Differential cross section times dimuon branching fraction of Y(1S) as a function of $y^{Y}_{CM}$ in pPb collisions. The global uncertainty arises from the integrated luminosity uncertainty in pPb collisions.

Differential cross section times dimuon branching fraction of Y(2S) as a function of $y^{Y}_{CM}$ in pPb collisions. The global uncertainty arises from the integrated luminosity uncertainty in pPb collisions.

Differential cross section times dimuon branching fraction of Y(3S) as a function of $y^{Y}_{CM}$ in pPb collisions. The global uncertainty arises from the integrated luminosity uncertainty in pPb collisions.

Differential cross section times dimuon branching fraction of Y(1S) as a function of pT in pp collisions. The global uncertainty arises from the integrated luminosity uncertainty in pp collisions.

Differential cross section times dimuon branching fraction of Y(2S) as a function of pT in pp collisions. The global uncertainty arises from the integrated luminosity uncertainty in pp collisions.

Differential cross section times dimuon branching fraction of Y(3S) as a function of pT in pp collisions. The global uncertainty arises from the integrated luminosity uncertainty in pp collisions.

Differential cross section times dimuon branching fraction of Y(1S) as a function of $|y^{Y}_{CM}|$ in pp collisions. The global uncertainty arises from the integrated luminosity uncertainty in pp collisions.

Differential cross section times dimuon branching fraction of Y(2S) as a function of $|y^{Y}_{CM}|$ in pp collisions. The global uncertainty arises from the integrated luminosity uncertainty in pp collisions.

Differential cross section times dimuon branching fraction of Y(3S) as a function of $|y^{Y}_{CM}|$ in pp collisions. The global uncertainty arises from the integrated luminosity uncertainty in pp collisions.

Nuclear modification factor of Y(1S) as a function of pT. The global uncertainty arises from the integrated luminosity uncertainties in pPb and pp collisions.

Nuclear modification factor of Y(2S) as a function of pT. The global uncertainty arises from the integrated luminosity uncertainties in pPb and pp collisions.

Nuclear modification factor of Y(3S) as a function of pT. The global uncertainty arises from the integrated luminosity uncertainties in pPb and pp collisions.

Nuclear modification factor of Y(1S) as a function of $y^{Y}_{CM}$. The global uncertainty arises from the integrated luminosity uncertainties in pPb and pp collisions.

Nuclear modification factor of Y(2S) as a function of $y^{Y}_{CM}$. The global uncertainty arises from the integrated luminosity uncertainties in pPb and pp collisions.

Nuclear modification factor of Y(3S) as a function of $y^{Y}_{CM}$. The global uncertainty arises from the integrated luminosity uncertainties in pPb and pp collisions.

Nuclear modification factor of Y(1S) at forward and backward $y^{Y}_{CM}$ for pT < 6 GeV/c. The global uncertainty arises from the integrated luminosity uncertainties in pPb and pp collisions.

Nuclear modification factor of Y(2S) at forward and backward $y^{Y}_{CM}$ for pT < 6 GeV/c. The global uncertainty arises from the integrated luminosity uncertainties in pPb and pp collisions.

Nuclear modification factor of Y(3S) at forward and backward $y^{Y}_{CM}$ for pT < 6 GeV/c. The global uncertainty arises from the integrated luminosity uncertainties in pPb and pp collisions.

Nuclear modification factor of Y(1S) at forward and backward $y^{Y}_{CM}$ for 6 < pT < 30 GeV/c. The global uncertainty arises from the integrated luminosity uncertainties in pPb and pp collisions.

Nuclear modification factor of Y(2S) at forward and backward $y^{Y}_{CM}$ for 6 < pT < 30 GeV/c. The global uncertainty arises from the integrated luminosity uncertainties in pPb and pp collisions.

Nuclear modification factor of Y(3S) at forward and backward $y^{Y}_{CM}$ for 6 < pT < 30 GeV/c. The global uncertainty arises from the integrated luminosity uncertainties in pPb and pp collisions.

RFB of Y(1S) versus $N^{|\eta_{lab}|<2.4}_{tracks}$.

RFB of Y(2S) versus $N^{|\eta_{lab}|<2.4}_{tracks}$.

RFB of Y(3S) versus $N^{|\eta_{lab}|<2.4}_{tracks}$.

RFB of Y(1S) versus $E^{|\eta_{lab}|>4}_{T}$.

RFB of Y(2S) versus $E^{|\eta_{lab}|>4}_{T}$.

RFB of Y(3S) versus $E^{|\eta_{lab}|>4}_{T}$.

Nuclear modification factor of Y(1S), Y(2S), and Y(3S) integrated over pT and $y^{Y}_{CM}$. The global uncertainty arises from the integrated luminosity uncertainties in pPb and pp collisions.

Rapidity dependence of $R_{\mathrm{pPb}}$ for prompt $\psi$(2S) mesons at $\sqrt(s_{\textrm{NN}})=5.02 $ TeV, in three $p_{\mathrm{T}}$ ranges. The fully correlated global uncertainty of 4.2% is not included in the point-by-point uncertainty.

Transverse momentum dependence of $R_{\mathrm{pPb}}$ for prompt $\psi$(2S) mesons at $\sqrt(s_{\textrm{NN}})=5.02 $ TeV, in seven $y_{\mathrm{CM}}$ ranges. The fully correlated global uncertainty of 4.2% is not incuded in the point-by-point uncertainty.

Differential cross section (multiplied by the dimuon branching fraction) of prompt J/$\psi$ mesons in pPb collisions at backward $y_{\mathrm{CM}}$.

Rapidity dependence of the cross section (multiplied by the dimuon branching fraction) for prompt J/$\psi$ mesons in the $p_{\mathrm{T}}$ intervals 6.5<$p_{\mathrm{T}}$<10 GeV and 10<$p_{\mathrm{T}}$<30 GeV in pp collisions.

Rapidity dependence of the cross section (multiplied by the dimuon branching fraction) for prompt J/$\psi$ mesons in the $p_{\mathrm{T}}$ intervals 6.5<$p_{\mathrm{T}}$<10 GeV and 10<$p_{\mathrm{T}}$<30 GeV in pPb collisions.

Transverse momentum dependence of $R_{\mathrm{pPb}}$ for prompt J/$\psi$ mesons in seven $y_{\mathrm{CM}}$ ranges.

Rapidity dependence of $R_{\mathrm{pPb}}$ for prompt J/$\psi$ mesons in $p_{\mathrm{T}}$ range 6.5<$p_{\mathrm{T}}$<10 GeV.

Rapidity dependence of $R_{\mathrm{pPb}}$ for prompt J/$\psi$ mesons in $p_{\mathrm{T}}$ range 10<$p_{\mathrm{T}}$<30 GeV.

Transverse momentum dependence of $R_{\mathrm{FB}}$ for prompt J/$\psi$ mesons in the 0<$y_{\mathrm{CM}}$<0.9 range.

Transverse momentum dependence of $R_{\mathrm{FB}}$ for prompt J/$\psi$ mesons in the 0.9<$y_{\mathrm{CM}}$<1.5 range.

Transverse momentum dependence of $R_{\mathrm{FB}}$ for prompt J/$\psi$ mesons in the 1.5<$y_{\mathrm{CM}}$<1.93 range.

Dependence of $R_{\mathrm{FB}}$ for prompt J/$\psi$ mesons on the hadronic activity in the event, given by the transverse energy deposited in the CMS detector at large pseudorapidities $E_{\mathrm{T}}^{\mathrm{HF}|\eta|>4}$.

Differential cross section (multiplied by the dimuon branching fraction) of nonprompt J/$\psi$ mesons in pp collisions at forward $y_{\mathrm{CM}}$.

Differential cross section (multiplied by the dimuon branching fraction) of nonprompt J/$\psi$ mesons in pp collisions at backward $y_{\mathrm{CM}}$.

Differential cross section (multiplied by the dimuon branching fraction) of nonprompt J/$\psi$ mesons in pPb collisions at forward $y_{\mathrm{CM}}$.

Differential cross section (multiplied by the dimuon branching fraction) of nonprompt J/$\psi$ mesons in pPb collisions at backward $y_{\mathrm{CM}}$.

Rapidity dependence of the cross section (multiplied by the dimuon branching fraction) for nonprompt J/$\psi$ mesons in the $p_{\mathrm{T}}$ intervals 6.5<$p_{\mathrm{T}}$<10 GeV and 10<$p_{\mathrm{T}}$<30 GeV in pp collisions.

Rapidity dependence of the cross section (multiplied by the dimuon branching fraction) for nonprompt J/$\psi$ mesons in the $p_{\mathrm{T}}$ intervals 6.5<$p_{\mathrm{T}}$<10 GeV and 10<$p_{\mathrm{T}}$<30 GeV in pPb collisions.

Transverse momentum dependence of $R_{\mathrm{pPb}}$ for nonprompt J/$\psi$ mesons in seven $y_{\mathrm{CM}}$ ranges.

Rapidity dependence of $R_{\mathrm{pPb}}$ for nonprompt J/$\psi$ mesons in $p_{\mathrm{T}}$ range 6.5<$p_{\mathrm{T}}$<10 GeV.

Rapidity dependence of $R_{\mathrm{pPb}}$ for nonprompt J/$\psi$ mesons in $p_{\mathrm{T}}$ range 10<$p_{\mathrm{T}}$<30 GeV.

Transverse momentum dependence of $R_{\mathrm{FB}}$ for nonprompt J/$\psi$ mesons in the 0<$y_{\mathrm{CM}}$<0.9 range.

Transverse momentum dependence of $R_{\mathrm{FB}}$ for nonprompt J/$\psi$ mesons in the 0.9<$y_{\mathrm{CM}}$<1.5 range.

Transverse momentum dependence of $R_{\mathrm{FB}}$ for nonprompt J/$\psi$ mesons in the 1.5<$y_{\mathrm{CM}}$<1.93 range.

Dependence of $R_{\mathrm{FB}}$ for nonprompt J/$\psi$ mesons on the hadronic activity in the event, given by the transverse energy deposited in the CMS detector at large pseudorapidities $E_{\mathrm{T}}^{\mathrm{HF}|\eta|>4}$.