi_c --> J/psi + gamma and J/psi --> mu+ mu-. The uncertainty envelope associated with the unknown chi_c spin alignment is also shown.

Differential cross-section for non-prompt chi_c1 production, measured in bins of chi_c1 pT, assuming unpolarised chi_c production. The measurements are not corrected for the branching fractions of the decays chi_c --> J/psi + gamma and J/psi --> mu+ mu-. The uncertainty envelope associated with the unknown chi_c spin alignment is also shown.

Differential cross-section for non-prompt chi_c2 production, measured in bins of chi_c2 pT, assuming unpolarised chi_c production. The measurements are not corrected for the branching fractions of the decays chi_c --> J/psi + gamma and J/psi --> mu+ mu-. The uncertainty envelope associated with the unknown chi_c spin alignment is also shown.

Fraction of prompt J/psi produced in feed-down from radiative chi_c decays as a function of J/psi pT, assuming unpolarised chi_c production. The uncertainty envelope associated with the unknown chi_c spin alignment is also shown. The spin-alignment envelope assumes that prompt J/psi are produced unpolarised and represents the maximum uncertainty due to the unknown chi_c spin alignment.

Production rate of prompt chi_c2 relative to prompt chi_c1, measured in bins of J/psi pT, assuming unpolarised chi_c production. The ratio is not corrected for the branching fractions of chi_c1 and chi_c2 into J/psi gamma. The uncertainty envelope associated with the unknown chi_c spin alignment is also shown.

Production rate of non-prompt chi_c2 relative to non-prompt chi_c1, measured in bins of J/psi pT, assuming unpolarised chi_c production. The ratio is not corrected for the branching fractions of chi_c1 and chi_c2 into J/psi gamma. The uncertainty envelope associated with the unknown chi_c spin alignment is also shown.

Fraction of chi_c1 produced in b-hadron decays as a function of chi_c1 pT, assuming unpolarised chi_c production. The uncertainty envelope associated with the unknown chi_c spin alignment is also shown.

Fraction of chi_c2 produced in b-hadron decays as a function of chi_c2 pT, assuming unpolarised chi_c production. The uncertainty envelope associated with the unknown chi_c spin alignment is also shown.

Lambda-Phi in the CS frame for the J/psi as a function of pT for 0.6 < |y| < 1.2.

Lambda-Theta-Phi in the CS frame for the J/psi as a function of pT for 0.0 < |y| < 0.6.

Lambda-Theta-Phi in the CS frame for the J/psi as a function of pT for 0.6 < |y| < 1.2.

Lambda-Tilde in the CS frame for the J/psi as a function of pT for 0.0 < |y| < 0.6.

Lambda-Tilde in the CS frame for the J/psi as a function of pT for 0.6 < |y| < 1.2.

Lambda-Theta in the HX frame for the J/psi as a function of pT for 0.0 < |y| < 0.6.

Lambda-Theta in the HX frame for the J/psi as a function of pT for 0.6 < |y| < 1.2.

Lambda-Phi in the HX frame for the J/psi as a function of pT for 0.0 < |y| < 0.6.

Lambda-Phi in the HX frame for the J/psi as a function of pT for 0.6 < |y| < 1.2.

Lambda-Theta-Phi in the HX frame for the J/psi as a function of pT for 0.0 < |y| < 0.6.

Lambda-Theta-Phi in the HX frame for the J/psi as a function of pT for 0.6 < |y| < 1.2.

Lambda-Tilde in the HX frame for the J/psi as a function of pT for 0.0 < |y| < 0.6.

Lambda-Tilde in the HX frame for the J/psi as a function of pT for 0.6 < |y| < 1.2.

Lambda-Theta in the PX frame for the J/psi as a function of pT for 0.0 < |y| < 0.6.

Lambda-Theta in the PX frame for the J/psi as a function of pT for 0.6 < |y| < 1.2.

Lambda-Phi in the PX frame for the J/psi as a function of pT for 0.0 < |y| < 0.6.

Lambda-Phi in the PX frame for the J/psi as a function of pT for 0.6 < |y| < 1.2.

Lambda-Theta-Phi in the PX frame for the J/psi as a function of pT for 0.0 < |y| < 0.6.

Lambda-Theta-Phi in the PX frame for the J/psi as a function of pT for 0.6 < |y| < 1.2.

Lambda-Tilde in the PX frame for the J/psi as a function of pT for 0.0 < |y| < 0.6.

Lambda-Tilde in the PX frame for the J/psi as a function of pT for 0.6 < |y| < 1.2.

Lambda-Theta in the CS frame for the psi(2S) as a function of pT for 0.0 < |y| < 0.6.

Lambda-Theta in the CS frame for the psi(2S) as a function of pT for 0.6 < |y| < 1.2.

Lambda-Theta in the CS frame for the psi(2S) as a function of pT for 1.2 < |y| < 1.5.

Lambda-Phi in the CS frame for the psi(2S) as a function of pT for 0.0 < |y| < 0.6.

Lambda-Phi in the CS frame for the psi(2S) as a function of pT for 0.6 < |y| < 1.2.

Lambda-Phi in the CS frame for the psi(2S) as a function of pT for 1.2 < |y| < 1.5.

Lambda-Theta-Phi in the CS frame for the psi(2S) as a function of pT for 0.0 < |y| < 0.6.

Lambda-Theta-Phi in the CS frame for the psi(2S) as a function of pT for 0.6 < |y| < 1.2.

Lambda-Theta-Phi in the CS frame for the psi(2S) as a function of pT for 1.2 < |y| < 1.5.

Lambda-Tilde in the CS frame for the psi(2S) as a function of pT for 0.0 < |y| < 0.6.

Lambda-Tilde in the CS frame for the psi(2S) as a function of pT for 0.6 < |y| < 1.2.

Lambda-Tilde in the CS frame for the psi(2S) as a function of pT for 1.2 < |y| < 1.5.

Lambda-Theta in the HX frame for the psi(2S) as a function of pT for 0.0 < |y| < 0.6.

Lambda-Theta in the HX frame for the psi(2S) as a function of pT for 0.6 < |y| < 1.2.

Lambda-Theta in the HX frame for the psi(2S) as a function of pT for 1.2 < |y| < 1.5.

Lambda-Phi in the HX frame for the psi(2S) as a function of pT for 0.0 < |y| < 0.6.

Lambda-Phi in the HX frame for the psi(2S) as a function of pT for 0.6 < |y| < 1.2.

Lambda-Phi in the HX frame for the psi(2S) as a function of pT for 1.2 < |y| < 1.5.

Lambda-Theta-Phi in the HX frame for the psi(2S) as a function of pT for 0.0 < |y| < 0.6.

Lambda-Theta-Phi in the HX frame for the psi(2S) as a function of pT for 0.6 < |y| < 1.2.

Lambda-Theta-Phi in the HX frame for the psi(2S) as a function of pT for 1.2 < |y| < 1.5.

Lambda-Tilde in the HX frame for the psi(2S) as a function of pT for 0.0 < |y| < 0.6.

Lambda-Tilde in the HX frame for the psi(2S) as a function of pT for 0.6 < |y| < 1.2.

Lambda-Tilde in the HX frame for the psi(2S) as a function of pT for 1.2 < |y| < 1.5.

Lambda-Theta in the PX frame for the psi(2S) as a function of pT for 0.0 < |y| < 0.6.

Lambda-Theta in the PX frame for the psi(2S) as a function of pT for 0.6 < |y| < 1.2.

Lambda-Theta in the PX frame for the psi(2S) as a function of pT for 1.2 < |y| < 1.5.

Lambda-Phi in the PX frame for the psi(2S) as a function of pT for 0.0 < |y| < 0.6.

Lambda-Phi in the PX frame for the psi(2S) as a function of pT for 0.6 < |y| < 1.2.

Lambda-Phi in the PX frame for the psi(2S) as a function of pT for 1.2 < |y| < 1.5.

Lambda-Theta-Phi in the PX frame for the psi(2S) as a function of pT for 0.0 < |y| < 0.6.

Lambda-Theta-Phi in the PX frame for the psi(2S) as a function of pT for 0.6 < |y| < 1.2.

Lambda-Theta-Phi in the PX frame for the psi(2S) as a function of pT for 1.2 < |y| < 1.5.

Lambda-Tilde in the PX frame for the psi(2S) as a function of pT for 0.0 < |y| < 0.6.

Lambda-Tilde in the PX frame for the psi(2S) as a function of pT for 0.6 < |y| < 1.2.

Lambda-Tilde in the PX frame for the psi(2S) as a function of pT for 1.2 < |y| < 1.5.

Differential inclusive cross J/PSI section for the |rapidity| range 1.6 to 2.4 for each prompt J/PSI polarization scenario considered.

Measured fractions of J/PSI mesons from B hadrons corrected for the prompt and non-prompt acceptances.

Measured fractions of J/PSI mesons from B hadrons corrected for the prompt and non-prompt acceptances.

Measured fractions of J/PSI mesons from B hadrons corrected for the prompt and non-prompt acceptances.

Differential prompt J/PSI cross section for the |rapidity| range 0 to 1.2 for each prompt J/PSI polarization scenario considered.

Differential prompt J/PSI cross section for the |rapidity| range 1.2 to 1.6 for each prompt J/PSI polarization scenario considered.

Differential prompt J/PSI cross section for the |rapidity| range 1.6 to 2.4 for each prompt J/PSI polarization scenario considered.

Differential non-prompt J/PSI cross section for the |rapidity| range 0 to 1.2.

Differential non-prompt J/PSI cross section for the |rapidity| range 1.2 to 1.6.

Differential non-prompt J/PSI cross section for the |rapidity| range 1.6 to 2.4.

The (unpolarised) acceptance corrected J/PSI cross section times branching ratio to MU+ MU- for (PROMPT) and NON-PROMPT) production in the |rapidity| bin 1.6-2.1.

The (unpolarised) acceptance corrected J/PSI cross section times branching ratio to MU+ MU- for (PROMPT) and NON-PROMPT) production in the |rapidity| bin 2.1-2.4.

The (unpolarised) acceptance corrected PSI(2S) cross section times branching ratio to MU+ MU- for (PROMPT) and NON-PROMPT production in the |rapidity| bin 0.0-1.2.

The (unpolarised) acceptance corrected PSI(2S) cross section times branching ratio to MU+ MU- for (PROMPT) and NON-PROMPT production in the |rapidity| bin 1.2-1.6.

The (unpolarised) acceptance corrected PSI(2S) cross section times branching ratio to MU+ MU- for (PROMPT) and NON-PROMPT production in the |rapidity| bin 1.6-2.4.

The uncorrected visible J/PSI cross section times branching ratio to MU+ MU- for PROMPT and NON-PROMPT production in the |rapidity| bin 0.0-0.9.

The uncorrected visible J/PSI cross section times branching ratio to MU+ MU- for PROMPT and NON-PROMPT production in the |rapidity| bin 0.9-1.2.

The uncorrected visible J/PSI cross section times branching ratio to MU+ MU- for PROMPT and NON-PROMPT production in the |rapidity| bin 1.2-1.6.

The uncorrected visible J/PSI cross section times branching ratio to MU+ MU- for PROMPT and NON-PROMPT production in the |rapidity| bin 1.6-2.1.

The uncorrected visible J/PSI cross section times branching ratio to MU+ MU- for PROMPT and NON-PROMPT production in the |rapidity| bin 2.1-2.4.

The uncorrected visible PSI(2S) cross section times branching ratio to MU+ MU- for PROMPT and NON-PROMPT production in the |rapidity| bin 0.0-1.2.

The uncorrected visible PSI(2S) cross section times branching ratio to MU+ MU- for PROMPT and NON-PROMPT production in the |rapidity| bin 1.2-1.6.

The uncorrected visible PSI(2S) cross section times branching ratio to MU+ MU- for PROMPT and NON-PROMPT production in the |rapidity| bin 1.6-2.4.

The ratio between the PSI(2S) and J/PSI cross sections times branching ratio to MU+ MU- for PROMPT and NON-PROMPT production in the |rapidity| bin 0.0-1.2.

The ratio between the PSI(2S) and J/PSI cross sections times branching ratio to MU+ MU- for PROMPT and NON-PROMPT production in the |rapidity| bin 1.2-1.6.

The ratio between the PSI(2S) and J/PSI cross sections times branching ratio to MU+ MU- for PROMPT and NON-PROMPT production in the |rapidity| bin 1.6-2.4.

The ratio between the PSI(2S) and J/PSI cross sections times branching ratio to MU+ MU- for PROMPT and NON-PROMPT production in the integrated |rapidity| bin 0.0-2.4.

The non-prompt fraction (FB) of J/PSI times branching ratio to MU+ MU- from B-HADRON decays in the |rapidity| bin 0.0-0.9.

The non-prompt fraction (FB) of J/PSI times branching ratio to MU+ MU- from B-HADRON decays in the |rapidity| bin 0.9-1.2.

The non-prompt fraction (FB) of J/PSI times branching ratio to MU+ MU- from B-HADRON decays in the |rapidity| bin 1.2-1.6.

The non-prompt fraction (FB) of J/PSI times branching ratio to MU+ MU- from B-HADRON decays in the |rapidity| bin 1.6-2.1.

The non-prompt fraction (FB) of J/PSI times branching ratio to MU+ MU- from B-HADRON decays in the |rapidity| bin 2.1-2.4.

The non-prompt fraction (FB) of PSI(2S) times branching ratio to MU+ MU- from B-HADRON decays in the |rapidity| bin 0.0-1.2.

The non-prompt fraction (FB) of PSI(2S) times branching ratio to MU+ MU- from B-HADRON decays in the |rapidity| bin 1.2-1.6.

The non-prompt fraction (FB) of PSI(2S) times branching ratio to MU+ MU- from B-HADRON decays in the |rapidity| bin 1.6-2.4.

The difference between the J/PSI cross section times branching ratio to MU+ MU- for non-prompt production calculated for four different polarization scenarios and the zero polarization values. The notation is (-1,CS), (+1,CS), (-1,HX), (+1,HX), where CS(HX) is the Collins-Soper (Helicity) frame and -1(+1) refer to full longitudinal (transverse) polarization.

The difference between the J/PSI cross section times branching ratio to MU+ MU- for non-prompt production calculated for four different polarization scenarios and the zero polarization values. The notation is (-1,CS), (+1,CS), (-1,HX), (+1,HX), where CS(HX) is the Collins-Soper (Helicity) frame and -1(+1) refer to full longitudinal (transverse) polarization.

The difference between the J/PSI cross section times branching ratio to MU+ MU- for non-prompt production calculated for four different polarization scenarios and the zero polarization values. The notation is (-1,CS), (+1,CS), (-1,HX), (+1,HX), where CS(HX) is the Collins-Soper (Helicity) frame and -1(+1) refer to full longitudinal (transverse) polarization.

The difference between the J/PSI cross section times branching ratio to MU+ MU- for non-prompt production calculated for four different polarization scenarios and the zero polarization values. The notation is (-1,CS), (+1,CS), (-1,HX), (+1,HX), where CS(HX) is the Collins-Soper (Helicity) frame and -1(+1) refer to full longitudinal (transverse) polarization.

The difference between the J/PSI cross section times branching ratio to MU+ MU- for non-prompt production calculated for four different polarization scenarios and the zero polarization values. The notation is (-1,CS), (+1,CS), (-1,HX), (+1,HX), where CS(HX) is the Collins-Soper (Helicity) frame and -1(+1) refer to full longitudinal (transverse) polarization.

The difference between the PSI(2S) cross section times branching ratio to MU+ MU- for non-prompt production calculated for four different polarization scenarios and the zero polarization values. The notation is (-1,CS), (+1,CS), (-1,HX), (+1,HX), where CS(HX) is the Collins-Soper (Helicity) frame and -1(+1) refer to full longitudinal (transverse) polarization.

The difference between the PSI(2S) cross section times branching ratio to MU+ MU- for non-prompt production calculated for four different polarization scenarios and the zero polarization values. The notation is (-1,CS), (+1,CS), (-1,HX), (+1,HX), where CS(HX) is the Collins-Soper (Helicity) frame and -1(+1) refer to full longitudinal (transverse) polarization.

The difference between the PSI(2S) cross section times branching ratio to MU+ MU- for non-prompt production calculated for four different polarization scenarios and the zero polarization values. The notation is (-1,CS), (+1,CS), (-1,HX), (+1,HX), where CS(HX) is the Collins-Soper (Helicity) frame and -1(+1) refer to full longitudinal (transverse) polarization.