Measured DPS effective cross section

pp -> J/psi J/psi J/psi X cross section

$pp \rightarrow J/\psi J/\psi J/\psi X~$ fiducial cross section

$v_{2}$ of $\Upsilon(\mathrm{1S})$ as a function of $p_{\mathrm{T}}$ in three centrality ranges, 10-30%, 30-50% and 50-90%.

$v_{2}$ of $\Upsilon(\mathrm{1S})$ as a function of $p_{\mathrm{T}}$ in 5-60% centrality range.

Summary of the measured values of $ d\sigma / d{m}$ (pb/GeV) in the dielectron channel with the statistical ($\delta_{\text{stat}}$), experimental ($\delta_{\text{exp}}$) and theoretical ($\delta_{\text{theo}}$) uncertainties, respectively. Here, $\delta_{\text{tot}}$ is the quadratic sum of the three components.

Summary of the measured values of fiducial $ d\sigma / d{m}$ (pb/GeV) (with no FSR correction applied) in the dimuon channel with the statistical ($\delta_{\text{stat}}$) and experimental ($\delta_{\text{exp}}$) uncertainties shown separately. Here, $\delta_{\text{tot}}$ is the quadratic sum of the two components.

of the measured values of fiducial $ d\sigma / d{m}$ (pb/GeV) (with no FSR correction applied) in the dielectron channel with the statistical ($\delta_{\text{stat}}$) and experimental ($\delta_{\text{exp}}$) uncertainties shown separately. Here, $\delta_{\text{tot}}$ is the quadratic sum of the two components.

Summary of the combined values of $ d\sigma / d{m}$ (pb/GeV) using the results from both the dimuon and dielectron channels. Here, $\delta_{\text{tot}}$ is the quadratic sum of the statistical, experimental and theoretical uncertainties.

Covariance matrix of the Drell-Yan differential cross section as a function of the dimuon invariant mass, measured in the full phase space, with FSR correction is applied. Luminosity uncertainty is not included in the covariance.

Covariance matrix of the Drell-Yan differential cross section as a function of the dielectron invariant mass, measured in the full phase space, with FSR correction is applied. Luminosity uncertainty is not included in the covariance.

Covariance matrix of the differential DY cross section measured for the combination of the two channels in the full phase space.

Differential cross sections of the Y(2S) meson as a function of pT for pp collisions. The global uncertainty arises from the integrated luminosity uncertainty in pp collisions.

Differential cross sections of the Y(3S) meson as a function of pT for pp collisions. The global uncertainty arises from the integrated luminosity uncertainty in pp collisions.

Differential cross sections of the Y(3S) meson as a function of pT for pp collisions. The global uncertainty arises from the integrated luminosity uncertainty in pp collisions.

Differential cross sections of the Y(1S) meson as a function of pT for PbPb collisions. Global uncertainties arise from the number of minimum bias events and TAA uncertainties for PbPb collisions.

Differential cross sections of the Y(1S) meson as a function of pT for PbPb collisions. Global uncertainties arise from the number of minimum bias events and TAA uncertainties for PbPb collisions.

Differential cross sections of the Y(2S) meson as a function of pT for PbPb collisions. Global uncertainties arise from the number of minimum bias events and TAA uncertainties for PbPb collisions.

Differential cross sections of the Y(2S) meson as a function of pT for PbPb collisions. Global uncertainties arise from the number of minimum bias events and TAA uncertainties for PbPb collisions.

Differential cross sections of the Y(3S) meson as a function of pT for PbPb collisions.

Differential cross sections of the Y(3S) meson as a function of pT for PbPb collisions.

Differential cross sections of the Y(1S) meson as a function of rapidity for pp collisions. The global uncertainty arises from the integrated luminosity uncertainty in pp collisions.

Differential cross sections of the Y(1S) meson as a function of rapidity for pp collisions. The global uncertainty arises from the integrated luminosity uncertainty in pp collisions.

Differential cross sections of the Y(2S) meson as a function of rapidity for pp collisions. The global uncertainty arises from the integrated luminosity uncertainty in pp collisions.

Differential cross sections of the Y(2S) meson as a function of rapidity for pp collisions. The global uncertainty arises from the integrated luminosity uncertainty in pp collisions.

Differential cross sections of the Y(3S) meson as a function of rapidity for pp collisions. The global uncertainty arises from the integrated luminosity uncertainty in pp collisions.

Differential cross sections of the Y(3S) meson as a function of rapidity for pp collisions. The global uncertainty arises from the integrated luminosity uncertainty in pp collisions.

Differential cross sections of the Y(1S) meson as a function of pT for PbPb collisions. Global uncertainties arise from the number of minimum bias events and TAA uncertainties for PbPb collisions.

Differential cross sections of the Y(1S) meson as a function of pT for PbPb collisions. Global uncertainties arise from the number of minimum bias events and TAA uncertainties for PbPb collisions.

Differential cross sections of the Y(2S) meson as a function of pT for PbPb collisions. Global uncertainties arise from the number of minimum bias events and TAA uncertainties for PbPb collisions.

Differential cross sections of the Y(2S) meson as a function of pT for PbPb collisions. Global uncertainties arise from the number of minimum bias events and TAA uncertainties for PbPb collisions.

Differential cross sections of the Y(3S) meson as a function of pT for PbPb collisions.

Differential cross sections of the Y(3S) meson as a function of pT for PbPb collisions.

Nuclear modification factor of the Y(1S) meson as a function of pT. Global uncertainty combines the uncertainties from TAA, pp luminosity, and number of minimum bias events in PbPb collisions.

Nuclear modification factor of the Y(1S) meson as a function of pT. Global uncertainty combines the uncertainties from TAA, pp luminosity, and number of minimum bias events in PbPb collisions.

Nuclear modification factor of the Y(2S) meson as a function of pT. Global uncertainty combines the uncertainties from TAA, pp luminosity, and number of minimum bias events in PbPb collisions.

Nuclear modification factor of the Y(2S) meson as a function of pT. Global uncertainty combines the uncertainties from TAA, pp luminosity, and number of minimum bias events in PbPb collisions.

Nuclear modification factor of the Y(3S) meson as a function of pT.

Nuclear modification factor of the Y(3S) meson as a function of pT.

Nuclear modification factor of the Y(1S) meson as a function of rapidity. Global uncertainty combines the uncertainties from TAA, pp luminosity, and number of minimum bias events in PbPb collisions.

Nuclear modification factor of the Y(1S) meson as a function of rapidity. Global uncertainty combines the uncertainties from TAA, pp luminosity, and number of minimum bias events in PbPb collisions.

Nuclear modification factor of the Y(2S) meson as a function of rapidity. Global uncertainty combines the uncertainties from TAA, pp luminosity, and number of minimum bias events in PbPb collisions.

Nuclear modification factor of the Y(2S) meson as a function of rapidity. Global uncertainty combines the uncertainties from TAA, pp luminosity, and number of minimum bias events in PbPb collisions.

Nuclear modification factor of the Y(3S) meson as a function of rapidity.

Nuclear modification factor of the Y(3S) meson as a function of rapidity.

Nuclear modification factor of the Y(1S) meson as a function of collision centrality. Global uncertainty combines the pp luminosity and number of minimum bias events in PbPb collisions. The PP Y(1S) global uncertainty consists of the statistical and systematic uncertainties of pp yield for Y(1S) state.

Nuclear modification factor of the Y(1S) meson as a function of collision centrality. Global uncertainty combines the pp luminosity and number of minimum bias events in PbPb collisions. The PP Y(1S) global uncertainty consists of the statistical and systematic uncertainties of pp yield for Y(1S) state.

Nuclear modification factor of the Y(2S) meson as a function of collision centrality. Global uncertainty combines the pp luminosity and number of minimum bias events in PbPb collisions. The PP Y(2S) global uncertainty consists of the statistical and systematic uncertainties of pp yield for Y(2S) state.

Nuclear modification factor of the Y(2S) meson as a function of collision centrality. Global uncertainty combines the pp luminosity and number of minimum bias events in PbPb collisions. The PP Y(2S) global uncertainty consists of the statistical and systematic uncertainties of pp yield for Y(2S) state.

Confidence intervals on the nuclear modification factors of the Y(3S) mesons as a function of collision centrality.

Confidence intervals on the nuclear modification factors of the Y(3S) mesons as a function of collision centrality.

Confidence intervals on the nuclear modification factors of the Y(2S) mesons as a function of collision centrality.

Confidence intervals on the nuclear modification factors of the Y(2S) mesons as a function of collision centrality.

Nuclear modification factors of the Y(1S) and Y(2S) mesons in the integrated pT, rapidity and centrality.

Nuclear modification factors of the Y(1S) and Y(2S) mesons in the integrated pT, rapidity and centrality.

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.

Double-differential cross section times the dimuon branching fraction of the Y(2S) meson for different ranges of pT in bins of |y| and for the full |y| < 1.2 range, for the unpolarized decay hypothesis. The global uncertainty in the integrated luminosity of 2.3% is not included in the systematic uncertainties.

Double-differential cross section times the dimuon branching fraction of the Y(3S) meson for different ranges of pT in bins of |y| and for the full |y| < 1.2 range, for the unpolarized decay hypothesis. The global uncertainty in the integrated luminosity of 2.3% is not included in the systematic uncertainties.

Multiplicative scaling factors to obtain the J/psi differential cross sections for different polarization scenarios (Lambda_{Theta} = +1, +0.10, -1) from the unpolarized cross section measurements given in Table 1.

Multiplicative scaling factors to obtain the psi(2S) differential cross sections for different polarization scenarios (Lambda_{Theta} = +1, +0.03, -1) from the unpolarized cross section measurements given in Table 2.

Multiplicative scaling factors to obtain the Y(1S) differential cross sections for different polarization scenarios (Lambda_{Theta} = +1, k, -1) from the unpolarized cross section measurements given in Table 3. The parameter k corresponds to a linear interpolation of the CMS measured value as a function of pT for pT < 50 GeV. For pT > 50 GeV, where no measurements exist, k is taken as the average of all the measured values for pT < 50 GeV.

Multiplicative scaling factors to obtain the Y(2S) differential cross sections for different polarization scenarios (Lambda_{Theta} = +1, k, -1) from the unpolarized cross section measurements given in Table 3. The parameter k corresponds to a linear interpolation of the CMS measured value as a function of pT for pT < 50 GeV. For pT > 50 GeV, where no measurements exist, k is taken as the average of all the measured values for pT < 50 GeV.

Multiplicative scaling factors to obtain the Y(3S) differential cross sections for different polarization scenarios (Lambda_{Theta} = +1, k, -1) from the unpolarized cross section measurements given in Table 3. The parameter k corresponds to a linear interpolation of the CMS measured value as a function of pT for pT < 50 GeV. For pT > 50 GeV, where no measurements exist, k is taken as the average of all the measured values for pT < 50 GeV.

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

Ratios of differential cross section times branching fractions of the prompt Y(2S) to Y(1S) and Y(3S) to Y(1S) mesons assuming unpolarized productions as a function of pT for |y| < 1.2.

Differential cross section for Y(2S) states as a function of their transverse momentum and per unit of rapidity in pp collisions. Statistical (systematic) uncertainties are displayed as error bars (boxes). Global relative uncertainties of 3.7% are not displayed.

Differential cross section for Y(3S) states as a function of their transverse momentum and per unit of rapidity in pp collisions. Statistical (systematic) uncertainties are displayed as error bars (boxes). Global relative uncertainties of 3.7% are not displayed.

Differential cross section for Y(3S) states as a function of their transverse momentum and per unit of rapidity in pp collisions. Statistical (systematic) uncertainties are displayed as error bars (boxes). Global relative uncertainties of 3.7% are not displayed.

Differential cross section for Y(1S) states as a function of their transverse momentum and per unit of rapidity in PbPb collisions. Statistical (systematic) uncertainties are displayed as error bars (boxes). Global relative uncertainties of 6.5% are not displayed.

Differential cross section for Y(1S) states as a function of their transverse momentum and per unit of rapidity in PbPb collisions. Statistical (systematic) uncertainties are displayed as error bars (boxes). Global relative uncertainties of 6.5% are not displayed.

Differential cross section for Y(2S) states as a function of their transverse momentum and per unit of rapidity in PbPb collisions. Statistical (systematic) uncertainties are displayed as error bars (boxes). Global relative uncertainties of 6.5% are not displayed.

Differential cross section for Y(2S) states as a function of their transverse momentum and per unit of rapidity in PbPb collisions. Statistical (systematic) uncertainties are displayed as error bars (boxes). Global relative uncertainties of 6.5% are not displayed.

Differential cross section for Y(1S) states as a function of their rapidity and integrated over transverse momentum in pp collisions. Statistical (systematic) uncertainties are displayed as error bars (boxes). Global relative uncertainties of 3.7% are not displayed.

Differential cross section for Y(1S) states as a function of their rapidity and integrated over transverse momentum in pp collisions. Statistical (systematic) uncertainties are displayed as error bars (boxes). Global relative uncertainties of 3.7% are not displayed.

Differential cross section for Y(2S) states as a function of their rapidity and integrated over transverse momentum in pp collisions. Statistical (systematic) uncertainties are displayed as error bars (boxes). Global relative uncertainties of 3.7% are not displayed.

Differential cross section for Y(2S) states as a function of their rapidity and integrated over transverse momentum in pp collisions. Statistical (systematic) uncertainties are displayed as error bars (boxes). Global relative uncertainties of 3.7% are not displayed.

Differential cross section for Y(3S) states as a function of their rapidity and integrated over transverse momentum in pp collisions. Statistical (systematic) uncertainties are displayed as error bars (boxes). Global relative uncertainties of 3.7% are not displayed.

Differential cross section for Y(3S) states as a function of their rapidity and integrated over transverse momentum in pp collisions. Statistical (systematic) uncertainties are displayed as error bars (boxes). Global relative uncertainties of 3.7% are not displayed.

Differential cross section for Y(1S) states as a function of their rapidity and integrated over transverse momentum in PbPb collisions. Statistical (systematic) uncertainties are displayed as error bars (boxes). Global relative uncertainties of 6.5% are not displayed.

Differential cross section for Y(1S) states as a function of their rapidity and integrated over transverse momentum in PbPb collisions. Statistical (systematic) uncertainties are displayed as error bars (boxes). Global relative uncertainties of 6.5% are not displayed.

Differential cross section for Y(2S) states as a function of their rapidity and integrated over transverse momentum in PbPb collisions. Statistical (systematic) uncertainties are displayed as error bars (boxes). Global relative uncertainties of 6.5% are not displayed.

Differential cross section for Y(2S) states as a function of their rapidity and integrated over transverse momentum in PbPb collisions. Statistical (systematic) uncertainties are displayed as error bars (boxes). Global relative uncertainties of 6.5% are not displayed.

Nuclear modification factor for Υ(1S) states in PbPb collisions as a function of pT. Statistical (systematic) uncertainties are displayed as error bars (boxes), while the global (fully correlated) uncertainty (7.5%) is displayed as a grey box at unity.

Nuclear modification factor for Υ(1S) states in PbPb collisions as a function of pT. Statistical (systematic) uncertainties are displayed as error bars (boxes), while the global (fully correlated) uncertainty (7.5%) is displayed as a grey box at unity.

Nuclear modification factor for Υ(2S) states in PbPb collisions as a function of pT. Statistical (systematic) uncertainties are displayed as error bars (boxes), while the global (fully correlated) uncertainty (7.5%) is displayed as a grey box at unity.

Nuclear modification factor for Υ(2S) states in PbPb collisions as a function of pT. Statistical (systematic) uncertainties are displayed as error bars (boxes), while the global (fully correlated) uncertainty (7.5%) is displayed as a grey box at unity.

Nuclear modification factor for Υ(1S) states in PbPb collisions as a function of |y|. Statistical (systematic) uncertainties are displayed as error bars (boxes), while the global (fully correlated) uncertainty (7.5%) is displayed as a grey box at unity.

Nuclear modification factor for Υ(1S) states in PbPb collisions as a function of |y|. Statistical (systematic) uncertainties are displayed as error bars (boxes), while the global (fully correlated) uncertainty (7.5%) is displayed as a grey box at unity.

Nuclear modification factor for Υ(2S) states in PbPb collisions as a function of |y|. Statistical (systematic) uncertainties are displayed as error bars (boxes), while the global (fully correlated) uncertainty (7.5%) is displayed as a grey box at unity.

Nuclear modification factor for Υ(2S) states in PbPb collisions as a function of |y|. Statistical (systematic) uncertainties are displayed as error bars (boxes), while the global (fully correlated) uncertainty (7.5%) is displayed as a grey box at unity.

Nuclear modification factors for Υ(1S) meson production in PbPb collisions, as a function of centrality, displayed as the average number of participating nucleons. Statistical (systematic) uncertainties are displayed as error bars (boxes), while the global (fully correlated) uncertainties from the PbPb data (3.2%) or from the pp reference (6.3%) are displayed at unity as empty and filled red black boxes, respectively.

Nuclear modification factors for Υ(1S) meson production in PbPb collisions, as a function of centrality, displayed as the average number of participating nucleons. Statistical (systematic) uncertainties are displayed as error bars (boxes), while the global (fully correlated) uncertainties from the PbPb data (3.2%) or from the pp reference (6.3%) are displayed at unity as empty and filled red black boxes, respectively.

Nuclear modification factors for Υ(2S) meson production in PbPb collisions, as a function of centrality, displayed as the average number of participating nucleons. Statistical (systematic) uncertainties are displayed as error bars (boxes), while the global (fully correlated) uncertainties from the PbPb data (3.2%) or from the pp reference (6.9%) are displayed at unity as empty and filled black black boxes, respectively.

Nuclear modification factors for Υ(2S) meson production in PbPb collisions, as a function of centrality, displayed as the average number of participating nucleons. Statistical (systematic) uncertainties are displayed as error bars (boxes), while the global (fully correlated) uncertainties from the PbPb data (3.2%) or from the pp reference (6.9%) are displayed at unity as empty and filled black black boxes, respectively.

Nuclear modification factors for Υ(1S), Υ(2S) and Υ(3S) meson production in PbPb collisions, integrated over centrality. For the Υ(3S), the upper limit derived on the nuclear modification factor is given.

Nuclear modification factors for Υ(1S), Υ(2S) and Υ(3S) meson production in PbPb collisions, integrated over centrality. For the Υ(3S), the upper limit derived on the nuclear modification factor is given.

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 production cross sections of $\psi$(2S) as a function of $p_{\rm T}$.

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

integrated production cross section of $\psi$(2S).

Differential production cross sections of $\Upsilon$(1S) as a function of $p_{\rm T}$.

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

integrated production cross section of $\Upsilon$(1S).

Differential production cross sections of $\Upsilon$(2S) as a function of rapidity.

integrated production cross section of Upsilon (2S).

integrated production cross section of Upsilon (3S).

$\psi$(2S) over J/$\psi$ ratio as a function of $p_{\rm T}$.

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

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

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

integrated $\Upsilon$(3S) over $\Upsilon$(1S) production cross section ratio.

pT-differential inclusive muon $v_{2}$ extracted with two-particle $Q$ cumulants method.

pT-differential inclusive muon $v_{2}$ extracted with scalar product method.

pT-differential inclusive muon $v_{2}$ extracted with two-particle cumulants method.

pT-differential inclusive muon $v_{2}$ extracted with four-particle cumulants method.

pT-differential inclusive muon $v_{2}$ extracted with Lee-Yang zeros (Sum) method.

pT-differential inclusive muon $v_{2}$ extracted with Lee-Yang zeros (Prod) method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with scalar product method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with two-particle $Q$ cumulants method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with scalar product method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with two-particle $Q$ cumulants method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with scalar product method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with two-particle cumulants method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with four-particle cumulants method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with Lee-Yang zeros (Sum) method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with Lee-Yang zeros (Prod) method.

Elliptic flow of muons from heavy-flavour hadron decays as a function of the collision centrality extracted with scalar product method.

Elliptic flow of muons from heavy-flavour hadron decays as a function of the collision centrality extracted with two-particle cumulants method.

Differential cross sections dsigma^cent_JPsi/dy for six centrality classes at forward (2.03<y_cms<3.53) and backward (-4.46<y_cms<-2.96) centre-of-mass rapidity. The first uncertainty is statistical, the second and third ones are the systematic uncertainties. The third uncertainty is fully correlated over centrality.

Nuclear modification factor Q_pA as function of centrality at forward (2.03<y_cms<3.53) and backward (-4.46<y_cms<-2.96) centre-of-mass rapidity. The first uncertainty is statistical, the second and third ones are the systematic uncertainties. The third uncertainty is fully correlated over centrality.

Nuclear modification factor Q_pA as function of centrality in the mid-rapidity range (-1.37 <y_cms< 0.43). The first uncertainty is statistical, the second and third one are the systematic uncertainties. The third uncertainty is fully correlated over centrality.

Values of <pT> and <pT^2> for six centrality classes at forward (2.03<y_cms<3.53) and backward (-4.46<y_cms<-2.96) centre-of-mass rapidity. The first uncertainty is statistical, the second one is the systematic uncertainty.

Values of <pT> and <pT^2> at forward (2.03<y_cms<3.53) and backward (2.96<y_cms<4.46) centre-of-mass rapidity in pp collisions calculated based on an interpolation procedure.

Values of Delta<pT^2> as a function of centrality at forward (2.03<y_cms<3.53) and backward (-4.46<y_cms<-2.96) centre-of-mass rapidity. The first uncertainty is statistical, the second and third ones are the systematic uncertainties. The third is related to the uncertainty on the <pT^2> in pp collisions and is correlated over centrality.

Nuclear modification factor Q_pA as function of pT for six centrality classes at backward (-4.46<y_cms<-2.96) centre-of-mass rapidity. The first uncertainty is statistical, the second one and the third ones are the systematic uncertainties. The third uncertainty is fully correlated over pT.

Nuclear modification factor Q_pA as a function of pT for six centrality classes at forward (2.03<y_cms<3.53) centre-of-mass rapidity. The first uncertainty is statistical, the second and the third ones are the systematic uncertainties. The third uncertainty is fully correlated over pT.

Covariance matrix of total experimental uncertainties (statistical and systematic uncertainties added in quadrature) of absolute double differential fiducial cross section. The bin index is PT_i + 10*y_j.

$p_{\rm T}$ dependence of the J/$\psi$ nuclear modification factor $R_{\rm pA}$ in the backward rapidity range (-4.46<$y_{\rm cms}$<-2.96). The first uncertainty is statistical, the second one is the $p_{\rm T}$-uncorrelated systematic uncertainty, the third is the partially $p_{\rm T}$-correlated, while the fourth is the $p_{\rm T}$-correlated one.

$p_{\rm T}$ dependence of the J/$\psi$ nuclear modification factor $R_{\rm pA}$ in the mid-rapidity range (-1.37<$y_{\rm cms}$<-0.43). The first uncertainty is statistical, the second one is the $p_{\rm T}$-uncorrelated systematic uncertainty, the third is the $p_{\rm T}$-correlated one.

$p_{\rm T}$ dependence of the J/$\psi$ nuclear modification factor $R_{\rm pA}$ in the forward rapidity range (2.03<$y_{\rm cms}$<3.53). The first uncertainty is statistical, the second one is the $p_{\rm T}$-uncorrelated systematic uncertainty, the third is the partially $p_{\rm T}$-correlated, while the fourth is the $p_{\rm T}$-correlated one.

Estimate of the $p_{\rm T}$-dependence of the Cold Nuclear Matter effects in Pb-Pb collisions calculated as $R^2_{\rm pPb}$. The first uncertainty is statistical, the second one is the $p_{\rm T}$-uncorrelated systematic uncertainty, the third is the $p_{\rm T}$-correlated one.

Estimate of the $p_{\rm T}$-dependence of the Cold Nuclear Matter effects in Pb-Pb collisions calculated as $R_{\rm pPb}$(-4.46 <y< -2.96) $\times$ $R_{\rm pPb}$(2.03 <y< 3.53). The first uncertainty is statistical, the second one is the $p_{\rm T}$-uncorrelated systematic uncertainty, the third is the partially $p_{\rm T}$-correlated, while the fourth is the $p_{\rm T}$ correlated one.

$p_{\rm T}$-dependence of the ratio between the $R_{\rm PbPb}$ and the cold nuclear matter effects evaluated as $R_{\rm pPb}$(-4.46 <y< -2.96) $\times$ $R_{\rm pPb}$(2.03 <y< 3.53). The first uncertainty is statistical, the second one is the quadratic combination of $p_{\rm T}$-uncorrelated and $p_{\rm T}$-partially correlated systematic uncertainties, while the third is the $p_{\rm T}$ correlated one.

Measured differential cross section dsigma/dET in pb/GeV given q_T < 10 GeV. For the data values, the first uncertainty is statistical and the second is systematic. For the theory values, the uncertainty combines statistical, PDF, and renormalization/factorization scale components.

Measured differential cross section dsigma/dET in pb/GeV given q_T > 50 GeV. For the data values, the first uncertainty is statistical and the second is systematic. For the theory values, the uncertainty combines statistical, PDF, and renormalization/factorization scale components.

Measured differential cross section dsigma/dDR in pb/radians. For the data values, the first uncertainty is statistical and the second is systematic. For the theory values, the uncertainty combines statistical, PDF, and renormalization/factorization scale components.

Measured differential cross section dsigma/dDR in pb/radians given q_T < 10 GeV. For the data values, the first uncertainty is statistical and the second is systematic. For the theory values, the uncertainty combines statistical, PDF, and renormalization/factorization scale components.

Measured differential cross section dsigma/dDR in pb/radians given q_T > 50 GeV. For the data values, the first uncertainty is statistical and the second is systematic. For the theory values, the uncertainty combines statistical, PDF, and renormalization/factorization scale components.

Fiducial cross sections for pT(gamma) > 15 GeV with statistical, systematic, and luminosity uncertainties, respectively. Combined result of electron and muon channels.

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.

The $p_{\rm T}$ bin width and corrected yield ratios R21 and R31 for $|y| < 0.6$. The statistical and systematic uncertainties in the corrected yield ratios are given as the percentage of the ratio.

The $p_{\rm T}$ bin width and corrected yield ratios R21 and R31 for $0.6 < |y| < 1.2$. The statistical and systematic uncertainties in the corrected yield ratios are given as the percentage of the ratio.

The $p_{\rm T}$ bin width and corrected yield ratios R21 and R31 for $|y| < 1.2$. The statistical and systematic uncertainties in the corrected yield ratios are given as the percentage of the ratio.

The dimuon acceptance $\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\mathcal{A}(\sigma^{\pm})$, and the values of the acceptance assuming no polarization $\mathcal{A}$(unpol), transverse polarization $\mathcal{A}(T)$, and longitudinal polarization $\mathcal{A}(L)$ for the $\Upsilon$(1S) state and $|y| <0.6$.

The dimuon acceptance $\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\mathcal{A}(\sigma^{\pm})$, and the values of the acceptance assuming no polarization $\mathcal{A}$(unpol), transverse polarization $\mathcal{A}(T)$, and longitudinal polarization $\mathcal{A}(L)$ for the $\Upsilon $(1S) state and $0.6 < |y| < 1.2$.

The dimuon acceptance $\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\mathcal{A}(\sigma^{\pm})$, and the values of the acceptance assuming no polarization $\mathcal{A}$(unpol), transverse polarization $\mathcal{A}(T)$, and longitudinal polarization $\mathcal{A}(L)$ for the $\Upsilon $(1S) state and $|y| < 1.2$.

The dimuon acceptance $\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\mathcal{A}(\sigma^{\pm})$, and the values of the acceptance assuming no polarization $\mathcal{A}$(unpol), transverse polarization $\mathcal{A}(T)$, and longitudinal polarization $\mathcal{A}(L)$ for the $\Upsilon $(2S) state and $|y| < 0.6$.

The dimuon acceptance $\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\mathcal{A}(\sigma^{\pm})$, and the values of the acceptance assuming no polarization $\mathcal{A}$(unpol), transverse polarization $\mathcal{A}(T)$, and longitudinal polarization $\mathcal{A}(L)$ for the $\Upsilon $(2S) state and $0.6 < |y| < 1.2$.

The dimuon acceptance $\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\mathcal{A}(\sigma^{\pm})$, and the values of the acceptance assuming no polarization $\mathcal{A}$(unpol), transverse polarization $\mathcal{A}(T)$, and longitudinal polarization $\mathcal{A}(L)$ for the $\Upsilon $(2S) state and $|y| < 1.2$.

The dimuon acceptance $\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\mathcal{A}(\sigma^{\pm})$, and the values of the acceptance assuming no polarization $\mathcal{A}$(unpol), transverse polarization $\mathcal{A}(T)$, and longitudinal polarization $\mathcal{A}(L)$ for the $\Upsilon $(3S) state and $|y| < 0.6$.

The dimuon acceptance $\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\mathcal{A}(\sigma^{\pm})$, and the values of the acceptance assuming no polarization $\mathcal{A}$(unpol), transverse polarization $\mathcal{A}(T)$, and longitudinal polarization $\mathcal{A}(L)$ for the $\Upsilon $(3S) state and $0.6 < |y| < 1.2$.

The dimuon acceptance $\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\mathcal{A}(\sigma^{\pm})$, and the values of the acceptance assuming no polarization $\mathcal{A}$(unpol), transverse polarization $\mathcal{A}(T)$, and longitudinal polarization $\mathcal{A}(L)$ for the $\Upsilon $(3S) state and $|y| < 1.2$.

The Drell-Yan pre-FSR dilepton rapidity distribution D(SIG)/DABS(YRAP) within the detector acceptance, for the mass bin 30-45 GeV, as measured in the combined dilepton channel.

The Drell-Yan pre-FSR dilepton rapidity distribution D(SIG)/DABS(YRAP) within the detector acceptance, for the mass bin 45-60 GeV, as measured in the combined dilepton channel.

The Drell-Yan pre-FSR dilepton rapidity distribution D(SIG)/DABS(YRAP) within the detector acceptance, for the mass bin 60-120 GeV, as measured in the combined dilepton channel.

The Drell-Yan pre-FSR dilepton rapidity distribution D(SIG)/DABS(YRAP) within the detector acceptance, for the mass bin 120-200 GeV, as measured in the combined dilepton channel.

The Drell-Yan pre-FSR dilepton rapidity distribution D(SIG)/DABS(YRAP) within the detector acceptance, for the mass bin 200-1500 GeV, as measured in the combined dilepton channel.

Measured ratio of the Drell-Yan normalized differential cross sections at center-of-mass energies of 7 and 8 TeV in the combined dilepton channel for the full phase space.

Measured ratio of the Drell-Yan normalized differential cross sections as a function of the absolute dilepton rapidity within the detector acceptance, at center-of-mass energies of 7 and 8 TeV in the combined dilepton channel. The mass bin 20-30 GeV.

Measured ratio of the Drell-Yan normalized differential cross sections as a function of the absolute dilepton rapidity within the detector acceptance, at center-of-mass energies of 7 and 8 TeV in the combined dilepton channel. The mass bin 30-45 GeV.

Measured ratio of the Drell-Yan normalized differential cross sections as a function of the absolute dilepton rapidity within the detector acceptance, at center-of-mass energies of 7 and 8 TeV in the combined dilepton channel. The mass bin 45-60 GeV.

Measured ratio of the Drell-Yan normalized differential cross sections as a function of the absolute dilepton rapidity within the detector acceptance, at center-of-mass energies of 7 and 8 TeV in the combined dilepton channel. The mass bin 60-120 GeV.

Measured ratio of the Drell-Yan normalized differential cross sections as a function of the absolute dilepton rapidity within the detector acceptance, at center-of-mass energies of 7 and 8 TeV in the combined dilepton channel. The mass bin 120-200 GeV.

Measured ratio of the Drell-Yan normalized differential cross sections as a function of the absolute dilepton rapidity within the detector acceptance, at center-of-mass energies of 7 and 8 TeV in the combined dilepton channel. The mass bin 200-1500 GeV.

The measured Z boson production cross section in pp collisions as a function of the Z boson rapidity for the dielectron decay channel.

Event centrality dependence of the $\mbox{Z}\rightarrow\mu^{+}\mu^{-}$ yields per MB event in PbPb collisions, divided by the expected average nuclear overlap function, $T_{\rm AA}$. On the horizontal axis, event centrality is depicted as the average number of participating nucleons, $N_{\rm part}$.

Event centrality dependence of the $\mbox{Z}\rightarrow e^{+}e^{-}$ yields per MB event in PbPb collisions, divided by the expected average nuclear overlap function, $T_{\rm AA}$. On the horizontal axis, event centrality is depicted as the average number of participating nucleons, $N_{\rm part}$.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson $p_{\rm T}$ for the dimuon decay channel.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson $p_{\rm T}$ for the dielectron decay channel.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson rapidity for the dimuon decay channel.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson rapidity for the dielectron decay channel.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson rapidity for the combined leptonic decay channel.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson $p_{\rm T}$ for the combined leptonic decay channel.

Event centrality dependence of the $\mbox{Z}\rightarrow l^{+}l^{-}$ yields per MB event in PbPb collisions, divided by the expected average nuclear overlap function, $T_{\rm AA}$. On the horizontal axis, event centrality is depicted as the average number of participating nucleons, $N_{\rm part}$.

The measured Z boson production cross section in pp collisions as a function of the Z boson rapidity for the combined leptonic decay channel.

The measured Z boson production cross section in pp collisions as a function of the Z boson pT for the combined leptonic decay channel in |y|<1.44.

Nuclear modification factor RAA of psi(2S) integrated over centrality, for the midrapidity and forward rapidity analysis bins.

Trans.min. scalar pT sum density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Away charged multiplicity density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 0 - 5 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 5 - 10 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 10 - 20 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 20 - 50 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 50 - 110 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 110 - 500 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 0 - 5 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 5 - 10 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 10 - 20 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 20 - 50 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 50 - 110 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 110 - 500 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 0 - 5 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 5 - 10 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 10 - 20 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 20 - 50 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 50 - 110 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 110 - 500 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 0 - 5 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 5 - 10 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 10 - 20 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 20 - 50 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 50 - 110 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 110 - 500 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 0 - 5 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 5 - 10 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 10 - 20 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 20 - 50 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 50 - 110 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 110 - 500 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 0 - 5 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 5 - 10 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 10 - 20 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 20 - 50 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 50 - 110 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 110 - 500 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards <mean pT(charged)> vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse <mean pT(charged)> vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Away <mean pT(charged)> vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Towards <mean pT(charged)> vs charged multiplicity, Born leptons : Statistical and systematic errors are added in quadrature.

Transverse <mean pT(charged)> vs charged multiplicity, Born leptons : Statistical and systematic errors are added in quadrature.

Away <mean pT(charged)> vs charged multiplicity, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 0 - 5 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 5 - 10 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 10 - 20 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 20 - 50 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 50 - 110 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 110 - 500 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.diff. scalar pT sum density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.diff. charged multiplicity density vs Z-boson pT, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 0 - 5 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 5 - 10 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 10 - 20 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 20 - 50 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 50 - 110 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 110 - 500 GeV, Born leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Away scalar pT sum density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Away charged multiplicity density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 0 - 5 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 5 - 10 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 10 - 20 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 20 - 50 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 50 - 110 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards scalar pT sum distribution, Z-boson pT = 110 - 500 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 0 - 5 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 5 - 10 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 10 - 20 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 20 - 50 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 50 - 110 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards charged multiplicity distribution, Z-boson pT = 110 - 500 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 0 - 5 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 5 - 10 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 10 - 20 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 20 - 50 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 50 - 110 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse charged multiplicity distribution, Z-boson pT = 110 - 500 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 0 - 5 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 5 - 10 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 10 - 20 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 20 - 50 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 50 - 110 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. charged multiplicity distribution, Z-boson pT = 110 - 500 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 0 - 5 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 5 - 10 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 10 - 20 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 20 - 50 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 50 - 110 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. charged multiplicity distribution, Z-boson pT = 110 - 500 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 0 - 5 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 5 - 10 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 10 - 20 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 20 - 50 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 50 - 110 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse scalar pT sum distribution, Z-boson pT = 110 - 500 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards <mean pT(charged)> vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse <mean pT(charged)> vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Away <mean pT(charged)> vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Towards <mean pT(charged)> vs charged multiplicity, dressed leptons : Statistical and systematic errors are added in quadrature.

Transverse <mean pT(charged)> vs charged multiplicity, dressed leptons : Statistical and systematic errors are added in quadrature.

Away <mean pT(charged)> vs charged multiplicity, dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 0 - 5 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 5 - 10 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 10 - 20 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 20 - 50 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 50 - 110 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.min. scalar pT sum distribution, Z-boson pT = 110 - 500 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.diff. scalar pT sum density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.diff. charged multiplicity density vs Z-boson pT, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 0 - 5 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 5 - 10 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 10 - 20 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 20 - 50 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 50 - 110 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Trans.max. scalar pT sum distribution, Z-boson pT = 110 - 500 GeV, Dressed leptons : Statistical and systematic errors are added in quadrature.

Prompt and non-prompt production cross-section times branching ratio as a function of $\psi(2\mathrm{S})$ $p_{\rm T}$ for $\psi(2\mathrm{S})$ rapidity interval of $0\leq |y| < 0.75$. The first uncertainty is statistical, the second is systematic. Spin-alignment and luminosity ($\pm 1.8\%$) uncertainties are not included.

Prompt and non-prompt production cross-section times branching ratio as a function of $\psi(2\mathrm{S})$ $p_{\rm T}$ for $\psi(2\mathrm{S})$ rapidity interval of $0.75\leq |y| < 1.5$. The first uncertainty is statistical, the second is systematic. Spin-alignment and luminosity ($\pm 1.8\%$) uncertainties are not included.

Prompt and non-prompt production cross-section times branching ratio as a function of $\psi(2\mathrm{S})$ $p_{\rm T}$ for $\psi(2\mathrm{S})$ rapidity interval of $1.5\leq |y| < 2$. The first uncertainty is statistical, the second is systematic. Spin-alignment and luminosity ($\pm 1.8\%$) uncertainties are not included.

Prompt and non-prompt production cross-section times branching ratio as a function of $J/\psi$ $p_{\rm T}$ for $J/\psi$ rapidity interval of $0\leq |y| < 0.75$. The first uncertainty is statistical, the second is systematic. Spin-alignment and luminosity ($\pm 1.8\%$) uncertainties are not included.

Prompt and non-prompt production cross-section times branching ratio as a function of $J/\psi$ $p_{\rm T}$ for $J/\psi$ rapidity interval of $0.75\leq |y| < 1.5$. The first uncertainty is statistical, the second is systematic. Spin-alignment and luminosity ($\pm 1.8\%$) uncertainties are not included.

Prompt and non-prompt production cross-section times branching ratio as a function of $J/\psi$ $p_{\rm T}$ for $J/\psi$ rapidity interval of $1.5\leq |y| < 2$. The first uncertainty is statistical, the second is systematic. Spin-alignment and luminosity ($\pm 1.8\%$) uncertainties are not included.

Reconstructed $\cos\theta^*$ distributions for data and the SM background estimate in the dimuon channel.

Reconstructed $A_{\rm FB}$ distributions for data and the SM background estimate as a function of dielectron mass.

Reconstructed $A_{\rm FB}$ distributions for data and the SM background estimate as a function of dimuon mass.

Summary of 95% C.L. lower exclusion limits on $\Lambda$ for the combined dilepton contact interaction search, using a uniform positive prior in 1/$\Lambda^2$.

Summary of 95% C.L. lower exclusion limits on $M_{\rm S}$ for the combined dilepton ADD large extra dimensions search, using a uniform positive prior in 1/$M_{\rm S}^8$.

Reconstructed $\cos\theta^*$ distributions for data and the SM background estimate in the electron channel.

Reconstructed $\cos\theta^*$ distributions for data and the SM background estimate in the muon channel.

Distribution of HT after the MTtau requirement for the 1-tau ''Tight'' SR. The SM prediction includes the data-driven corrections discussed in the paper. MC events are normalized to data in the CRs corresponding to MTtau below 130 GeV. Also shown is the expected signal from typical mSUGRA, GMSB and bRPV samples. The last bin in the expected background distribution is an overflow bin.

Distribution of MTtau1 + MTtau2 in the 2tau channel after all analysis requirements but the final SR requirements on MTtau1 + MTtau2 and HT2j. To reduce the contributions from events with Z bosons decaying into tau leptons, the requirement MTtau1 + MTtau2 > 150 GeV is applied to all distributions. The SM prediction includes the data-driven corrections discussed in the paper. MC events are normalized to data in the CRs corresponding to HT2j below 550 GeV.

Distribution of HT2j in the 2tau channel after all analysis requirements but the final SR requirements on MTtau1 + MTtau2 and HT2j. To reduce the contributions from events with Z bosons decaying into tau leptons, the requirement MTtau1 + MTtau2 > 150 GeV is applied to all distributions. The SM prediction includes the data-driven corrections discussed in the paper. MC events are normalized to data in the CRs corresponding to HT2j below 550 GeV.

Distribution of the jet multiplicity in the 2tau channel after all analysis requirements but the final SR requirements on MTtau1 + MTtau2 and HT2j. To reduce the contributions from events with Z bosons decaying into tau leptons, the requirement MTtau1 + MTtau2 > 150 GeV is applied to all distributions. The SM prediction includes the data-driven corrections discussed in the paper. MC events are normalized to data in the CRs corresponding to HT2j below 550 GeV.

Distribution of the final kinematic variables in the tau+e channel after all analysis requirements but the final SR selections on Meff for the bRPV model. The SM prediction includes the data-driven corrections discussed in the paper. MC events are normalized to data in specific CRs. The last bin in the expected background distribution is an overflow bin. There are no data events in the overflow bin after all analysis requirements are applied.

Distribution of the final kinematic variables in the tau+e channel after all analysis requirements but the final SR selections on MEFF for the GMSB model. The SM prediction includes the data-driven corrections discussed in the paper. MC events are normalized to data in specific CRs. The last bin in the expected background distribution is an overflow bin. There are no data events in the overflow bin after all analysis requirements are applied.

Distribution of the final kinematic variables in the tau+e channel after all analysis requirements but the final SR selections on MET for the mSUGRA model. The SM prediction includes the data-driven corrections discussed in the paper. MC events are normalized to data in specific CRs. The last bin in the expected background distribution is an overflow bin. There are no data events in the overflow bin after all analysis requirements are applied.

Distribution of the final kinematic variables in the tau+e channel after all analysis requirements but the final SR selections on MET for the nGM model. The SM prediction includes the data-driven corrections discussed in the paper. MC events are normalized to data in specific CRs. The last bin in the expected background distribution is an overflow bin. There are no data events in the overflow bin after all analysis requirements are applied.

Distribution of the final kinematic variables in the tau+mu channel after all analysis requirements but the final SR selections on MEFF for the bRPV model. The SM prediction includes the data-driven corrections discussed in the paper. MC events are normalized to data in specific CRs. The last bin in the expected background distribution is an overflow bin. There are no data events in the overflow bin after all analysis requirements are applied.

Distribution of the final kinematic variables in the tau+mu channel after all analysis requirements but the final SR selections on MEFF for the GMSB model. The SM prediction includes the data-driven corrections discussed in the paper. MC events are normalized to data in specific CRs. The last bin in the expected background distribution is an overflow bin. There are no data events in the overflow bin after all analysis requirements are applied.

Distribution of the final kinematic variables in the tau+mu channel after all analysis requirements but the final SR selections on MET for the mSUGRA model. The SM prediction includes the data-driven corrections discussed in the paper. MC events are normalized to data in specific CRs. The last bin in the expected background distribution is an overflow bin. There are no data events in the overflow bin after all analysis requirements are applied.

Distribution of the final kinematic variables in the tau+mu channel after all analysis requirements but the final SR selections on MET for the nGM model. The SM prediction includes the data-driven corrections discussed in the paper. MC events are normalized to data in specific CRs. The last bin in the expected background distribution is an overflow bin. There are no data events in the overflow bin after all analysis requirements are applied.

Observed 95% CL lower limits on the minimal GMSB model parameters Lambda and tan(beta) using a combination of all channels. The result is obtained using 20.3 fb-1 of sqrt(s) = 8 TeV ATLAS data. Additional model parameters are M(mess) = 250 TeV, N5 = 3, mu>0 and Cgrav =1.

Expected 95% CL lower limits on the minimal GMSB model parameters Lambda and tan(beta) using a combination of all channels. The result is obtained using 20.3 fb-1 of sqrt(s) = 8 TeV ATLAS data. Additional model parameters are M(mess) = 250 TeV, N5 = 3, mu>0 and Cgrav =1.

Observed 95% CL lower limits on the mSUGRA/CMSSM model parameters m0 and m1/2 for the combination of the 1tau, tau+e and tau+mu channels. Additional model parameters are A0 = -2m0, tan(beta) = 30 and sign(mu) = +1.

Expected 95% CL lower limits on the mSUGRA/CMSSM model parameters m0 and m1/2 for the combination of the 1tau, tau+e and tau+mu channels. Additional model parameters are A0 = -2m0, tan(beta) = 30 and sign(mu) = +1.

Observed 95% CL lower limits on the simplified nGM model parameters m(stau) and m(gluino) for the combination of the 2tau, tau+e and tau+mu channels. Additional squark and slepton mass parameters are set to 2.5 TeV, M1 = M2 = 2.5 TeV, and all trilinear coupling terms are set to zero. Also, the parameter mu is fixed to mu = 400 GeV.

Expected 95% CL lower limits on the simplified nGM model parameters m(stau) and m(gluino) for the combination of the 2tau, tau+e and tau+mu channels. Additional squark and slepton mass parameters are set to 2.5 TeV, M1 = M2 = 2.5 TeV, and all trilinear coupling terms are set to zero. Also, the parameter mu is fixed to mu = 400 GeV.

Observed 95% CL lower limits on the bRPV model parameters m0 and m1/2 for the combination of all channels. Additional model parameters are A0 = -2m0 , tan(beta) = 30 and sign(mu) = +1.

Expected 95% CL lower limits on the bRPV model parameters m0 and m1/2 for the combination of all channels. Additional model parameters are A0 = -2m0 , tan(beta) = 30 and sign(mu) = +1.

Cross section predictions for the nGM grid. For each signal point 25000 MC events have been generated.

Observed upper cross section limits for the nGM grid. For each signal point 25000 MC events have been generated. The limit is derived for the combination of the 2tau and the tau+lepton channels.

Systematic uncertainty for the GMSB grid in the 1-tau analysis.

Acceptance for the GMSB grid in the 1-tau analysis.

Efficiency for the GMSB grid in the 1-tau analysis.

The product of acceptance and efficiency for the GMSB grid in the 1-tau analysis.

Expected CLs values for the GMSB grid in the 1tau analysis.

Observed CLs values for the GMSB grid in the 1tau analysis.

Systematic uncertainty for the mSUGRA grid in the 1-tau analysis.

Acceptance for the mSUGRA grid in the 1-tau analysis.

Efficiency for the mSUGRA grid in the 1-tau analysis.

Product of acceptance and efficiency for the mSUGRA grid in the 1-tau analysis.

Expected CLs values for the mSUGRA grid in the 1tau analysis.

Observed CLs values for the mSUGRA grid in the 1tau analysis.

Systematic uncertainty for the bRPV grid in the 1-tau analysis.

Acceptance for the bRPV grid in the 1-tau analysis.

Efficiency for the bRPV grid in the 1-tau analysis.

Product of acceptance and efficiency for the bRPV grid in the 1-tau analysis.

Expected CLs values for the bRPV grid in the 1tau analysis.

Observed CLs values for the bRPV grid in the 1tau analysis.

Systematic uncertainty for the GMSB grid in the 2tau analysis.

Acceptance for the GMSB grid in the 2tau analysis.

Efficiency for the GMSB grid in the 2tau analysis.

Product of acceptance and efficiency for the GMSB grid in the 2tau analysis.

Expected CLs values for the GMSB grid in the 2tau analysis.

Observed CLs values for the GMSB grid in the 2tau analysis.

Systematic uncertainty for the nGM grid in the 2tau analysis.

Acceptance for the nGM grid in the 2tau analysis.

Efficiency for the nGM grid in the 2tau analysis.

Product of acceptance and efficiency for the nGM grid in the 2tau analysis.

Expected CLs values for the nGM grid in the 2tau analysis.

Observed CLs values for the nGM grid in the 2tau analysis.

Systematic uncertainty for the bRPV grid in the 2tau analysis.

Acceptance for the bRPV grid in the 2tau analysis.

Efficiency for the bRPV grid in the 2tau analysis.

Product of acceptance and efficiency for the bRPV grid in the 2tau analysis.

Expected CLs values for the bRPV grid in the 2tau analysis.

Observed CLs values for the bRPV grid in the 2tau analysis.

Systematic Uncertainty for the GMSB grid in the tau+e analysis.

Acceptance for the GMSB grid in the tau+e analysis.

Efficiency for the GMSB grid in the tau+e analysis.

Product of acceptance and efficiency for the GMSB grid in the tau+e analysis.

Expected CLs values for the GMSB grid in the tau+e analysis.

Observed CLs values for the GMSB grid in the tau+e analysis.

Systematic Uncertainty for the nGM grid in the tau+e analysis.

Acceptance for the nGM grid in the tau+e analysis.

Efficiency for the nGM grid in the tau+e analysis.

Product of acceptance and efficiency for the nGM grid in the tau+e analysis.

Expected CLs values for the nGM grid in the tau+e analysis.

Observed CLs values for the nGM grid in the tau+e analysis.

Systematic Uncertainty for the bRPV grid in the tau+e analysis.

Acceptance for the bRPV grid in the tau+e analysis.

Efficiency for the bRPV grid in the tau+e analysis.

Product of acceptance and efficiency for the bRPV grid in the tau+e analysis.

Expected CLs values for the bRPV grid in the tau+e analysis.

Observed CLs values for the bRPV grid in the tau+e analysis.

Systematic Uncertainty for the mSUGRA grid in the tau+e analysis.

Acceptance for the mSUGRA grid in the tau+e analysis.

Efficiency for the mSUGRA grid in the tau+e analysis.

Product of acceptance and efficiency for the mSUGRA grid in the tau+e analysis.

Expected CLs values for the mSUGRA grid in the tau+e analysis.

Observed CLs values for the mSUGRA grid in the tau+e analysis.

Systematic Uncertainty for the GMSB grid in the tau+mu analysis.

Acceptance for the GMSB grid in the tau+mu analysis.

Efficiency for the GMSB grid in the tau+mu analysis.

Product of acceptance and efficiency for the GMSB grid in the tau+mu analysis.

Expected CLs values for the GMSB grid in the tau+mu analysis.

Observed CLs values for the GMSB grid in the tau+mu analysis.

Systematic Uncertainty for the nGM grid in the tau+mu analysis.

Acceptance for the nGM grid in the tau+mu analysis.

Efficiency for the nGM grid in the tau+mu analysis.

Product of acceptance and efficiency for the nGM grid in the tau+mu analysis.

Expected CLs values for the nGM grid in the tau+mu analysis.

Observed CLs values for the nGM grid in the tau+mu analysis.

Systematic Uncertainty for the bRPV grid in the tau+mu analysis.

Acceptance for the bRPV grid in the tau+mu analysis.

Efficiency for the bRPV grid in the tau+mu analysis.

Product of acceptance and efficiency for the bRPV grid in the tau+mu analysis.

Expected CLs values for the bRPV grid in the tau+mu analysis.

Observed CLs values for the bRPV grid in the tau+mu analysis.

Systematic Uncertainty for the mSUGRA grid in the tau+mu analysis.

Acceptance for the mSUGRA grid in the tau+mu analysis.

Efficiency for the mSUGRA grid in the tau+mu analysis.

Product of acceptance and efficiency for the mSUGRA grid in the tau+mu analysis.

Expected CLs values for the mSUGRA grid in the tau+mu analysis.

Observed CLs values for the mSUGRA grid in the tau+mu analysis.

Example cutflow for three benchmark signal points in the 1-tau channel. For the GMSB point 50000 events have been generated, 20000 for nGM and 20000 for mSUGRA respectively. These event numbers are then normalised to 21 fb^{-1} luminosity.

Example cutflow for three benchmark signal points in the 2tau analysis. Specific SRs are indicated at the respective cut. Event numbers are normalised to 21 fb^{-1} luminosity. For the GMSB point 50000 events have been generated, 20000 for nGM and 25000 for bRPV respectively.

Example cutflow for four benchmark signal points in the tau+e analysis. Event numbers are normalised to 21 fb^{-1} luminosity. For the GMSB point 50000 events have been generated, 20000 for nGM, 20000 for mSUGRA and 25000 for bRPV respectively.

Example cutflow for four benchmark signal points in the tau+mu analysis. Event numbers are normalised to 21 fb^{-1} luminosity. For the GMSB point 50000 events have been generated, 20000 for nGM, 20000 for mSUGRA and 25000 for bRPV respectively.

The differential cross section measurement as a function of the transverse momentum of the second leading jet.

The differential cross section measurement as a function of the transverse momentum of the third leading jet.

The differential cross section measurement as a function of the transverse momentum of the fourth leading jet.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for jet multiplicities of one or more.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for jet multiplicities of two or more.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for jet multiplicities of three or more.

The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for jet multiplicities of four or more.

The differential cross section measurement as a function of the absolute value of the pseudorapidity of the first leading jet.

The differential cross section measurement as a function of the absolute value of the pseudorapidity of the first second jet.

The differential cross section measurement as a function of the absolute value of the pseudorapidity of the third leading jet.

The differential cross section measurement as a function of the absolute value of the pseudorapidity of the fourth leading jet.

The differential cross section measurement as a function of the absolute value of the azimuthal separation between the first leading jet and the muon.

The differential cross section measurement as a function of the absolute value of the azimuthal separation between the second leading jet and the muon.

The differential cross section measurement as a function of the absolute value of the azimuthal separation between the third leading jet and the muon.

The differential cross section measurement as a function of the absolute value of the azimuthal separation between the fourth leading jet and the muon.

The Psi(2S) pT-differential cross sections in p-Pb, in the centre of mass rapidity range 2.03<y_cms<3.53. First uncertainty is statistical, the second one is the pT-correlated systematic, the third is the uncorrelated systematic. The fourth is a global uncertainty common to p-Pb and Pb-p results.

The Psi(2S) pT-differential cross sections in Pb-p, in the centre of mass rapidity range -4.46<y_cms<-2.96. First uncertainty is statistical, the second one is the pT-correlated systematic, the third the uncorrelated systematic. The fourth is a global uncertainty common to p-Pb and Pb-p results.

Double ratio [sigma(Psi(2S))/sigma(J/Psi)]_pA/[sigma(Psi(2S))/sigma(J/Psi)]_pp in p-Pb collisions as a function of pT. Results are obtained in the centre of mass rapidity range 2.03<y_cms<3.53. First uncertainty is statistical, the second one is the correlated systematic, the third the uncorrelated systematic.

Double ratio [sigma(Psi(2S))/sigma(J/Psi)]_pA/[sigma(Psi(2S))/sigma(J/Psi)]_pp in Pb-p collisions as a function of pT. Results are obtained in the centre of mass rapidity range -4.46<y_cms<-2.96. First uncertainty is statistical, the second one is the correlated systematic, the third the uncorrelated systematic.

The Psi(2S) RpA versus pT in p-Pb collisions. Results are obtained in the centre of mass rapidity range 2.03<y_cms<3.53. First uncertainty is statistical, the second one is the correlated systematic, the third the uncorrelated systematic. The fourth is a global uncertainty common to the JPsi and PsiP RpA.

The Psi(2S) RpA versus pT in Pb-p collisions. Results are obtained in the centre of mass rapidity range -4.46<y_cms<-2.96. First uncertainty is statistical, the second one is the correlated systematic, the third the uncorrelated systematic. The fourth is a global uncertainty common to the JPsi and PsiP RpA.

Normalised differential TOP TOPBAR production cross section as a function of the number of additional jets with PT(JET) > 30 GeV in the lepton+jets channel. The total uncertainties are shown and include the statistical and systematic uncertainties.

Measured gap fraction in the dilepton channel as a function of the additional jet transverse momentum, GAPFRAC(PT) = N(PT)/N(TOTAL) where N(PT) is the number of events that do not contain additional jets above the given PT threshold.

Measured gap fraction in the dilepton channel as a function of the scalar sum of the transverse momentum of the additional jets, HT = SUM(PT(ADD. JETS)), GAPFRAC(HT) = N(HT)/N(TOTAL) where N(HT) is the number of events in which HT (with PT > 30 GeV) is less than the given threshold.

The systematic uncertainties for the nominal muon-channel cross-section measurement. Some sources of uncertainty have both correlated and uncorrelated components. Correlated uncertainties arise from the uncertainty in the electroweak background contributions delta(e.w.)_cor, from corrections to the Monte Carlo modelling of the Z/gamma* pT spectra, and from the reconstruction, trigger and isolation efficiency corrections, given by delta(reco)_cor, delta(trig)_cor and delta(iso)_cor respectively. The uncertainty on the multijet and electroweak background cross sections, given by delta(multijet and delta(e.w.), respectively and muon momentum scale uncertainty, delta(pT_scale) are also correlated. Uncorrelated uncertainties are due to corrections for the trigger and isolation efficiencies, given by delta(trig)_unc and delta(iso)_unc respectively. The uncertainty from the muon resolution correction, delta(res), from the size of the signal Monte Carlo sample, delta(MC), and the uncertaintities due to corrections for the reconstruction, delta(reco)_unc, are also uncorrelated. The luminosity uncertainty 1.8% is not included.

The combined Born-level fiducial differential cross section dsigma/dm_ll, statistical delta(stat), total correlated delta(cor), uncorrelated delta(unc), and total delta(total) uncertainties, as well as individual correlated sources delta(cor)_i. The correlated uncertainties are a linear combination of the 13 correlated uncertainties in the nominal muon and electron channels. As the uncertainties on the combined result no longer originate from individual error sources they are numbered 1-13. Also shown is the correction factor used to derive the dressed cross section (D), and the NNLO extrapolation factor (A) used to derive the cross section for the full phase space, along with the uncertainties associated to variations in scale choice delta(A)_scale, and PDF uncertainty delta(A)_pdf_alpha_s. The luminosity uncertainty 1.8% is not included.

The extended muon channel Born-level fiducial differential cross section dsigma/dm_ll, with the statistical delta(stat), systematic delta(syst), and total delta(tot) uncertainties for each invariant mass bin. Also shown is the correction factor used to derive the dressed cross section (D), and the extrapolation factor (A) used to derive the cross section for the full phase space, along with the uncertainties associated to variations in scale delta(A)_scale, and PDF uncertainty delta(A)_pdf_alpha_s. The luminosity uncertainty 3.5% is not included.

The systematic uncertainties for the extended muon channel cross-section measurement in each invariant mass bin. Correlated uncertainties come from the reconstruction, trigger and isolation efficiency corrections, given by delta(reco), delta(trig) and delta(iso) respectively. The uncertainty on the multijet background cross section, delta(multijet) and the uncertainty on the muon momentum scale, delta(pT_scale), are also correlated across bins. Uncorrelated uncertainties are due to the uncertainty from the muon resolution correction, delta(res), and the sample size of the signal Monte Carlo sample, delta(MC). The luminosity uncertainty 3.5% is not included.

Theory predictions for NLO+LLPS and for fixed-order calculations at NLO and NNLO including higher-order electroweak corrections, for the nominal analysis of the differential cross section dsigma/dm_ll as a function of the invariant mass m_ll. The scale uncertainty is defined as the envelope of variations for 0.5< mu_R,mu_F<2.0 for Powheg. For Fewz the scale uncertainty is defined by the variation 0.5<mu_R=mu_F<2.0. The uncertainty labelled as "stat" in the table corresponds to the pdf+alpha_s uncertainty for Fewz or just the pdf uncertainty for Powheg.

Theory predictions for NLO+LLPS and for fixed-order calculations at NLO and NNLO including higher-order electroweak corrections, for the extended analysis of the differential cross section dsigma/dm_ll as a function of the invariant mass m_ll. The scale uncertainty is defined as the envelope of variations for 0.5<mu_R,mu_F<2.0 for Powheg. For Fewz the scale uncertainty is defined by the variation 0.5<mu_R=mu_F<2.0. The uncertainty labelled as "stat" in the table corresponds to the pdf+alpha_s uncertainty for Fewz or just the pdf uncertainty for Powheg.

Higher-order electroweak corrections in nominal analysis, Delta(HOEW), and the correction for the Photon Induced process, Delta(PI), together with its uncertainty derived from the uncertainty of the photon PDF as a function of the dilepton invariant mass m_ll. Also shown is the difference arising from the non-convergence of calculations derived with different electroweak schema, delta(scheme).

Higher-order electroweak corrections in extended analysis, Delta(HOEW), and the correction for the Photon Induced process, Delta(PI), together with its uncertainty derived from the uncertainty of the photon PDF as a function of the dilepton invariant mass m_ll. Also shown is the difference arising from the non-convergence of calculations derived with different electroweak schema, delta(scheme).

Values of chi^2 for the nominal and extended DY cross-section measurements for predictions based from Fewz at NLO and NNLO and Powheg using MSTW2008 PDFs accounting for the experimental correlated systematic uncertainties. The _pdf_scale columns show the chi^2 when the PDF and scale uncertainties on the theoretical predictions are taken into account.

The chi^2 values from NLO and NNLO QCD fits made using the ATLAS nominal and extended Drell--Yan cross-section measurements and the HERA-I dataset accounting for the experimental correlated systematic uncertainties.

The measured individual cross sections in the fiducial region and the combined cross sections for 4-muon and 4-electron final states at a centre-of-collision energy of 8 TeV.

The measured individual cross sections in the fiducial region and the combined cross sections for for 2-muon-2-electron final states at a centre-of-collision energy of 8 TeV.

The measured cross section for four-lepton final states at a centre-of-collision energy of 8 TeV.

The branching fraction for Z0 --> 4 LEPTON, summed over all final states, measured using both the 7 and 8 TeV datasets.

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.

Measured differential cross sections as function of the lepton pseudo-rapidity of the production of a W boson with a D meson or a D* meson times the branching ratio W -> l nu in the fiducial regions together with the statistical and systematic uncertainties. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events.

Measured cross section ratios of the production of a W boson with a D meson or a D* meson and the inclusive production of a W boson in the fiducial regions together with the statistical and systematic uncertainties. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events.

Measured differential cross section ratios of the production of a W boson with a D meson or a D* meson and the inclusive production of a W boson in the fiducial regions as function of the D/D* meson pT together with the statistical and systematic uncertainties. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events.

Measured integrated cross sections of the production of a W boson in association with a single c-jet and exactly zero or one additional non-c-jets times the branching ratio W -> l nu in the fiducial regions together with the statistical and systematic uncertainties. The particle-level c-jet is defined as the one containing a weakly decaying c-hadron with pt>5 GeV, within DeltaR<0.3. Jets containing c-hadrons originating from b-hadron decays are not counted as c-jets. The cross sections are defined for OS-SS events.

Measured integrated cross sections ratio of the production of a W+ and W- bosons in association with a single c-jet and exactly zero or one additional non-c-jets in the fiducial regions together with the statistical and systematic uncertainties. The particle-level c-jet is defined as the one containing a weakly decaying c-hadron with pt>5 GeV, within DeltaR<0.3. Jets containing c-hadrons originating from b-hadron decays are not counted as c-jets. The cross sections are defined for OS-SS events.

Measured integrated cross sections of the production of a W boson in association with a single c-jet decaying into a soft muon in the fiducial regions together with the statistical and systematic uncertainties. The particle-level c-jet is defined as the one containing a weakly decaying c-hadron with pt>5 GeV, within DeltaR<0.3. Jets containing c-hadrons originating from b-hadron decays are not counted as c-jets. Soft muons are associated to c-jets within a cone of DeltaR<0.5. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events.

Correlation matrix corresponding to the total uncertainties of measured integrated cross sections of the production of a W boson with a single c-jet, a D meson or a D* meson times the branching ratio W -> l nu in the fiducial regions.

Systematic uncertainties after the averaging procedure of the inclusive cross sections in different channels. The first row (labeled Uncorr.) represents the uncorrelated systematic uncertainties. The following rows represent the diagonalized list of systematic uncertainties which are correlated across all channels. The luminosity is included in these correlated systematic uncertainties.

Systematic uncertainties after the averaging procedure of the differential cross sections as function of the lepton pseudo-rapidity in different channels. The first row (labeled Uncorr.) represents the uncorrelated systematic uncertainties. The following rows represent the diagonalized list of systematic uncertainties which are correlated across all channels and bins. The luminosity is included in these correlated systematic uncertainties. The systematic uncertainties for the W+ + cbar-jet channel are shown in this table.

Systematic uncertainties after the averaging procedure of the differential cross sections as function of the lepton pseudo-rapidity in different channels. The first row (labeled Uncorr.) represents the uncorrelated systematic uncertainties. The following rows represent the diagonalized list of systematic uncertainties which are correlated across all channels and bins. The luminosity is included in these correlated systematic uncertainties. The systematic uncertainties for the W- + c-jet channel are shown in this table.

Systematic uncertainties after the averaging procedure of the differential cross sections as function of the lepton pseudo-rapidity in different channels. The first row (labeled Uncorr.) represents the uncorrelated systematic uncertainties. The following rows represent the diagonalized list of systematic uncertainties which are correlated across all channels and bins. The luminosity is included in these correlated systematic uncertainties. The systematic uncertainties for the W+ D- and W- D+ channels are shown in this table.

Systematic uncertainties after the averaging procedure of the differential cross sections as function of the lepton pseudo-rapidity in different channels. The first row (labeled Uncorr.) represents the uncorrelated systematic uncertainties. The following rows represent the diagonalized list of systematic uncertainties which are correlated across all channels and bins. The luminosity is included in these correlated systematic uncertainties. The systematic uncertainties for the W+ D*- and W- D*+ channels are shown in this table.

Theoretical Predictions for the integrated cross section of the production of W+ and W- bosons associated with a single c-jet, a D meson or a D* meson in the fiducial regions together with the statistical and systematic uncertainties. For the W+c-jet cross sections events with more than one c-jet are discarded. The particle-level c-jet is defined as the one containing a weakly decaying c-hadron with pt>5 GeV, within DeltaR<0.3. Jets containing c-hadrons originating from b-hadron decays are not counted as c-jets. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events. The predictions have been obtained the aMC@NLO MC simulation interfaced to the Herwig++ parton shower programme. The uncertainties on the predictions entail PDF uncertainties, parton shower, fragmentation and scale uncertainties. The predictions are reweighted using LHAPDF from the CT10nlo PDF set to the following PDF sets with the LHAPDF IDs given in brackets: CT10nlo (11000), MSTW2008nlo68cl (21100), NNPDF23_nlo_as_0119 (230000), NNPDF23_nlo_collider_as_0119 (236000), HERAPDF15NLO (EIG+VAR, 60700+60730), ATLAS-epWZ12 (EIG+VAR, 65000+65040).

PDF uncertainty for each of the used PDF sets as well as the combined parton shower, fragmentation and scale uncertainties (given in percent) for the theoretical Predictions for the integrated cross section of the production of W+ and W- bosons associated with a single c-jet, a D meson or a D* meson in the fiducial regions together with the statistical and systematic uncertainties. If added quadratically, these uncertainties represent the total uncertainty on the quoted theory prediction. For the W+c-jet cross sections events with more than one c-jet are discarded. The particle-level c-jet is defined as the one containing a weakly decaying c-hadron with pt>5 GeV, within DeltaR<0.3. Jets containing c-hadrons originating from b-hadron decays are not counted as c-jets. Jets are not required for the W+D/D* cross sections. The cross sections are defined for OS-SS events. The predictions have been obtained the aMC@NLO MC simulation interfaced to the Herwig++ parton shower programme. The uncertainties on the predictions entail PDF uncertainties, FSR uncertainties and scale uncertainties. The predictions are reweighted using LHAPDF from the CT10nlo PDF set to the following PDF sets with the LHAPDF IDs given in brackets: CT10nlo (11000), MSTW2008nlo68cl (21100), NNPDF23_nlo_as_0119 (230000), NNPDF23_nlo_collider_as_0119 (236000), HERAPDF15NLO (EIG+VAR, 60700+60730), ATLAS-epWZ12 (EIG+VAR, 65000+65040). The determination of the parton shower, fragmentation and scale uncertainties is detailed in the paper.

The fully corrected measurement of ASYM(FB) as a function of the muon-pair invariant mass.

The cross section ratio for a Z boson produced with at least one b-jet, relative to a Z boson produced with at least one jet of any flavour.

The inclusive (SPS+DPS) cross-section ratio (times 10^6) as a function of J/psi transverse momentum under the TRANSVERSE-0 spin-alignment hypothesis. The first uncertainty is statistical and the second uncertainty is systematic.

The inclusive (SPS+DPS) cross-section ratio (times 10^6) as a function of J/psi transverse momentum under the TRANSVERSE-P spin-alignment hypothesis. The first uncertainty is statistical and the second uncertainty is systematic.

The inclusive (SPS+DPS) cross-section ratio (times 10^6) as a function of J/psi transverse momentum under the TRANSVERSE-M spin-alignment hypothesis. The first uncertainty is statistical and the second uncertainty is systematic.

Covariance matrix (statistical and systematic uncertainties combined) with the muon $p_{T}>35$ GeV. The units are in $10^{-4}$.

The DY pre-FSR cross section measurements for the combined dimuon and dielectron channels normalized to the Z-peak region in the full acceptance.

The DY dimuon rapidity spectrum within the detector acceptance, normalized to the Z-peak region, for the mass bin 20-30 GeV. The two columns correspond to pre-FSR and post-FSR. The uncertainties are the total experimental uncertainties.

The DY dimuon rapidity spectrum within the detector acceptance, normalized to the Z-peak region, for the mass bin 30-45 GeV. The two columns correspond to pre-FSR and post-FSR. The uncertainties are the total experimental uncertainties.

The DY dimuon rapidity spectrum within the detector acceptance, normalized to the Z-peak region, for the mass bin 45-60 GeV. The two columns correspond to pre-FSR and post-FSR. The uncertainties are the total experimental uncertainties.

The DY dimuon rapidity spectrum within the detector acceptance, normalized to the Z-peak region, for the mass bin 60-120 GeV. The two columns correspond to pre-FSR and post-FSR. The uncertainties are the total experimental uncertainties.

The DY dimuon rapidity spectrum within the detector acceptance, normalized to the Z-peak region, for the mass bin 120-200 GeV. The two columns correspond to pre-FSR and post-FSR. The uncertainties are the total experimental uncertainties.

The DY dimuon rapidity spectrum within the detector acceptance, normalized to the Z-peak region, for the mass bin 200-1500 GeV. The two columns correspond to pre-FSR and post-FSR. The uncertainties are the total experimental uncertainties.