Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.81<|\eta^{\gamma}|<2.37$.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $|\eta^{\gamma}|<0.6$.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $0.6<|\eta^{\gamma}|<1.37$.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.56<|\eta^{\gamma}|<1.81$.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.81<|\eta^{\gamma}|<2.37$.

The pseudorapidity ($|\eta|$) distribution for $K^{0}_{S}$ production inside $b$-jets for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), out-of-fiducial events and the unfolding non-closure.

The multiplicity ($N_K$) distribution for $K^{0}_{S}$ production inside $b$-jets for unfolded data to particle level, including only visible decays ($K^0_S \rightarrow \pi^+ \pi^-$), normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), out-of-fiducial events and the unfolding non-closure.

The transverse momentum ($p_{T}$) distribution for $K^{0}_{S}$ production inside non $b$-jets for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), out-of-fiducial events and the unfolding non-closure.

The energy fraction ($x_{K}$) distribution for $K^{0}_{S}$ production inside non $b$-jets for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), out-of-fiducial events and the unfolding non-closure.

The energy distribution for $K^{0}_{S}$ production inside non $b$-jets for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), out-of-fiducial events and the unfolding non-closure.

The pseudorapidity ($|\eta|$) distribution for $K^{0}_{S}$ production inside non $b$-jets for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), out-of-fiducial events and the unfolding non-closure.

The multiplicity ($N_K$) distribution for $K^{0}_{S}$ production inside non $b$-jets for unfolded data to particle level, including only visible decays ($K^0_S \rightarrow \pi^+ \pi^-$), normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), out-of-fiducial events and the unfolding non-closure.

The transverse momentum ($p_{T}$) distribution for $K^{0}_{S}$ production not associated with jets for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), the pile-up, out-of-fiducial events and the unfolding non-closure.

The energy distribution for $K^{0}_{S}$ production not associated with jets for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), the pile-up, out-of-fiducial events and the unfolding non-closure.

The pseudorapidity ($|\eta|$) distribution for $K^{0}_{S}$ production not associated with jets for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), the pile-up, out-of-fiducial events and the unfolding non-closure.

The multiplicity ($N_K$) distribution for $K^{0}_{S}$ production not associated with jets for unfolded data to particle level, including only visible decays ($K^0_S \rightarrow \pi^+ \pi^-$), normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), the pile-up, out-of-fiducial events and the unfolding non-closure.

The transverse momentum ($p_{T}$) distribution for the total $K^{0}_{S}$ production for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), the pile-up, out-of-fiducial events and the unfolding non-closure.

The energy distribution for the total $K^{0}_{S}$ production for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), the pile-up, out-of-fiducial events and the unfolding non-closure.

The pseudorapidity ($|\eta|$) distribution for the total $K^{0}_{S}$ production for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), the pile-up, out-of-fiducial events and the unfolding non-closure.

The multiplicity ($N_K$) distribution for the total $K^{0}_{S}$ production for unfolded data to particle level, including only visible decays ($K^0_S \rightarrow \pi^+ \pi^-$), normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), the pile-up, out-of-fiducial events and the unfolding non-closure.

The transverse momentum ($p_{T}$) distribution for the total $\Lambda$ production for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), the pile-up, out-of-fiducial events and the unfolding non-closure.

The energy distribution for the total $\Lambda$ production for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), the pile-up, out-of-fiducial events and the unfolding non-closure.

The pseudorapidity ($|\eta|$) distribution for the total $\Lambda$ production for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), the pile-up, out-of-fiducial events and the unfolding non-closure.

$K^0_S$ and $\Lambda$ unfolded (particle-level) average multiplicities per event ($\langle n_{K,\Lambda}\rangle$), including statistical and systematic uncertainties, for each class and for the total sample.

Normalised production yields of $W^+$ and $W^-$ bosons as a function of $⟨N_{\mathrm{part}}⟩$ shown for the combination of electron and muon decay channels.

Normalised production yields for $W^+$ bosons as a function of $⟨N_{\mathrm{part}}⟩$ for geometric parameters obtained with the MCGlauber v2.4 and v3.2.

Normalised production yields for $W^-$ bosons as a function of $⟨N_{\mathrm{part}}⟩$ for geometric parameters obtained with the MCGlauber v2.4 and v3.2.

Nuclear modification factor $R_{\mathrm{AA}}$ obtained from the fiducial $W^+$ and $W^-$ boson production yields as a function of $⟨N_{\mathrm{part}}⟩$.

The covariance matrix of the differential normalised production yields for $W^+$ bosons. Systematic uncertainties related to $T_{\mathrm{AA}}$ (1.6%) are not included.

The covariance matrix of the differential normalised production yields for $W^-$ bosons. Systematic uncertainties related to $T_{\mathrm{AA}}$ (1.6%) are not included.

The covariance matrix of the lepton charge asymmetry.

Dependence of the overall signal efficiency on the pT of the long-lived Z' for Z' -> ee. The error bars indicate the total uncertainties.

Dependence of the overall signal efficiency on the transverse decay radius Rxy of the long-lived Z' for Z' -> emu. The error bars indicate the total uncertainties.

Dependence of the overall signal efficiency on the pT of the long-lived Z' for Z' -> emu. The error bars indicate the total uncertainties.

Dependence of the overall signal efficiency on the transverse decay radius Rxy of the long-lived Z' for Z' -> mumu. The error bars indicate the total uncertainties.

Dependence of the overall signal efficiency on the pT of the long-lived Z' for Z' -> mumu. The error bars indicate the total uncertainties.

Overall signal efficiency as a function of the mean proper lifetime (ctau) of the neutralino for the lambda121 scenario of the RPV SUSY model. The error bars indicate the total uncertainties.

Overall signal efficiency as a function of the mean proper lifetime (ctau) of the neutralino for the lambda122 scenario of the RPV SUSY model. The error bars indicate the total uncertainties.

95% CL upper limits on the squark-antisquark production cross-section as a function of the mean proper lifetime (ctau) of the neutralino for the lambda121 scenario of the RPV SUSY model and a 700 GeV squark. The uncertainties of the expected limit indicate the +-1sigma variations.

95% CL upper limits on the squark-antisquark production cross-section as a function of the mean proper lifetime (ctau) of the neutralino for the lambda122 scenario of the RPV SUSY model and a 700 GeV squark. The uncertainties of the expected limit indicate the +-1sigma variations.

95% CL upper limits on the squark-antisquark production cross-section as a function of the mean proper lifetime (ctau) of the neutralino for the lambda121 scenario of the RPV SUSY model and a 1600 GeV squark. The uncertainties of the expected limit indicate the +-1sigma variations.

95% CL upper limits on the squark-antisquark production cross-section as a function of the mean proper lifetime (ctau) of the neutralino for the lambda122 scenario of the RPV SUSY model and a 1600 GeV squark. The uncertainties of the expected limit indicate the +-1sigma variations.

Fraction of detector volume covered by the material veto as a function of z and Rxy of the displaced dilepton vertex.

Fraction of detector volume covered by the disabled pixel modules veto veto as a function of z and Rxy of the displaced dilepton vertex.

Observed Rxy distribution of vertices composed of two non-leptonic tracks in a control sample in the data and the predicted distribution obtained from the event mixing. The error bars indicate the statistical uncertainties.

Rxy distributions of Kshort vertices from the large radius tracking in the data and background MC samples. Data has been normalised such that the total number of Kshort from the standard tracking in the data agrees with the total number of Kshort from the standard tracking in the MC. The error bars indicate the statistical uncertainties.

Acceptance per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> eenu. The error bars indicate the statistical uncertainties.

Acceptance per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> emunu. The error bars indicate the statistical uncertainties.

Acceptance per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> mumunu. The error bars indicate the statistical uncertainties.

Detection efficiency per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> eenu. The error bars indicate the total uncertainties.

Detection efficiency per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> emunu. The error bars indicate the total uncertainties.

Detection efficiency per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> mumunu. The error bars indicate the total uncertainties.

Overall signal efficiency (acceptance times efficiency) per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> eenu. The error bars indicate the total uncertainties.

Overall signal efficiency (acceptance times efficiency) per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> emunu. The error bars indicate the total uncertainties.

Overall signal efficiency (acceptance times efficiency) per decay as a function of the mean proper lifetime (ctau) of the neutralino for neutralino -> mumunu. The error bars indicate the total uncertainties.

Detection efficiency per decay for Rxy < 22 mm as a function of the invariant mass and pT of the electron pair in LLP -> eeX.

Detection efficiency per decay for 22 <= Rxy < 38 mm as a function of the invariant mass and pT of the electron pair in LLP -> eeX.

Detection efficiency per decay for 38 <= Rxy < 73 mm as a function of the invariant mass and pT of the electron pair in LLP -> eeX.

Detection efficiency per decay for 73 <= Rxy < 111 mm as a function of the invariant mass and pT of the electron pair in LLP -> eeX.

Detection efficiency per decay for 111 <= Rxy < 145 mm as a function of the invariant mass and pT of the electron pair in LLP -> eeX.

Detection efficiency per decay for 145 <= Rxy < 300 mm as a function of the invariant mass and pT of the electron pair in LLP -> eeX.

Detection efficiency per decay for Rxy < 22 mm as a function of the invariant mass and pT of the electron and muon pair in LLP -> emuX.

Detection efficiency per decay for 22 <= Rxy < 38 mm as a function of the invariant mass and pT of the electron and muon pair in LLP -> emuX.

Detection efficiency per decay for 38 <= Rxy < 73 mm as a function of the invariant mass and pT of the electron and muon pair in LLP -> emuX.

Detection efficiency per decay for 73 <= Rxy < 111 mm as a function of the invariant mass and pT of the electron and muon pair in LLP -> emuX.

Detection efficiency per decay for 111 <= Rxy < 145 mm as a function of the invariant mass and pT of the electron and muon pair in LLP -> emuX.

Detection efficiency per decay for 145 <= Rxy < 300 mm as a function of the invariant mass and pT of the electron and muon pair in LLP -> emuX.

Detection efficiency per decay for Rxy < 22 mm as a function of the invariant mass and pT of the muon pair in LLP -> mumuX.

Detection efficiency per decay for 22 <= Rxy < 38 mm as a function of the invariant mass and pT of the muon pair in LLP -> mumuX.

Detection efficiency per decay for 38 <= Rxy < 73 mm as a function of the invariant mass and pT of the muon pair in LLP -> mumuX.

Detection efficiency per decay for 73 <= Rxy < 111 mm as a function of the invariant mass and pT of the muon pair in LLP -> mumuX.

Detection efficiency per decay for 111 <= Rxy < 145 mm as a function of the invariant mass and pT of the muon pair in LLP -> mumuX.

Detection efficiency per decay for 145 <= Rxy < 300 mm as a function of the invariant mass and pT of the muon pair in LLP -> mumuX.

Detection efficiency per decay as a function of the transverse decay radius Rxy and the dilepton pT for a LLP mass of 100 GeV and LLP -> ee.

Detection efficiency per decay as a function of the transverse decay radius Rxy and the dilepton pT for a LLP mass of 100 GeV and LLP -> emu.

Detection efficiency per decay as a function of the transverse decay radius Rxy and the dilepton pT for a LLP mass of 100 GeV and LLP -> mumu.

Detection efficiency per decay as a function of the transverse decay radius Rxy and the dilepton pT for a LLP mass of 250 GeV and LLP -> ee.

Detection efficiency per decay as a function of the transverse decay radius Rxy and the dilepton pT for a LLP mass of 250 GeV and LLP -> emu.

Detection efficiency per decay as a function of the transverse decay radius Rxy and the dilepton pT for a LLP mass of 250 GeV and LLP -> mumu.

Detection efficiency per decay as a function of the transverse decay radius Rxy and the dilepton pT for a LLP mass of 500 GeV and LLP -> ee.

Detection efficiency per decay as a function of the transverse decay radius Rxy and the dilepton pT for a LLP mass of 500 GeV and LLP -> emu.

Detection efficiency per decay as a function of the transverse decay radius Rxy and the dilepton pT for a LLP mass of 500 GeV and LLP -> mumu.

Detection efficiency per decay as a function of the transverse decay radius Rxy and the dilepton pT for a LLP mass of 750 GeV and LLP -> ee.

Detection efficiency per decay as a function of the transverse decay radius Rxy and the dilepton pT for a LLP mass of 750 GeV and LLP -> emu.

Detection efficiency per decay as a function of the transverse decay radius Rxy and the dilepton pT for a LLP mass of 750 GeV and LLP -> mumu.

Detection efficiency per decay as a function of the transverse decay radius Rxy and the dilepton pT for a LLP mass of 1000 GeV and LLP -> ee.

Detection efficiency per decay as a function of the transverse decay radius Rxy and the dilepton pT for a LLP mass of 1000 GeV and LLP -> emu.

Detection efficiency per decay as a function of the transverse decay radius Rxy and the dilepton pT for a LLP mass of 1000 GeV and LLP -> mumu.

Acceptance, detection efficiency, and overall signal efficiency in the Z' toy model for mZ' = 100 GeV, three mean proper lifetimes (ctau) and the three decay modes of the Z'.

Acceptance, detection efficiency, and overall signal efficiency in the Z' toy model for mZ' = 250 GeV, three mean proper lifetimes (ctau) and the three decay modes of the Z'.

Acceptance, detection efficiency, and overall signal efficiency in the Z' toy model for mZ' = 500 GeV, three mean proper lifetimes (ctau) and the three decay modes of the Z'.

Acceptance, detection efficiency, and overall signal efficiency in the Z' toy model for mZ' = 750 GeV, three mean proper lifetimes (ctau) and the three decay modes of the Z'.

Acceptance, detection efficiency, and overall signal efficiency in the Z' toy model for mZ' = 1000 GeV, three mean proper lifetimes (ctau) and the three decay modes of the Z'.

The double-differential Z + jets production cross-section as a function of |y_{jet}| in the 100 GeV < p_{T}^{jet} < 200 GeV range. The particle level phase space definition: - 66 GeV < m_{ee} < 116 GeV - |eta_{electron}| < 2.47 - p_{T}^{electron} > 20 GeV - anti-kt R=0.4 jets N>=1 - |y_{jet}| < 3.4 - p_{T}^{jet} > 25 GeV - Delta R(jet, electron) > 0.4

The double-differential Z + jets production cross-section as a function of |y_{jet}| in the 200 GeV < p_{T}^{jet} < 300 GeV range. The particle level phase space definition: - 66 GeV < m_{ee} < 116 GeV - |eta_{electron}| < 2.47 - p_{T}^{electron} > 20 GeV - anti-kt R=0.4 jets N>=1 - |y_{jet}| < 3.4 - p_{T}^{jet} > 25 GeV - Delta R(jet, electron) > 0.4

The double-differential Z + jets production cross-section as a function of |y_{jet}| in the 300 GeV < p_{T}^{jet} < 400 Gev range. The particle level phase space definition: - 66 GeV < m_{ee} < 116 GeV - |eta_{electron}| < 2.47 - p_{T}^{electron} > 20 GeV - anti-kt R=0.4 jets N>=1 - |y_{jet}| < 3.4 - p_{T}^{jet} > 25 GeV - Delta R(jet, electron) > 0.4

The double-differential Z + jets production cross-section as a function of |y_{jet}| in the 400 GeV < p_{T}^{jet} < 1050 GeV range. The particle level phase space definition: - 66 GeV < m_{ee} < 116 GeV - |eta_{electron}| < 2.47 - p_{T}^{electron} > 20 GeV - anti-kt R=0.4 jets N>=1 - |y_{jet}| < 3.4 - p_{T}^{jet} > 25 GeV - Delta R(jet, electron) > 0.4

The non-perturbative correction for the Z + jets production cross-section as a function of |y_{jet}| in the 25 GeV < p_{T}^{jet} < 50 GeV range. The particle level phase space definition: - 66 GeV < m_{ee} < 116 GeV - |eta_{electron}| < 2.47 - p_{T}^{electron} > 20 GeV - anti-kt R=0.4 jets N>=1 - |y_{jet}| < 3.4 - p_{T}^{jet} > 25 GeV - Delta R(jet, electron) > 0.4

The non-perturbative correction for the Z + jets production cross-section as a function of |y_{jet}| in the 50 GeV < p_{T}^{jet} < 100 GeV range. The particle level phase space definition: - 66 GeV < m_{ee} < 116 GeV - |eta_{electron}| < 2.47 - p_{T}^{electron} > 20 GeV - anti-kt R=0.4 jets N>=1 - |y_{jet}| < 3.4 - p_{T}^{jet} > 25 GeV - Delta R(jet, electron) > 0.4

The non-perturbative correction for the Z + jets production cross-section as a function of |y_{jet}| in the 100 GeV < p_{T}^{jet} < 200 GeV range. The particle level phase space definition: - 66 GeV < m_{ee} < 116 GeV - |eta_{electron}| < 2.47 - p_{T}^{electron} > 20 GeV - anti-kt R=0.4 jets N>=1 - |y_{jet}| < 3.4 - p_{T}^{jet} > 25 GeV - Delta R(jet, electron) > 0.4

The non-perturbative correction for the Z + jets production cross-section as a function of |y_{jet}| in the 200 GeV < p_{T}^{jet} < 300 GeV range. The particle level phase space definition: - 66 GeV < m_{ee} < 116 GeV - |eta_{electron}| < 2.47 - p_{T}^{electron} > 20 GeV - anti-kt R=0.4 jets N>=1 - |y_{jet}| < 3.4 - p_{T}^{jet} > 25 GeV - Delta R(jet, electron) > 0.4

The non-perturbative correction for the Z + jets production cross-section as a function of |y_{jet}| in the 300 GeV < p_{T}^{jet} < 400 Gev range. The particle level phase space definition: - 66 GeV < m_{ee} < 116 GeV - |eta_{electron}| < 2.47 - p_{T}^{electron} > 20 GeV - anti-kt R=0.4 jets N>=1 - |y_{jet}| < 3.4 - p_{T}^{jet} > 25 GeV - Delta R(jet, electron) > 0.4

The non-perturbative correction for the Z + jets production cross-section as a function of |y_{jet}| in the 400 GeV < p_{T}^{jet} < 1050 GeV range. The particle level phase space definition: - 66 GeV < m_{ee} < 116 GeV - |eta_{electron}| < 2.47 - p_{T}^{electron} > 20 GeV - anti-kt R=0.4 jets N>=1 - |y_{jet}| < 3.4 - p_{T}^{jet} > 25 GeV - Delta R(jet, electron) > 0.4

The correction for QED radiation effects for the Z + jets production cross-section as a function of |y_{jet}| in the 25 GeV < p_{T}^{jet} < 50 GeV range. The particle level phase space definition: - 66 GeV < m_{ee} < 116 GeV - |eta_{electron}| < 2.47 - p_{T}^{electron} > 20 GeV - anti-kt R=0.4 jets N>=1 - |y_{jet}| < 3.4 - p_{T}^{jet} > 25 GeV - Delta R(jet, electron) > 0.4

The correction for QED radiation effects for the Z + jets production cross-section as a function of |y_{jet}| in the 50 GeV < p_{T}^{jet} < 100 GeV range. The particle level phase space definition: - 66 GeV < m_{ee} < 116 GeV - |eta_{electron}| < 2.47 - p_{T}^{electron} > 20 GeV - anti-kt R=0.4 jets N>=1 - |y_{jet}| < 3.4 - p_{T}^{jet} > 25 GeV - Delta R(jet, electron) > 0.4

The correction for QED radiation effects for the Z + jets production cross-section as a function of |y_{jet}| in the 100 GeV < p_{T}^{jet} < 200 GeV range. The particle level phase space definition: - 66 GeV < m_{ee} < 116 GeV - |eta_{electron}| < 2.47 - p_{T}^{electron} > 20 GeV - anti-kt R=0.4 jets N>=1 - |y_{jet}| < 3.4 - p_{T}^{jet} > 25 GeV - Delta R(jet, electron) > 0.4

The correction for QED radiation effects for the Z + jets production cross-section as a function of |y_{jet}| in the 200 GeV < p_{T}^{jet} < 300 GeV range. The particle level phase space definition: - 66 GeV < m_{ee} < 116 GeV - |eta_{electron}| < 2.47 - p_{T}^{electron} > 20 GeV - anti-kt R=0.4 jets N>=1 - |y_{jet}| < 3.4 - p_{T}^{jet} > 25 GeV - Delta R(jet, electron) > 0.4

The correction for QED radiation effects for the Z + jets production cross-section as a function of |y_{jet}| in the 300 GeV < p_{T}^{jet} < 400 Gev range. The particle level phase space definition: - 66 GeV < m_{ee} < 116 GeV - |eta_{electron}| < 2.47 - p_{T}^{electron} > 20 GeV - anti-kt R=0.4 jets N>=1 - |y_{jet}| < 3.4 - p_{T}^{jet} > 25 GeV - Delta R(jet, electron) > 0.4

The correction for QED radiation effects for the Z + jets production cross-section as a function of |y_{jet}| in the 400 GeV < p_{T}^{jet} < 1050 GeV range. The particle level phase space definition: - 66 GeV < m_{ee} < 116 GeV - |eta_{electron}| < 2.47 - p_{T}^{electron} > 20 GeV - anti-kt R=0.4 jets N>=1 - |y_{jet}| < 3.4 - p_{T}^{jet} > 25 GeV - Delta R(jet, electron) > 0.4

Correlation matrix for the bins of the Z + jets cross-section. The particle level phase space definition: - 66 GeV < m_{ee} < 116 GeV - |eta_{electron}| < 2.47 - p_{T}^{electron} > 20 GeV - anti-kt R=0.4 jets N>=1 - |y_{jet}| < 3.4 - p_{T}^{jet} > 25 GeV - Delta R(jet, electron) > 0.4

The $c_{k}$ for the 0.3-2 GeV $p_{T}$ range as a function of event multiplicity $N_{ch}$ in p+Pb collisions.

The $c_{k}$ for the 0.3-5 GeV $p_{T}$ range as a function of event multiplicity $N_{ch}$ in p+Pb collisions.

The $c_{k}$ for the 0.5-2 GeV $p_{T}$ range as a function of event multiplicity $N_{ch}$ in p+Pb collisions.

The $Var(v_{2}^{2})_{dyn}$ for Pb+Pb collisions for the $p_T$ 0.5-2 GeV interval as a function $N_{ch}$.

The $Var(v_{2}^{2})_{dyn}$ for Pb+Pb collisions for the $p_T$ 0.5-5 GeV interval as a function $N_{ch}$.

The $Var(v_{2}^{2})_{dyn}$ for Pb+Pb collisions for the $p_T$ 1-2 GeV interval as a function $N_{ch}$.

The $Var(v_{3}^{2})_{dyn}$ for Pb+Pb collisions for the $p_T$ 0.5-2 GeV interval as a function $N_{ch}$.

The $Var(v_{3}^{2})_{dyn}$ for Pb+Pb collisions for the $p_T$ 0.5-5 GeV interval as a function $N_{ch}$.

The $Var(v_{3}^{2})_{dyn}$ for Pb+Pb collisions for the $p_T$ 1-2 GeV interval as a function $N_{ch}$.

The $Var(v_{4}^{2})_{dyn}$ for Pb+Pb collisions for the $p_T$ 0.5-2 GeV interval as a function $N_{ch}$.

The $Var(v_{4}^{2})_{dyn}$ for Pb+Pb collisions for the $p_T$ 0.5-5 GeV interval as a function $N_{ch}$.

The $Var(v_{4}^{2})_{dyn}$ for Pb+Pb collisions for the $p_T$ 1-2 GeV interval as a function $N_{ch}$.

The $Var(v_{2}^{2})_{dyn}$ for p+Pb collisions for the $p_T$ 0.3-2 GeV interval as a function $N_{ch}$.

The $Var(v_{2}^{2})_{dyn}$ for p+Pb collisions for the $p_T$ 0.3-5 GeV interval as a function $N_{ch}$.

The $Var(v_{2}^{2})_{dyn}$ for p+Pb collisions for the $p_T$ 0.5-2 GeV interval as a function $N_{ch}$.

The $cov(v_{2}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-2 GeV interval as a function $N_{ch}$.

The $cov(v_{2}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-5 GeV interval as a function $N_{ch}$.

The $cov(v_{2}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 1-2 GeV interval as a function $N_{ch}$.

The $cov(v_{3}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-2 GeV interval as a function $N_{ch}$.

The $cov(v_{3}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-5 GeV interval as a function $N_{ch}$.

The $cov(v_{3}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 1-2 GeV interval as a function $N_{ch}$.

The $cov(v_{4}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-2 GeV interval as a function $N_{ch}$.

The $cov(v_{4}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-5 GeV interval as a function $N_{ch}$.

The $cov(v_{4}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 1-2 GeV interval as a function $N_{ch}$.

The $cov(v_{2}^{2},[p_{T}])$ for p+Pb collisions for the $p_T$ 0.3-2 GeV interval as a function $N_{ch}$.

The $cov(v_{2}^{2},[p_{T}])$ for p+Pb collisions for the $p_T$ 0.3-5 GeV interval as a function $N_{ch}$.

The $cov(v_{2}^{2},[p_{T}])$ for p+Pb collisions for the $p_T$ 0.5-2 GeV interval as a function $N_{ch}$.

The $\rho(v_{2}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-2 GeV interval as a function $N_{ch}$.

The $\rho(v_{2}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-5 GeV interval as a function $N_{ch}$.

The $\rho(v_{2}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 1-2 GeV interval as a function $N_{ch}$.

The $\rho(v_{3}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-2 GeV interval as a function $N_{ch}$.

The $\rho(v_{3}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-5 GeV interval as a function $N_{ch}$.

The $\rho(v_{3}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 1-2 GeV interval as a function $N_{ch}$.

The $\rho(v_{4}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-2 GeV interval as a function $N_{ch}$.

The $\rho(v_{4}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-5 GeV interval as a function $N_{ch}$.

The $\rho(v_{4}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 1-2 GeV interval as a function $N_{ch}$.

The $\rho(v_{2}^{2},[p_{T}])$ for p+Pb collisions for the $p_T$ 0.3-2 GeV interval as a function $N_{ch}$.

The $\rho(v_{2}^{2},[p_{T}])$ for p+Pb collisions for the $p_T$ 0.3-5 GeV interval as a function $N_{ch}$.

The $\rho(v_{2}^{2},[p_{T}])$ for p+Pb collisions for the $p_T$ 0.5-2 GeV interval as a function $N_{ch}$.

The $\rho(v_{2}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-2 GeV interval as a function $N_{part}$.

The $\rho(v_{2}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-5 GeV interval as a function $N_{part}$.

The $\rho(v_{2}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 1-2 GeV interval as a function $N_{part}$.

The $\rho(v_{3}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-2 GeV interval as a function $N_{part}$.

The $\rho(v_{3}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-5 GeV interval as a function $N_{part}$.

The $\rho(v_{3}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 1-2 GeV interval as a function $N_{part}$.

The $\rho(v_{4}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-2 GeV interval as a function $N_{part}$.

The $\rho(v_{4}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-5 GeV interval as a function $N_{part}$.

The $\rho(v_{4}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 1-2 GeV interval as a function $N_{part}$.

Measured fiducial cross section times leptonic branching ratio for W- production in the W- -> mu- nu final state.

Measured fiducial cross section times leptonic branching ratio for Z/gamma* production in the Z/gamma* -> e+ e- final state.

Measured fiducial cross section times leptonic branching ratio for Z/gamma* production in the Z/gamma* -> mu+ mu- final state.

Measured total cross section times leptonic branching ratio for W+ production in the W+ -> e+ nu final state.

Measured total cross section times leptonic branching ratio for W+ production in the W+ -> mu+ nu final state.

Measured total cross section times leptonic branching ratio for W- production in the W- -> e- nu final state.

Measured total cross section times leptonic branching ratio for W- production in the W- -> mu- nu final state.

Measured total cross section times leptonic branching ratio for Z/gamma* production in the Z/gamma* -> e+ e- final state.

Measured total cross section times leptonic branching ratio for Z/gamma* production in the Z/gamma* -> mu+ mu- final state.

Combined fiducial cross-section measurements for W+ boson production in the W+ -> l+ nu (l = e, mu) final state.

Combined fiducial cross-section measurements for W- boson production in the W- -> l- nu (l = e, mu) final state.

Combined fiducial cross-section measurements for W boson production in the W -> l nu (l = e, mu) final state.

Combined fiducial cross-section measurements for Z/gamma* production in the Z/gamma* -> l- l+ (l = e, mu) final state.

Combined total cross-section measurements for W+ boson production in the W+ -> l+ nu (l = e, mu) final state.

Combined total cross-section measurements for W- boson production in the W- -> l- nu (l = e, mu) final state.

Combined total cross-section measurements for W boson production in the W -> l nu (l = e, mu) final state.

Combined total cross-section measurements for Z/gamma* production in the Z/gamma* -> l- l+ (l = e, mu) final state.

Measured fiducial cross-section ratio R_{W+-/Z} = sigma (W+/- -> l+/- nu/nubar) / sigma (Z/gamma^* -> l+ l-) where l = e, mu.

Measured fiducial cross-section ratio R_{W+/W-} = sigma (W+ -> l+ nu) / sigma (W- -> l- nubar) where l = e, mu.

Measured charge asymmetry in W-boson production A_{l} = ( sigma (W+ -> l+ nu) - sigma (W- -> l- nubar) ) / ( sigma (W+ -> l+ nu) + sigma (W- -> l- nubar) ) where l = e, mu.

The ratio of measured W+ cross-sections in the electron and muon decay channels R_{W+} = sigma (W+ -> e+ nu) / sigma (W+ -> mu+ nu)

The ratio of measured W- cross-sections in the electron and muon decay channels R_{W-} = sigma (W- -> e- nu) / sigma (W- -> mu- nu)

The ratio of measured W cross-sections in the electron and muon decay channels R_{W} = sigma (W -> e nu) / sigma (W -> mu nu)

The ratio of measured Z/gamma^* cross-sections in the electron and muon decay channels R_{Z/gamma^*} = sigma (Z/gamma^* -> e+ e-) / sigma (Z/gamma^* -> mu+ mu-)

Correlation coefficients among (W- -> l- nubar), (W+ -> l+ nu), (Z/gamma^* -> l+ l-) where (l = e, mu) excluding the common normalisation uncertainty due to the luminosity calibration.

$\langle \zeta \rangle$, central jet.

$\langle p_{T}^{rel} / GeV \rangle$, forward jet.

$\langle p_{T}^{rel} / GeV \rangle$, central jet.

$\langle r \rangle$, forward jet.

$\langle r \rangle$, central jet.

$\langle n_{ch} \rangle$, both jets.

$\langle \zeta \rangle$, combined jet.

$\langle p_{T}^{rel} / GeV \rangle$, both jets.

$\langle r \rangle$, both jets.

$n_{ch}$ , 100 GeV < Jet p_{T} < 200 GeV, both jets.

$n_{ch}$ , 200 GeV < Jet p_{T} < 300 GeV, both jets.

$n_{ch}$ , 300 GeV < Jet p_{T} < 400 GeV, both jets.

$n_{ch}$ , 400 GeV < Jet p_{T} < 500 GeV, both jets.

$n_{ch}$ , 500 GeV < Jet p_{T} < 600 GeV, both jets.

$n_{ch}$ , 600 GeV < Jet p_{T} < 700 GeV, both jets.

$n_{ch}$ , 700 GeV < Jet p_{T} < 800 GeV, both jets.

$n_{ch}$ , 800 GeV < Jet p_{T} < 900 GeV, both jets.

$n_{ch}$ , 900 GeV < Jet p_{T} < 1000 GeV, both jets.

$n_{ch}$ , 1000 GeV < Jet p_{T} < 1200 GeV, both jets.

$n_{ch}$ , 1200 GeV < Jet p_{T} < 1400 GeV, both jets.

$n_{ch}$ , 1400 GeV < Jet p_{T} < 1600 GeV, both jets.

$n_{ch}$ , 1600 GeV < Jet p_{T} < 2000 GeV, both jets.

$n_{ch}$ , 2000 GeV < Jet p_{T} < 2500 GeV, both jets.

$r$ , 100 GeV < Jet p_{T} < 200 GeV, both jets.

$r$ , 200 GeV < Jet p_{T} < 300 GeV, both jets.

$r$ , 300 GeV < Jet p_{T} < 400 GeV, both jets.

$r$ , 400 GeV < Jet p_{T} < 500 GeV, both jets.

$r$ , 500 GeV < Jet p_{T} < 600 GeV, both jets.

$r$ , 600 GeV < Jet p_{T} < 700 GeV, both jets.

$r$ , 700 GeV < Jet p_{T} < 800 GeV, both jets.

$r$ , 800 GeV < Jet p_{T} < 900 GeV, both jets.

$r$ , 900 GeV < Jet p_{T} < 1000 GeV, both jets.

$r$ , 1000 GeV < Jet p_{T} < 1200 GeV, both jets.

$r$ , 1200 GeV < Jet p_{T} < 1400 GeV, both jets.

$r$ , 1400 GeV < Jet p_{T} < 1600 GeV, both jets.

$r$ , 1600 GeV < Jet p_{T} < 2000 GeV, both jets.

$r$ , 2000 GeV < Jet p_{T} < 2500 GeV, both jets.

$\zeta$ , 100 GeV < Jet p_{T} < 200 GeV, both jets.

$\zeta$ , 200 GeV < Jet p_{T} < 300 GeV, both jets.

$\zeta$ , 300 GeV < Jet p_{T} < 400 GeV, both jets.

$\zeta$ , 400 GeV < Jet p_{T} < 500 GeV, both jets.

$\zeta$ , 500 GeV < Jet p_{T} < 600 GeV, both jets.

$\zeta$ , 600 GeV < Jet p_{T} < 700 GeV, both jets.

$\zeta$ , 700 GeV < Jet p_{T} < 800 GeV, both jets.

$\zeta$ , 800 GeV < Jet p_{T} < 900 GeV, both jets.

$\zeta$ , 900 GeV < Jet p_{T} < 1000 GeV, both jets.

$\zeta$ , 1000 GeV < Jet p_{T} < 1200 GeV, both jets.

$\zeta$ , 1200 GeV < Jet p_{T} < 1400 GeV, both jets.

$\zeta$ , 1400 GeV < Jet p_{T} < 1600 GeV, both jets.

$\zeta$ , 1600 GeV < Jet p_{T} < 2000 GeV, both jets.

$\zeta$ , 2000 GeV < Jet p_{T} < 2500 GeV, both jets.

$p_{T}^{rel} / GeV$ , 100 GeV < Jet p_{T} < 200 GeV, both jets.

$p_{T}^{rel} / GeV$ , 200 GeV < Jet p_{T} < 300 GeV, both jets.

$p_{T}^{rel} / GeV$ , 300 GeV < Jet p_{T} < 400 GeV, both jets.

$p_{T}^{rel} / GeV$ , 400 GeV < Jet p_{T} < 500 GeV, both jets.

$p_{T}^{rel} / GeV$ , 500 GeV < Jet p_{T} < 600 GeV, both jets.

$p_{T}^{rel} / GeV$ , 600 GeV < Jet p_{T} < 700 GeV, both jets.

$p_{T}^{rel} / GeV$ , 700 GeV < Jet p_{T} < 800 GeV, both jets.

$p_{T}^{rel} / GeV$ , 800 GeV < Jet p_{T} < 900 GeV, both jets.

$p_{T}^{rel} / GeV$ , 900 GeV < Jet p_{T} < 1000 GeV, both jets.

$p_{T}^{rel} / GeV$ , 1000 GeV < Jet p_{T} < 1200 GeV, both jets.

$p_{T}^{rel} / GeV$ , 1200 GeV < Jet p_{T} < 1400 GeV, both jets.

$p_{T}^{rel} / GeV$ , 1400 GeV < Jet p_{T} < 1600 GeV, both jets.

$p_{T}^{rel} / GeV$ , 1600 GeV < Jet p_{T} < 2000 GeV, both jets.

$p_{T}^{rel} / GeV$ , 2000 GeV < Jet p_{T} < 2500 GeV, both jets.

$n_{ch}$ , 100 GeV < Jet p_{T} < 200 GeV, more forward jet.

$n_{ch}$ , 200 GeV < Jet p_{T} < 300 GeV, more forward jet.

$n_{ch}$ , 300 GeV < Jet p_{T} < 400 GeV, more forward jet.

$n_{ch}$ , 400 GeV < Jet p_{T} < 500 GeV, more forward jet.

$n_{ch}$ , 500 GeV < Jet p_{T} < 600 GeV, more forward jet.

$n_{ch}$ , 600 GeV < Jet p_{T} < 700 GeV, more forward jet.

$n_{ch}$ , 700 GeV < Jet p_{T} < 800 GeV, more forward jet.

$n_{ch}$ , 800 GeV < Jet p_{T} < 900 GeV, more forward jet.

$n_{ch}$ , 900 GeV < Jet p_{T} < 1000 GeV, more forward jet.

$n_{ch}$ , 1000 GeV < Jet p_{T} < 1200 GeV, more forward jet.

$n_{ch}$ , 1200 GeV < Jet p_{T} < 1400 GeV, more forward jet.

$n_{ch}$ , 1400 GeV < Jet p_{T} < 1600 GeV, more forward jet.

$n_{ch}$ , 1600 GeV < Jet p_{T} < 2000 GeV, more forward jet.

$n_{ch}$ , 2000 GeV < Jet p_{T} < 2500 GeV, more forward jet.

$r$ , 100 GeV < Jet p_{T} < 200 GeV, more forward jet.

$r$ , 200 GeV < Jet p_{T} < 300 GeV, more forward jet.

$r$ , 300 GeV < Jet p_{T} < 400 GeV, more forward jet.

$r$ , 400 GeV < Jet p_{T} < 500 GeV, more forward jet.

$r$ , 500 GeV < Jet p_{T} < 600 GeV, more forward jet.

$r$ , 600 GeV < Jet p_{T} < 700 GeV, more forward jet.

$r$ , 700 GeV < Jet p_{T} < 800 GeV, more forward jet.

$r$ , 800 GeV < Jet p_{T} < 900 GeV, more forward jet.

$r$ , 900 GeV < Jet p_{T} < 1000 GeV, more forward jet.

$r$ , 1000 GeV < Jet p_{T} < 1200 GeV, more forward jet.

$r$ , 1200 GeV < Jet p_{T} < 1400 GeV, more forward jet.

$r$ , 1400 GeV < Jet p_{T} < 1600 GeV, more forward jet.

$r$ , 1600 GeV < Jet p_{T} < 2000 GeV, more forward jet.

$r$ , 2000 GeV < Jet p_{T} < 2500 GeV, more forward jet.

$\zeta$ , 100 GeV < Jet p_{T} < 200 GeV, more forward jet.

$\zeta$ , 200 GeV < Jet p_{T} < 300 GeV, more forward jet.

$\zeta$ , 300 GeV < Jet p_{T} < 400 GeV, more forward jet.

$\zeta$ , 400 GeV < Jet p_{T} < 500 GeV, more forward jet.

$\zeta$ , 500 GeV < Jet p_{T} < 600 GeV, more forward jet.

$\zeta$ , 600 GeV < Jet p_{T} < 700 GeV, more forward jet.

$\zeta$ , 700 GeV < Jet p_{T} < 800 GeV, more forward jet.

$\zeta$ , 800 GeV < Jet p_{T} < 900 GeV, more forward jet.

$\zeta$ , 900 GeV < Jet p_{T} < 1000 GeV, more forward jet.

$\zeta$ , 1000 GeV < Jet p_{T} < 1200 GeV, more forward jet.

$\zeta$ , 1200 GeV < Jet p_{T} < 1400 GeV, more forward jet.

$\zeta$ , 1400 GeV < Jet p_{T} < 1600 GeV, more forward jet.

$\zeta$ , 1600 GeV < Jet p_{T} < 2000 GeV, more forward jet.

$\zeta$ , 2000 GeV < Jet p_{T} < 2500 GeV, more forward jet.

$p_{T}^{rel} / GeV$ , 100 GeV < Jet p_{T} < 200 GeV, more forward jet.

$p_{T}^{rel} / GeV$ , 200 GeV < Jet p_{T} < 300 GeV, more forward jet.

$p_{T}^{rel} / GeV$ , 300 GeV < Jet p_{T} < 400 GeV, more forward jet.

$p_{T}^{rel} / GeV$ , 400 GeV < Jet p_{T} < 500 GeV, more forward jet.

$p_{T}^{rel} / GeV$ , 500 GeV < Jet p_{T} < 600 GeV, more forward jet.

$p_{T}^{rel} / GeV$ , 600 GeV < Jet p_{T} < 700 GeV, more forward jet.

$p_{T}^{rel} / GeV$ , 700 GeV < Jet p_{T} < 800 GeV, more forward jet.

$p_{T}^{rel} / GeV$ , 800 GeV < Jet p_{T} < 900 GeV, more forward jet.

$p_{T}^{rel} / GeV$ , 900 GeV < Jet p_{T} < 1000 GeV, more forward jet.

$p_{T}^{rel} / GeV$ , 1000 GeV < Jet p_{T} < 1200 GeV, more forward jet.

$p_{T}^{rel} / GeV$ , 1200 GeV < Jet p_{T} < 1400 GeV, more forward jet.

$p_{T}^{rel} / GeV$ , 1400 GeV < Jet p_{T} < 1600 GeV, more forward jet.

$p_{T}^{rel} / GeV$ , 1600 GeV < Jet p_{T} < 2000 GeV, more forward jet.

$p_{T}^{rel} / GeV$ , 2000 GeV < Jet p_{T} < 2500 GeV, more forward jet.

$n_{ch}$ , 100 GeV < Jet p_{T} < 200 GeV, more central jet.

$n_{ch}$ , 200 GeV < Jet p_{T} < 300 GeV, more central jet.

$n_{ch}$ , 300 GeV < Jet p_{T} < 400 GeV, more central jet.

$n_{ch}$ , 400 GeV < Jet p_{T} < 500 GeV, more central jet.

$n_{ch}$ , 500 GeV < Jet p_{T} < 600 GeV, more central jet.

$n_{ch}$ , 600 GeV < Jet p_{T} < 700 GeV, more central jet.

$n_{ch}$ , 700 GeV < Jet p_{T} < 800 GeV, more central jet.

$n_{ch}$ , 800 GeV < Jet p_{T} < 900 GeV, more central jet.

$n_{ch}$ , 900 GeV < Jet p_{T} < 1000 GeV, more central jet.

$n_{ch}$ , 1000 GeV < Jet p_{T} < 1200 GeV, more central jet.

$n_{ch}$ , 1200 GeV < Jet p_{T} < 1400 GeV, more central jet.

$n_{ch}$ , 1400 GeV < Jet p_{T} < 1600 GeV, more central jet.

$n_{ch}$ , 1600 GeV < Jet p_{T} < 2000 GeV, more central jet.

$n_{ch}$ , 2000 GeV < Jet p_{T} < 2500 GeV, more central jet.

$r$ , 100 GeV < Jet p_{T} < 200 GeV, more central jet.

$r$ , 200 GeV < Jet p_{T} < 300 GeV, more central jet.

$r$ , 300 GeV < Jet p_{T} < 400 GeV, more central jet.

$r$ , 400 GeV < Jet p_{T} < 500 GeV, more central jet.

$r$ , 500 GeV < Jet p_{T} < 600 GeV, more central jet.

$r$ , 600 GeV < Jet p_{T} < 700 GeV, more central jet.

$r$ , 700 GeV < Jet p_{T} < 800 GeV, more central jet.

$r$ , 800 GeV < Jet p_{T} < 900 GeV, more central jet.

$r$ , 900 GeV < Jet p_{T} < 1000 GeV, more central jet.

$r$ , 1000 GeV < Jet p_{T} < 1200 GeV, more central jet.

$r$ , 1200 GeV < Jet p_{T} < 1400 GeV, more central jet.

$r$ , 1400 GeV < Jet p_{T} < 1600 GeV, more central jet.

$r$ , 1600 GeV < Jet p_{T} < 2000 GeV, more central jet.

$r$ , 2000 GeV < Jet p_{T} < 2500 GeV, more central jet.

$\zeta$ , 100 GeV < Jet p_{T} < 200 GeV, more central jet.

$\zeta$ , 200 GeV < Jet p_{T} < 300 GeV, more central jet.

$\zeta$ , 300 GeV < Jet p_{T} < 400 GeV, more central jet.

$\zeta$ , 400 GeV < Jet p_{T} < 500 GeV, more central jet.

$\zeta$ , 500 GeV < Jet p_{T} < 600 GeV, more central jet.

$\zeta$ , 600 GeV < Jet p_{T} < 700 GeV, more central jet.

$\zeta$ , 700 GeV < Jet p_{T} < 800 GeV, more central jet.

$\zeta$ , 800 GeV < Jet p_{T} < 900 GeV, more central jet.

$\zeta$ , 900 GeV < Jet p_{T} < 1000 GeV, more central jet.

$\zeta$ , 1000 GeV < Jet p_{T} < 1200 GeV, more central jet.

$\zeta$ , 1200 GeV < Jet p_{T} < 1400 GeV, more central jet.

$\zeta$ , 1400 GeV < Jet p_{T} < 1600 GeV, more central jet.

$\zeta$ , 1600 GeV < Jet p_{T} < 2000 GeV, more central jet.

$\zeta$ , 2000 GeV < Jet p_{T} < 2500 GeV, more central jet.

$p_{T}^{rel} / GeV$ , 100 GeV < Jet p_{T} < 200 GeV, more central jet.

$p_{T}^{rel} / GeV$ , 200 GeV < Jet p_{T} < 300 GeV, more central jet.

$p_{T}^{rel} / GeV$ , 300 GeV < Jet p_{T} < 400 GeV, more central jet.

$p_{T}^{rel} / GeV$ , 400 GeV < Jet p_{T} < 500 GeV, more central jet.

$p_{T}^{rel} / GeV$ , 500 GeV < Jet p_{T} < 600 GeV, more central jet.

$p_{T}^{rel} / GeV$ , 600 GeV < Jet p_{T} < 700 GeV, more central jet.

$p_{T}^{rel} / GeV$ , 700 GeV < Jet p_{T} < 800 GeV, more central jet.

$p_{T}^{rel} / GeV$ , 800 GeV < Jet p_{T} < 900 GeV, more central jet.

$p_{T}^{rel} / GeV$ , 900 GeV < Jet p_{T} < 1000 GeV, more central jet.

$p_{T}^{rel} / GeV$ , 1000 GeV < Jet p_{T} < 1200 GeV, more central jet.

$p_{T}^{rel} / GeV$ , 1200 GeV < Jet p_{T} < 1400 GeV, more central jet.

$p_{T}^{rel} / GeV$ , 1400 GeV < Jet p_{T} < 1600 GeV, more central jet.

$p_{T}^{rel} / GeV$ , 1600 GeV < Jet p_{T} < 2000 GeV, more central jet.

$p_{T}^{rel} / GeV$ , 2000 GeV < Jet p_{T} < 2500 GeV, more central jet.

The total uncertainty covariance matrix for the average number of tracks per jet $p_T$ bin. The covariance matrix is the sum of the covariance matrices for each source of systematic and statistical uncertainty. Note that the overall sign for the systematic uncertainty covariances is arbitrary.

The total uncertainty covariance matrix for the average fragmentation function per jet $p_T$ bin. The covariance matrix is the sum of the covariance matrices for each source of systematic and statistical uncertainty. Note that the overall sign for the systematic uncertainty covariances is arbitrary.

The total uncertainty covariance matrix for the average relative $p_T$ per jet $p_T$ bin. The covariance matrix is the sum of the covariance matrices for each source of systematic and statistical uncertainty. Note that the overall sign for the systematic uncertainty covariances is arbitrary.

The total uncertainty covariance matrix for the average r per jet $p_T$ bin. The covariance matrix is the sum of the covariance matrices for each source of systematic and statistical uncertainty. Note that the overall sign for the systematic uncertainty covariances is arbitrary.

The total uncertainty covariance matrix for the number of tracks. The first half of the bins on a given axis correspond to the more central jet while the second half correspond to the more forward jet. See Fig. 4 in the paper for more information about the binning. The covariance matrix is the sum of the covariance matrices for each source of systematic and statistical uncertainty. Note that the overall sign for the systematic uncertainty covariances is arbitrary.

The total uncertainty covariance matrix for the fragmentation function. The first half of the bins on a given axis correspond to the more central jet while the second half correspond to the more forward jet. See Fig. 4 in the paper for more information about the binning. The covariance matrix is the sum of the covariance matrices for each source of systematic and statistical uncertainty. Note that the overall sign for the systematic uncertainty covariances is arbitrary.

The total uncertainty covariance matrix for the relative $p_T$. The first half of the bins on a given axis correspond to the more central jet while the second half correspond to the more forward jet. See Fig. 4 in the paper for more information about the binning. The covariance matrix is the sum of the covariance matrices for each source of systematic and statistical uncertainty. Note that the overall sign for the systematic uncertainty covariances is arbitrary.

The total uncertainty covariance matrix for the r. The first half of the bins on a given axis correspond to the more central jet while the second half correspond to the more forward jet. See Fig. 4 in the paper for more information about the binning. The covariance matrix is the sum of the covariance matrices for each source of systematic and statistical uncertainty. Note that the overall sign for the systematic uncertainty covariances is arbitrary.

Limit Plot

Limit Plot

Limit Plot

HVT WW Acceptance times Efficiency

HVT WZ Acceptance times Efficiency

RS Graviton WW Acceptance times Efficiency

RS Graviton ZZ Acceptance times Efficiency