Bayesian upper exclusion limits on the ratio $g_{W'}/g_{W}$ for an SSM-like W$\prime$ boson are shown. The unity coupling ratio (blue dotted curve) corresponds to the SSM common benchmark. The 68 and 95% quantiles of the limits are represented by the green and yellow bands, respectively.

Bayesian lower exclusion limits on the NUGIM G(221) mixing angle $\cot(\theta_{E})$ are shown as a function of the W$\prime$ boson mass. The theoretically excluded region is shaded in grey. The 68 and 95% quantiles of the limits are represented by the green and yellow bands, respectively.

Bayesian upper exclusion limits at 95% CL on the product of the production cross section and branching fraction of a QBH in an associated $ au$ lepton and neutrino final state. Minimum threshold masses $m_{th}$ of up to 6.6 TeV are excluded at 95% CL. The observed limit (solid line) is obtained from the intersection with the LO QBH cross section (blue dotted curve). The 68 and 95% quantiles of the limits are represented by the green and yellow bands, respectively.

Bayesian upper limits at 95% CL on the cross section of the process $pp\rightarrow\tau\nu$ mediated via LQ exchange in the t-channel. The inner (green) band and the outer (yellow) band indicate the regions containing 68 and 95%, respectively, of the distribution of limits expected under the background-only hypothesis. The predicted LQ cross section at LO in the three coupling benchmark scenarios is depicted in different colors for $g_{U}=1$. The uncertainty bandy correspond to the sum in quadrature of PDF and scale variations. The first benchmark scenario considers only couplings to left-handed SM fermions (i.e. $\beta_{\text{R}}^{ij}=0$) and is referred to as "best fit LH". The second benchmark, referred to as "best fit LH+RH", considers $|\beta_{\text{R}}^{\text{b}\tau}|=1$ and all other $\beta_{\text{R}}^{ij}=0$. In the third "democratic" benchmark, equal couplings only to LH fermions are assumed, i.e. $\beta_{\text{L}}^{ij}=1$ and $\beta_{\text{R}}^{ij}=0$ for all $i$ and $j$.

Expected and observed lower limits of the LQ mass as a function of the coupling $g_{U}$ in the LH scenario. The blue band shows the 68% and 95% regions of $g_{U}$ preferred by the fit to the b anomalies data.

Expected and observed lower limits of the LQ mass as a function of the coupling $g_{U}$ in the LH+RH scenario. The blue band shows the 68% and 95% regions of $g_{U}$ preferred by the fit to the b anomalies data.

Expected and observed lower limits of the LQ mass as a function of the coupling $g_{U}$ in the democratic scenario. The blue band shows the 68% and 95% regions of $g_{U}$ preferred by the fit to the b anomalies data.

Bayesian upper exclusion limits at 95% CL on each of the Wilson coefficients described by the EFT model based on 2016-2018 data. The three different coupling types represent a left-handed vector coupling ($\epsilon^{cb}_{L}$), tensor-like coupling ($\epsilon^{cb}_{T}$), and scalar-tensor-like coupling ($\epsilon^{cb}_{S_{L}}$). The 68 and 95% quantiles of the limits are represented by the green and yellow bands, respectively.

Summary of exclusion limits (expected and observed) calculated at 95% CL for full Run-2 CMS data.

Background prediction and observed data yields in the signal region bins. The background yields are obtained from the background-only fit and serve as input to the simplified likelihood reinterpretation scheme. The naming of the bins is "year_binnumber", following the binning from Figure 4.

Matrix of covariance coefficients between signal region bins. The coefficients are obtained from the background-only fit and serve as input to the simplified likelihood reinterpretation scheme. The naming of the bins is "year_binnumber", following the binning used in Figure 4.

Predicted signal yields for the 2017 data-taking period, corresponding to 41.3 fb$^{-1}$, after the application of each search requirement (cumulative) for various signal hypothesis. The requirements listed are presented as total efficiencies w.r.t. the previous selection step.

Upper limits on the production cross section times branching fraction of the b* RH hypothesis at a 95% CL. Dashed colored lines show the expected limits from the l+jets and all-hadronic channels, where the latter start at resonance masses of 1.4 TeV. The observed and expected limits from the combination are shown as solid and dashed black lines, respectively. The green and yellow bands show the 68 and 95% confidence intervals on the combined expected limits.

Upper limits on the production cross section times branching fraction of the b* VL hypothesis at a 95% CL. Dashed colored lines show the expected limits from the l+jets and all-hadronic channels, where the latter start at resonance masses of 1.4 TeV. The observed and expected limits from the combination are shown as solid and dashed black lines, respectively. The green and yellow bands show the 68 and 95% confidence intervals on the combined expected limits.

Upper limits on the production cross section times branching fraction of the B+b hypothesis at a 95% CL. Dashed colored lines show the expected limits from the l+jets and all-hadronic channels, where the latter start at resonance masses of 1.4 TeV. The observed and expected limits from the combination are shown as solid and dashed black lines, respectively. The green and yellow bands show the 68 and 95% confidence intervals on the combined expected limits.

Upper limits on the production cross section times branching fraction of the B+t hypothesis at a 95% CL. Dashed colored lines show the expected limits from the l+jets and all-hadronic channels, where the latter start at resonance masses of 1.4 TeV. The observed and expected limits from the combination are shown as solid and dashed black lines, respectively. The green and yellow bands show the 68 and 95% confidence intervals on the combined expected limits.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction off protons with a Soeding-inspired analytic function --- statistical correlations only. Only one half of the (symmetric) matrix is stored.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction off protons, differential in the dipion mass and in bins of $W$. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction off protons, differential in the dipion mass and in bins of $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons, in bins of the photon-proton energy $W$. The cross section is defined as the integral of the relativistic Breit Wigner resonance in the dipion mass over the range $2m_\pi<m_{\pi\pi}<1.53$ GeV. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons in bins of the photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction cross sections off protons as a function of energy. Parameters with subscript "el" and "pd" correspond to elastic and proton-dissociative cross sections, respectively.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction cross sections off protons as a function of energy --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of elastic $\rho^0(770)$ photoproduction cross section off protons as a function of energy (various experiments)

Fit of elastic $\rho^0(770)$ photoproduction cross sections off protons as a function of energy (various experiments) --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction cross section off protons, double-differential in the dipion mass and the momentum transfer $\vert t\vert$. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction cross section off protons, double-differential in the dipion mass and the momentum transfer $\vert t\vert$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons, single-differential in the momentum transfer $\vert t\vert$. The cross section is defined as the integral of the relativistic Breit Wigner resonance in the dipion mass over the range $2m_\pi<m_{\pi\pi}<1.53$ GeV. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons, single differential in the momentum transfer $\vert t\vert$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$. Parameters with subscript "el" and "pd" correspond to elastic and proton-dissociative cross sections, respectively.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction double-differenial cross section off protons, as a function of the dipion mass and the momentum transfer $\vert t\vert$, in bins of the photon-proton energy $W$ The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction double-differenial cross section off protons, as a function of the dipion mass and the momentum transfer $\vert t\vert$, in bins of the photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons, single-differential in the momentum transfer $\vert t\vert$, in bins of the photon-proton energy $W$. The cross section is defined as the integral of the relativistic Breit Wigner resonance in the dipion mass over the range $2m_\pi<m_{\pi\pi}<1.53$ GeV. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction cross section off protons, single differential in the momentum transfer $\vert t\vert$ and in bins of the photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Regge fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ and photon-proton energy $W$. Parameters with subscript "el" and "pd" correspond to elastic and proton-dissociative cross sections, respectively.

Regge fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ and photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of $b$-slopes in elastic ($m_Y=m_p$) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ in bins of photon-proton energy $W$.

Fit of $b$-slopes in elastic ($m_Y=m_p$) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ in bins of photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of Pomeron trajectories in elastic ($m_Y=m_p$) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ in bins of photon-proton energy $W$.

Fit of Pomeron trajectories in elastic ($m_Y=m_p$) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ in bins of photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

The neutral current reduced cross section at Q^2=90 GeV^2 for a proton energy of 460 GeV.

The neutral current reduced cross section at Q^2=120 GeV^2 for a proton energy of 460 GeV.

The neutral current reduced cross section at Q^2=150 GeV^2 for a proton energy of 460 GeV.

The neutral current reduced cross section at Q^2=200 GeV^2 for a proton energy of 460 GeV.

The neutral current reduced cross section at Q^2=250 GeV^2 for a proton energy of 460 GeV.

The neutral current reduced cross section at Q^2=300 GeV^2 for a proton energy of 460 GeV.

The neutral current reduced cross section at Q^2=400 GeV^2 for a proton energy of 460 GeV.

The neutral current reduced cross section at Q^2=500 GeV^2 for a proton energy of 460 GeV.

The neutral current reduced cross section at Q^2=650 GeV^2 for a proton energy of 460 GeV.

The neutral current reduced cross section at Q^2=800 GeV^2 for a proton energy of 460 GeV.

The neutral current reduced cross section at Q^2=35 GeV^2 for a proton energy of 575 GeV.

The neutral current reduced cross section at Q^2=45 GeV^2 for a proton energy of 575 GeV.

The neutral current reduced cross section at Q^2=60 GeV^2 for a proton energy of 575 GeV.

The neutral current reduced cross section at Q^2=90 GeV^2 for a proton energy of 575 GeV.

The neutral current reduced cross section at Q^2=120 GeV^2 for a proton energy of 575 GeV.

The neutral current reduced cross section at Q^2=150 GeV^2 for a proton energy of 575 GeV.

The neutral current reduced cross section at Q^2=200 GeV^2 for a proton energy of 575 GeV.

The neutral current reduced cross section at Q^2=250 GeV^2 for a proton energy of 575 GeV.

The neutral current reduced cross section at Q^2=300 GeV^2 for a proton energy of 575 GeV.

The neutral current reduced cross section at Q^2=400 GeV^2 for a proton energy of 575 GeV.

The neutral current reduced cross section at Q^2=500 GeV^2 for a proton energy of 575 GeV.

The neutral current reduced cross section at Q^2=650 GeV^2 for a proton energy of 575 GeV.

The neutral current reduced cross section at Q^2=800 GeV^2 for a proton energy of 575 GeV.

The proton structure functions FL and F2 measured at Q^2=1.5 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=2.0 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=2.5 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=3.5 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=5.0 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=6.5 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=8.5 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=12 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=15 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=20 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=25 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=35 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=45 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=60 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=90 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=120 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=150 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=200 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=250 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=300 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=400 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=500 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=650 GeV^2 as a function of X without model assumptions.

The proton structure functions FL and F2 measured at Q^2=800 GeV^2 as a function of X without model assumptions.

The proton structure function FL obtained by averaging the FL data from the previous tables.

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 W+ production in the W+ -> mu+ nu final state.

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

Measured fiducial cross section times leptonic branching ratio for W+/- production in the combined W+ -> mu+ nu and W- -> mu- nubar 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- -> e- nubar final state.

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

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

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

Measured total 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+ -> l+ nu (l = e, mu) final states.

Measured total cross section times leptonic branching ratio for W- production in the W- -> l- nubar (l = e, mu) final states.

Measured total cross section times leptonic branching ratio for W+/- production in the combined W+ -> l+ nu and W- -> l- nubar (l = e, mu) final states.

Measured total cross section times leptonic branching ratio for Z/gamma* production in the combined Z/gamma* -> l+ l- (l = e, mu) final states.

Measured total cross-section ratio R_{W+/Z} = sigma (W+ -> e+ nu) / sigma (Z/gamma^* -> e+ e-).

Measured total cross-section ratio R_{W-/Z} = sigma (W- -> e- nubar) / sigma (Z/gamma^* -> e+ e-).

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

Measured total cross-section ratio R_{W+/Z} = sigma (W+ -> mu+ nu) / sigma (Z/gamma^* -> mu+ mu-).

Measured total cross-section ratio R_{W-/Z} = sigma (W- -> mu- nubar) / sigma (Z/gamma^* -> mu+ mu-).

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

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

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

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

Measured lepton asymmetry from W+ -> e+ nu and W- -> e- nubar, binned as a function pseudorapidity.

Measured lepton asymmetry from W+ -> e+ nu and W- -> e- nubar.

Measured lepton asymmetry from W+ -> mu+ nu and W- -> mu- nubar, binned as a function pseudorapidity.

Measured lepton asymmetry from W+ -> mu+ nu and W- -> mu- nubar.

Measured lepton asymmetry from W+ -> l+ nu and W- -> l- nubar (l = e, mu), binned as a function pseudorapidity.

Measured lepton asymmetry from W+ -> l+ nu and W- -> l- nubar (l = e, mu).

Bin averaged differential cross section as a function of ET in the defined phase space.

Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range -1.00 to -0.57.

Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range -0.57 to 0.20.

Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range 0.20 to 0.94.

Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range 0.94 to 1.42.

Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range 1.42 to 2.43.

Bin averaged differential cross section for prompt photon plus jet as a function of the photon transverse energy.

Bin averaged differential cross section for prompt photon plus jet as a function of the photon pseudorapidity.

Bin averaged differential cross section for prompt photon plus jet as a function of the jet transverse energy.

Bin averaged differential cross section for prompt photon plus jet as a function of the jet pseudorapidity.

Bin averaged differential cross section for prompt photon plus jet as a function of X(C=GAMMA,LO) thelongitudinal momentum fraction of the partons in the photon in LO approximation.

Bin averaged differential cross section for prompt photon plus jet as a function of X(C=P,LO) thelongitudinal momentum fraction of the partons in the proton in LO approximation.

Bin averaged differential cross section for prompt photon plus jet as a function of the photons transverse momentum perpendicular to the jet direction separated into two regions of X(C=GAMMA,LO).

Bin averaged differential cross section for prompt photon plus jet as a function of the difference in azimuthal angle between the photon and the jet separated into two regions of X(C=GAMMA,LO).

Bin averaged hadron level differential cross section for diffractive dijet production as a function of X(C=POMERON). The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of Z(C=POMERON). The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of the average pseudorapidity of the dijet system. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of the absolute difference of the pseudorapidities of the two jets. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of W. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of the dijet invariant mass. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of mass of the diffractive system. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level double-differential cross section for diffractive dijet production as a function of X(GAMMA) for 3 ranges of ET of jet 1. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level double-differential cross section for diffractive dijet production as a function of Z(POMERON) for 2 ranges of X(GAMMA). The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of X(C=GAMMA). The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of ET of jet 1. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of the average pseudorapidity of the dijet system. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of the absolute difference in the pseudorapidities of the 2 jets. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of the invariant mass of the dijet system. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of W. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Measured differential photoproduction cross sections as a function of the squared transverse momentum of the J/PSI in 4 bins of elasticity.

Measured differential photoproduction cross sections as a function of the elasticity of the J/PSI in 4 bins of transverse momentum.

Measured differential electroproduction cross section as a function of Q**2.

Measured differential electroproduction cross section as a function of the squared transverse momentum of the J/PSI in the GAMMA* P frame.

Measured differential electroproduction cross section as a function of the elasticity of the J/PSI.

Measured differential electroproduction cross section as a function of the photon-proton centre of mass energy W.

Measured differential electroproduction cross section as a function of the squared transverse momentum of the J/PSI in the GAMMA* P rest frame.

Measured differential electroproduction cross section as a function of the squared transverse momentum of the J/PSI in the GAMMA* P rest frame.

Measured differential electroproduction cross section as a function of the squared transverse momentum of the J/PSI in the GAMMA* P rest frame.

Measured differential electroproduction cross section as a function of the elasticity of the J/PSI.

Measured differential electroproduction cross section as a function of the elasticity of the J/PSI.

Measured differential electroproduction cross section as a function of the elasticity of the J/PSI.

Measured polarization parameter in the Helicity Frame. Here ALPHA is given by DSIG/DCOS(THETA) ~ 1+ ALPHA COS(THETA)**2 and NU is given by DSIG/DPHI ~ 1+ ALPHA/3 + (NU/3)*COS(2THETA).

Measured polarization parameter in the Collins-Soper Frame. Here ALPHA is given by DSIG/DCOS(THETA) ~ 1+ ALPHA COS(THETA)**2 and NU is given by DSIG/DPHI ~ 1+ ALPHA/3 + (NU/3)*COS(2THETA).

Measured polarization parameter in the Helicity Frame. Here ALPHA is given by DSIG/DCOS(THETA) ~ 1+ ALPHA COS(THETA)**2 and NU is given by DSIG/DPHI ~ 1+ ALPHA/3 + (NU/3)*COS(2THETA).

Measured polarization parameter in the Collins-Soper Frame. Here ALPHA is given by DSIG/DCOS(THETA) ~ 1+ ALPHA COS(THETA)**2 and NU is given by DSIG/DPHI ~ 1+ ALPHA/3 + (NU/3)*COS(2THETA).

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=0.1 GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=0.15 GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=0.2 GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=0.25 GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=0.35 GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=0.4 GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=0.5 GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=0.65 GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=0.85 GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=1.2 GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=1.5 GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=2. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=2.7 GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=3.5 GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=4.5 GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=6.5 GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=8.5 GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=10. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=12. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=15. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=18. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=22. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=27. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=35. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=45. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=60. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=70. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=90. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=120. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=150. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=200. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=250. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=300. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=400. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=500. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=650. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=800. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=1000. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=1200. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=1500. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=2000. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=3000. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=5000. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=8000. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=12000. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=20000. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E+ P scattering at Q**2=30000. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=90. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=120. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=150. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=200. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=250. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=300. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=400. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=500. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=650. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=800. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=1000. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=1200. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=1500. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=2000. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=3000. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=5000. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=8000. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=12000. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=20000. GeV**2.

Combined reduced cross section data and F2 for Neutral Current E- P scattering at Q**2=30000. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E+ P scattering at Q**2=300. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E+ P scattering at Q**2=500. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E+ P scattering at Q**2=1000. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E+ P scattering at Q**2=1500. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E+ P scattering at Q**2=2000. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E+ P scattering at Q**2=3000. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E+ P scattering at Q**2=5000. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E+ P scattering at Q**2=8000. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E+ P scattering at Q**2=15000. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E- P scattering at Q**2=300. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E- P scattering at Q**2=500. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E- P scattering at Q**2=1000. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E- P scattering at Q**2=1500. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E- P scattering at Q**2=2000. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E- P scattering at Q**2=3000. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E- P scattering at Q**2=5000. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E- P scattering at Q**2=8000. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E- P scattering at Q**2=15000. GeV**2.

Combined double differential cross section and reduced cross section data for Charged Current E- P scattering at Q**2=30000. GeV**2.