Differential fiducial cross section (without the acceptance correction) for the DY process measured in the muon channel, as a function of $p_{\textrm{T}}$ for $15<m_{\mu\mu}<60$ GeV. The quoted error is the quadratic sum of the statistical and systematic uncertainties. The global normalisation uncertainty of 3.5% is listed separately.

Differential fiducial cross section (without the acceptance correction) for the DY process measured in the muon channel, as a function of $p_{\textrm{T}}$ for $60<m_{\mu\mu}<120$ GeV. The quoted error is the quadratic sum of the statistical and systematic uncertainties. The global normalisation uncertainty of 3.5% is listed separately.

Differential fiducial cross section (without the acceptance correction) for the DY process measured in the muon channel, as a function of $\phi^*$ for $15<m_{\mu\mu}<60$ GeV. The quoted error is the quadratic sum of the statistical and systematic uncertainties. The global normalisation uncertainty of 3.5% is listed separately.

Differential fiducial cross section (without the acceptance correction) for the DY process measured in the muon channel, as a function of $\phi^*$ for $60<m_{\mu\mu}<120$ GeV. The quoted error is the quadratic sum of the statistical and systematic uncertainties. The global normalisation uncertainty of 3.5% is listed separately.

Integrated fiducial cross section for the DY process measured in the muon channel. The quoted error is the quadratic sum of the statistical and systematic uncertainties. The global normalisation uncertainty of 3.5% is listed separately.

Differential cross section for the DY process measured in the muon channel, as a function of dimuon invariant mass. The quoted error is the quadratic sum of the statistical and systematic uncertainties. The global normalisation uncertainty of 3.5% is listed separately.

Differential cross section for the DY process measured in the muon channel, as a function of rapidity in the centre-of-mass frame for $15<m_{\mu\mu}<60$ GeV. The quoted error is the quadratic sum of the statistical and systematic uncertainties. The global normalisation uncertainty of 3.5% is listed separately.

Differential cross section for the DY process measured in the muon channel, as a function of rapidity in the centre-of-mass frame for $60<m_{\mu\mu}<120$ GeV. The quoted error is the quadratic sum of the statistical and systematic uncertainties. The global normalisation uncertainty of 3.5% is listed separately.

Differential cross section for the DY process measured in the muon channel, as a function of $p_{\textrm{T}}$ for $15<m_{\mu\mu}<60$ GeV. The quoted error is the quadratic sum of the statistical and systematic uncertainties. The global normalisation uncertainty of 3.5% is listed separately.

Differential cross section for the DY process measured in the muon channel, as a function of $p_{\textrm{T}}$ for $60<m_{\mu\mu}<120$ GeV. The quoted error is the quadratic sum of the statistical and systematic uncertainties. The global normalisation uncertainty of 3.5% is listed separately.

Differential cross section for the DY process measured in the muon channel, as a function of $\phi^*$ for $15<m_{\mu\mu}<60$ GeV. The quoted error is the quadratic sum of the statistical and systematic uncertainties. The global normalisation uncertainty of 3.5% is listed separately.

Differential cross section for the DY process measured in the muon channel, as a function of $\phi^*$ for $60<m_{\mu\mu}<120$ GeV. The quoted error is the quadratic sum of the statistical and systematic uncertainties. The global normalisation uncertainty of 3.5% is listed separately.

Integrated cross section for the DY process measured in the muon channel. The quoted error is the quadratic sum of the statistical and systematic uncertainties. The global normalisation uncertainty of 3.5% is listed separately.

Forward-backward ratios for $15<m_{\mu\mu}<60$ GeV. Quoted uncertainties are the quadratic sum of the statistical and systematic uncertainties.

Forward-backward ratios for $60<m_{\mu\mu}<120$ GeV. Quoted uncertainties are the quadratic sum of the statistical and systematic uncertainties.

Correlation matrix for the systematic uncertainties, excluding integrated luminosity, as a function of dimuon invariant mass.

Correlation matrix for the systematic uncertainties, excluding integrated luminosity, as a function of rapidity in the centre-of-mass frame for $15<m_{\mu\mu}<60$ GeV.

Correlation matrix for the systematic uncertainties, excluding integrated luminosity, as a function of rapidity in the centre-of-mass frame for $60<m_{\mu\mu}<120$ GeV.

Correlation matrix for the systematic uncertainties, excluding integrated luminosity, as a function of $p_{\textrm{T}}$ for $15<m_{\mu\mu}<60$ GeV.

Correlation matrix for the systematic uncertainties, excluding integrated luminosity, as a function of $p_{\textrm{T}}$ for $60<m_{\mu\mu}<120$ GeV.

Correlation matrix for the systematic uncertainties, excluding integrated luminosity, as a function of $\phi^*$ for $15<m_{\mu\mu}<60$ GeV.

Correlation matrix for the systematic uncertainties, excluding integrated luminosity, as a function of $\phi^*$ for $60<m_{\mu\mu}<120$ GeV.

Correlation matrix for the systematic uncertainties, excluding integrated luminosity, as a function of rapidity in the centre-of-mass frame, putting together low and high masses. Each bin is labeled lm_i or hm_i, where lm stands for $15<m_{\mu\mu}<60$ GeV, hm stands for $60<m_{\mu\mu}<120$ GeV, and i is the corresponding bin number in rapidity in the centre-of-mass frame. The global normalisation uncertainty of 3.5% is not included. Data from Figure [3, 4, 4].

Correlation matrix for the systematic uncertainties, excluding integrated luminosity, as a function of $p_{\textrm{T}}$, putting together low and high masses. Each bin is labeled lm_i or hm_i, where lm stands for $15<m_{\mu\mu}<60$ GeV, hm stands for $60<m_{\mu\mu}<120$ GeV, and i is the corresponding bin number in $p_{\textrm{T}}$. The global normalisation uncertainty of 3.5% is not included. Data from Figure [3, 4, 4].

Correlation matrix for the systematic uncertainties, excluding integrated luminosity, as a function of $\phi^*$, putting together low and high masses. Each bin is labeled lm_i or hm_i, where lm stands for $15<m_{\mu\mu}<60$ GeV, hm stands for $60<m_{\mu\mu}<120$ GeV, and i is the corresponding bin number in $\phi^*$. The global normalisation uncertainty of 3.5% is not included. Data from Figure [3, 4, 4].

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Forward cross sections.

Backward cross sections.

From S, P and D wave fit to d(sig)/domega.

The differential cross section of $Z$ boson production scaled by 1/$p_\mathrm{T}^{Z}$, (1/$p_\mathrm{T}^{Z}$) $d\sigma /dp_\mathrm{T}^{Z}$, for $-3<y^\mathrm{*}_{Z}<2$.

The differential cross section of $Z$ boson production scaled by 1/$p_\mathrm{T}^{Z}$, (1/$p_\mathrm{T}^{Z}$) $d\sigma /dp_\mathrm{T}^{Z}$, for $-2<y^\mathrm{*}_{Z}<0$ and $0<y^\mathrm{*}_{Z}<2.

Centrality bias corrected $Z$ boson yields per event for $-3<y^\mathrm{*}_{Z}<2$ scaled by by $\langle N_{coll}\rangle$. (To remove the centrality bias correction each value may be multiplied by the approriate correction value found in arXiv:1412.0976.).

The rapidity differential Z boson yields per event scaled by $\langle N_{coll}\rangle$ for three centrality ranges.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles emittedon an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.7 < ETA RAP < 2.02, is subdivided into eight nominally equal bins of 0.16 in pseudo rapidity.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.22 < ET ARAP < 2.5, is subdivided into eight nominally equal bins of 0.16 in pseudo rapidity.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.38 < ET ARAP < 2.34, is subdivided into eight nominally equal bins of 0.16 in pseud orapidity.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.54 < ET ARAP < 2.18, is subdivided into eight nominally equal bins of 0.16 in pseud orapidity.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.7 < ETA RAP < 2.02, is subdivided into eight nominally equal bins of 0.16 in pseudo rapidity.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.22 < ET ARAP < 2.5, is subdivided into eight nominally equal bins of 0.16 in pseudo rapidity.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.38 < ET ARAP < 2.34, is subdivided into eight nominally equal bins of 0.16 in pseud orapidity.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.54 < ET ARAP < 2.18, is subdivided into eight nominally equal bins of 0.16 in pseud orapidity.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.7 < ETA RAP < 2.02, is subdivided into eight nominally equal bins of 0.16 in pseudo rapidity.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.22 < ET ARAP < 2.5, is subdivided into eight nominally equal bins of 0.16 in pseudo rapidity. ET distributions define centrality, tipically by a certain upper perc entile of the distribution. In the table centrality denoted as ZCAL(Zero de gree CALorimeter).

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.38 < ET ARAP < 2.34, is subdivided into eight nominally equal bins of 0.16 in pseud orapidity. ET distributions define centrality, tipically by a certain upper perc entile of the distribution. In the table centrality denoted as ZCAL(Zero de gree CALorimeter).

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.54 < ET ARAP < 2.18, is subdivided into eight nominally equal bins of 0.16 in pseud orapidity. ET distributions define centrality, tipically by a certain upper perc entile of the distribution. In the table centrality denoted as ZCAL(Zero de gree CALorimeter).

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.7 < ETA RAP < 2.02, is subdivided into eight nominally equal bins of 0.16 in pseudo rapidity. ET distributions define centrality, tipically by a certain upper perc entile of the distribution. In the table centrality denoted as ZCAL(Zero de gree CALorimeter).

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.22 < ET ARAP < 2.5, is subdivided into eight nominally equal bins of 0.16 in pseudo rapidity.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.38 < ET ARAP < 2.34, is subdivided into eight nominally equal bins of 0.16 in pseud orapidity.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.54 < ET ARAP < 2.18, is subdivided into eight nominally equal bins of 0.16 in pseud orapidity.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.7 < ETA RAP < 2.02, is subdivided into eight nominally equal bins of 0.16 in pseudo rapidity.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.22 ETAR AP < 2.50, is subdivided into eight nominally equal bins of 0.16 in pseudor apidity.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.38 ETAR AP < 2.34, is subdivided into eight nominally equal bins of 0.16 in pseudor apidity.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.54 ETAR AP < 2.18, is subdivided into eight nominally equal bins of 0.16 in pseudor apidity.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.7 ETARA P < 2.02, is subdivided into eight nominally equal bins of 0.16 in pseudora pidity.

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.22 ETAR AP < 2.50, is subdivided into eight nominally equal bins of 0.16 in pseudor apidity. ET distributions define centrality, tipically by a certain upper perc entile of the distribution. In the table centrality denoted as ZCAL(Zero de gree CALorimeter).

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.38 ETAR AP < 2.34, is subdivided into eight nominally equal bins of 0.16 in pseudor apidity. ET distributions define centrality, tipically by a certain upper perc entile of the distribution. In the table centrality denoted as ZCAL(Zero de gree CALorimeter).

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.54 ETAR AP < 2.18, is subdivided into eight nominally equal bins of 0.16 in pseudor apidity. ET distributions define centrality, tipically by a certain upper perc entile of the distribution. In the table centrality denoted as ZCAL(Zero de gree CALorimeter).

ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.7 ETARA P < 2.02, is subdivided into eight nominally equal bins of 0.16 in pseudora pidity. ET distributions define centrality, tipically by a certain upper perc entile of the distribution. In the table centrality denoted as ZCAL(Zero de gree CALorimeter).

Incident energy 14.6 GeV/nucleon.

Incident energy 14.6 GeV/nucleon.

Incident energy 11.6 GeV/nucleon.

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EXTRAPOLATION OF Q**2 AND T DEPENDENCE TO CALCULATE THE TOTAL ELASTIC J/PSI PHOTOPRODUCTION (Q**2=0) ON IRON.