Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.56<|\eta^{\gamma}|<1.81$ and photon isolation cone radius $R=0.4$.

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.81<|\eta^{\gamma}|<2.01$ and photon isolation cone radius $R=0.4$.

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $2.01<|\eta^{\gamma}|<2.37$ and photon isolation cone radius $R=0.4$.

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $|\eta^{\gamma}|<0.6$ and photon isolation cone radius $R=0.2$.

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $0.6<|\eta^{\gamma}|<0.8$ and photon isolation cone radius $R=0.2$.

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $0.8<|\eta^{\gamma}|<1.37$ and photon isolation cone radius $R=0.2$.

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.56<|\eta^{\gamma}|<1.81$ and photon isolation cone radius $R=0.2$.

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.81<|\eta^{\gamma}|<2.01$ and photon isolation cone radius $R=0.2$.

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $2.01<|\eta^{\gamma}|<2.37$ and photon isolation cone radius $R=0.2$.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $|\eta^{\gamma}|<0.6$ and isolation cone radius $0.4$ at NNLO QCD.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $0.6<|\eta^{\gamma}|<0.8$ and isolation cone radius $0.4$ at NNLO QCD.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $0.8<|\eta^{\gamma}|<1.37$ and isolation cone radius $0.4$ at NNLO QCD.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.56<|\eta^{\gamma}|<1.81$ and isolation cone radius $0.4$ at NNLO QCD.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.81<|\eta^{\gamma}|<2.01$ and isolation cone radius $0.4$ at NNLO QCD.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $2.01<|\eta^{\gamma}|<2.37$ and isolation cone radius $0.4$ at NNLO QCD.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $|\eta^{\gamma}|<0.6$ and isolation cone radius $0.2$ at NNLO QCD.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $0.6<|\eta^{\gamma}|<0.8$ and isolation cone radius $0.2$ at NNLO QCD.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $0.8<|\eta^{\gamma}|<1.37$ and isolation cone radius $0.2$ at NNLO QCD.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.56<|\eta^{\gamma}|<1.81$ and isolation cone radius $0.2$ at NNLO QCD.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.81<|\eta^{\gamma}|<2.01$ and isolation cone radius $0.2$ at NNLO QCD.

Predicted cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $2.01<|\eta^{\gamma}|<2.37$ and isolation cone radius $0.2$ at NNLO QCD.

Measured ratio of the differential cross sections for inclusive isolated-photon production for $R=0.2$ and $R=0.4$ as a function of $E_{\rm T}^{\gamma}$ for $|\eta^{\gamma}|<0.6$.

Measured ratio of the differential cross sections for inclusive isolated-photon production for $R=0.2$ and $R=0.4$ as a function of $E_{\rm T}^{\gamma}$ for $0.6<|\eta^{\gamma}|<0.8$.

Measured ratio of the differential cross sections for inclusive isolated-photon production for $R=0.2$ and $R=0.4$ as a function of $E_{\rm T}^{\gamma}$ for $0.8<|\eta^{\gamma}|<1.37$.

Measured ratio of the differential cross sections for inclusive isolated-photon production for $R=0.2$ and $R=0.4$ as a function of $E_{\rm T}^{\gamma}$ for $1.56<|\eta^{\gamma}|<1.81$.

Measured ratio of the differential cross sections for inclusive isolated-photon production for $R=0.2$ and $R=0.4$ as a function of $E_{\rm T}^{\gamma}$ for $1.81<|\eta^{\gamma}|<2.01$.

Measured ratio of the differential cross sections for inclusive isolated-photon production for $R=0.2$ and $R=0.4$ as a function of $E_{\rm T}^{\gamma}$ for $2.01<|\eta^{\gamma}|<2.37$.

Predicted ratio of the differential cross sections for inclusive isolated-photon production for $R=0.2$ and $R=0.4$ as a function of $E_{\rm T}^{\gamma}$ for $|\eta^{\gamma}|<0.6$ at NNLO QCD.

Predicted ratio of the differential cross sections for inclusive isolated-photon production for $R=0.2$ and $R=0.4$ as a function of $E_{\rm T}^{\gamma}$ for $0.6<|\eta^{\gamma}|<0.8$ at NNLO QCD.

Predicted ratio of the differential cross sections for inclusive isolated-photon production for $R=0.2$ and $R=0.4$ as a function of $E_{\rm T}^{\gamma}$ for $0.8<|\eta^{\gamma}|<1.37$ at NNLO QCD.

Predicted ratio of the differential cross sections for inclusive isolated-photon production for $R=0.2$ and $R=0.4$ as a function of $E_{\rm T}^{\gamma}$ for $1.56<|\eta^{\gamma}|<1.81$ at NNLO QCD.

Predicted ratio of the differential cross sections for inclusive isolated-photon production for $R=0.2$ and $R=0.4$ as a function of $E_{\rm T}^{\gamma}$ for $1.81<|\eta^{\gamma}|<2.01$ at NNLO QCD.

Predicted ratio of the differential cross sections for inclusive isolated-photon production for $R=0.2$ and $R=0.4$ as a function of $E_{\rm T}^{\gamma}$ for $2.01<|\eta^{\gamma}|<2.37$ at NNLO QCD.

Measured fiducial integrated cross section for inclusive isolated-photon production as a function of $R$ for $|\eta^{\gamma}|<0.6$.

Measured fiducial integrated cross section for inclusive isolated-photon production as a function of $R$ for $0.6<|\eta^{\gamma}|<0.8$.

Measured fiducial integrated cross section for inclusive isolated-photon production as a function of $R$ for $0.8<|\eta^{\gamma}|<1.37$.

Measured fiducial integrated cross section for inclusive isolated-photon production as a function of $R$ for $1.56<|\eta^{\gamma}|<1.81$.

Measured fiducial integrated cross section for inclusive isolated-photon production as a function of $R$ for $1.81<|\eta^{\gamma}|<2.01$.

Measured fiducial integrated cross section for inclusive isolated-photon production as a function of $R$ for $2.01<|\eta^{\gamma}|<2.37$.

Predicted fiducial integrated cross section for inclusive isolated-photon production as a function of $R$ for $|\eta^{\gamma}|<0.6$ at NNLO QCD.

Predicted fiducial integrated cross section for inclusive isolated-photon production as a function of $R$ for $0.6<|\eta^{\gamma}|<0.8$ at NNLO QCD.

Predicted fiducial integrated cross section for inclusive isolated-photon production as a function of $R$ for $0.8<|\eta^{\gamma}|<1.37$ at NNLO QCD.

Predicted fiducial integrated cross section for inclusive isolated-photon production as a function of $R$ for $1.56<|\eta^{\gamma}|<1.81$ at NNLO QCD.

Predicted fiducial integrated cross section for inclusive isolated-photon production as a function of $R$ for $1.81<|\eta^{\gamma}|<2.01$ at NNLO QCD.

Predicted fiducial integrated cross section for inclusive isolated-photon production as a function of $R$ for $2.01<|\eta^{\gamma}|<2.37$ at NNLO QCD.

Measured unfolded differential cross-section as a function of the dilepton transverse momentum $p^{ll}_{\mathrm{T}}$. NLO predictions from Sherpa 2.2.10 and MadGraph5_aMC@NLO 2.7.3 are also shown. The uncertainty in the predictions is divided into statistical and theoretical uncertainties (scale and PDF+$\alpha_{s}$).

Measured unfolded differential cross-section as a function of the the four-body transverse momentum $p^{ll\gamma\gamma}_{\mathrm{T}}$. NLO predictions from Sherpa 2.2.10 and MadGraph5_aMC@NLO 2.7.3 are also shown. The uncertainty in the predictions is divided into statistical and theoretical uncertainties (scale and PDF+$\alpha_{s}$).

Measured unfolded differential cross-section as a function of the diphoton invariant mass $m_{\gamma\gamma}$. NLO predictions from Sherpa 2.2.10 and MadGraph5_aMC@NLO 2.7.3 are also shown. The uncertainty in the predictions is divided into statistical and theoretical uncertainties (scale and PDF+$\alpha_{s}$).

Measured unfolded differential cross-section as a function of the four-body invariant mass $m_{ll\gamma\gamma}$. NLO predictions from Sherpa 2.2.10 and MadGraph5_aMC@NLO 2.7.3 are also shown. The uncertainty in the predictions is divided into statistical and theoretical uncertainties (scale and PDF+$\alpha_{s}$).

Expected and observed $95\%$ confidence intervals for the coupling parameters $f_{T,j}/\Lambda^{4}$ of transverse dimension-8 operators. All parameter values outside of the stated range are excluded at the chosen confidence level. No unitarity constraints are applied.

Expected and observed unitarised $95\%$ confidence intervals for the coupling parameter $f_{T,8}/\Lambda^{4}$ in the clipping energy range between 1.1 and 5 TeV. The non-unitarised limits ($E_c = \infty$) are also shown. All parameter values outside of the stated range are excluded at the chosen confidence level.

Expected and observed unitarised $95\%$ confidence intervals for the coupling parameter $f_{T,0}/\Lambda^{4}$ in the clipping energy range between 1.1 and 5 TeV. The non-unitarised limits ($E_c = \infty$) are also shown. All parameter values outside of the stated range are excluded at the chosen confidence level.

Expected and observed unitarised $95\%$ confidence intervals for the coupling parameter $f_{T,1}/\Lambda^{4}$ in the clipping energy range between 1.1 and 5 TeV. The non-unitarised limits ($E_c = \infty$) are also shown. All parameter values outside of the stated range are excluded at the chosen confidence level.

Expected and observed unitarised $95\%$ confidence intervals for the coupling parameter $f_{T,2}/\Lambda^{4}$ in the clipping energy range between 1.1 and 5 TeV. The non-unitarised limits ($E_c = \infty$) are also shown. All parameter values outside of the stated range are excluded at the chosen confidence level.

Expected and observed unitarised $95\%$ confidence intervals for the coupling parameter $f_{T,5}/\Lambda^{4}$ in the clipping energy range between 1.1 and 5 TeV. The non-unitarised limits ($E_c = \infty$) are also shown. All parameter values outside of the stated range are excluded at the chosen confidence level.

Expected and observed unitarised $95\%$ confidence intervals for the coupling parameter $f_{T,6}/\Lambda^{4}$ in the clipping energy range between 1.1 and 5 TeV. The non-unitarised limits ($E_c = \infty$) are also shown. All parameter values outside of the stated range are excluded at the chosen confidence level.

Expected and observed unitarised $95\%$ confidence intervals for the coupling parameter $f_{T,7}/\Lambda^{4}$ in the clipping energy range between 1.1 and 5 TeV. The non-unitarised limits ($E_c = \infty$) are also shown. All parameter values outside of the stated range are excluded at the chosen confidence level.

Expected and observed unitarised $95\%$ confidence intervals for the coupling parameter $f_{T,9}/\Lambda^{4}$ in the clipping energy range between 1.1 and 5 TeV. The non-unitarised limits ($E_c = \infty$) are also shown. All parameter values outside of the stated range are excluded at the chosen confidence level.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 21 to 75 GeV and the W(C=GAMMA P) range 95 to 285 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 21 to 35 GeV and the W(C=GAMMA P) range 95 to 285 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 35 to 52 GeV and the W(C=GAMMA P) range 95 to 285 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 52 to 75 GeV and the W(C=GAMMA P) range 95 to 285 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 21 to 35 GeV and the W(C=GAMMA P) range 95 to 212 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 21 to 35 GeV and the W(C=GAMMA P) range 212 to 285 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 35 to 52 GeV and the W(C=GAMMA P) range 95 to 212 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 35 to 52 GeV and the W(C=GAMMA P) range 212 to 285 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 1 GeV**2) integrated over the ET range 52 to 75 GeV and the W(C=GAMMA P) range 212 to 285 GeV.

Measured differential E+ P cross section DSIG/DETARAP for inclusive jet photoproduction(Q**2 < 0.01 GeV**2) integrated over the ET ranges 5 to 12 GeV and 12 to 21 GeV and the W(C=GAMMA P) range 164 to 242 GeV.

Measured differential E+ P cross section DSIG/DET for inclusive jet photoproductionm, with jets defined by the cone algorithm with R = 1, for the two Q**2 ranges integrated over the jet pseudorapidity range -1 to 2.5 in the W(C=GAMMA P) range 164 to 242 GeV.

The scaled GAMMA P cross section at a mean W of 200 GeV as a function of the jet XT for the jet CM rapidity range -0.5 to 0.5. Jets are defined by the conealgorithm with R = 1.

Inclusive jet cross section DSIG/D(ET**2/Q**2) in the pseudorapidity range 0.5 to 1.5.

Inclusive jet cross section DSIG/D(ET**2/Q**2) in the pseudorapidity range 1.5 to 2.8.

The inelastic dijet cross section as a function of the ET gap.

The dijet cross sections as a function of the rapidity gap with the requirement that ET(C=GAP) is less than ET(C=CUT).

The dijet cross sections as a function of the rapidity gap with the requirement that ET(C=GAP) is less than ET(C=CUT).

The gap fraction defined as the fraction of all dijet events with ET(C= GAP)<ET(C=CUT).

The gap fraction defined as the fraction of all dijet events with ET(C= GAP)<ET(C=CUT).

The dijet cross sections as a function of X(C=GAMMA) with the requirement that ET(C=GAP) is less than ET(C=CUT).

The dijet cross sections as a function of X(C=GAMMA) with the requirement that ET(C=GAP) is less than ET(C=CUT).

The gap fraction defined as the fraction of all dijet events with ET(C= GAP)<ET(C=CUT).

The gap fraction defined as the fraction of all dijet events with ET(C= GAP)<ET(C=CUT).

The dijet cross sections as a function of XP with the requirement that ET(C=GAP) is less than ET(C=CUT).

The dijet cross sections as a function of XP with the requirement that ET(C=GAP) is less than ET(C=CUT).

The gap fraction defined as the fraction of all dijet events with ET(C= GAP)<ET(C=CUT).

The gap fraction defined as the fraction of all dijet events with ET(C= GAP)<ET(C=CUT).

Differential ep cross section for dijet production as a function of the average pseudorapidity the two jets in two transverse energy regions and in the Y region 0.1 to 0.5.

Differential ep cross section for dijet production as a function of the average pseudorapidity the two jets in two transverse energy regions and in the Y region 0.5 to 0.9.

Differential ep cross section for dijet production as a function of the photon momentum fraction X(C=GAMMA) in two regions of proton fractional momentum XP.

Differential ep cross section for dijet production as a function of the proton momentum fraction XP in two regions of photon fractional momentum X(C=GAMMA).

Differential ep cross section for dijet production as a function of the photon momentum fraction X(C=GAMMA) in two regions maximum jet transverseenergy.

Differential ep cross section for dijet production as a function of COS(THETA*) in two regions of fractional photon momentum fraction X(C=GAMMA).

Differential ep cross section for dijet production as a function of COS(THETA*) for dijet masses > 65 GeV in two regions of fractional photon momentum fraction X(C=GAMMA).

Normalised distribution in M(P=4_5) for NC and CC dijet events. M(P=4_5) is the dijet mass.

Normalised distribution in ZP for NC and CC dijet events. ZP corresponds to 0.5*MIN(1-COS(THETA*)) summed over the two jets. THETA* is the polar angle of each parton in the c.m. system of the virtual boson and the incoming parton.

Normalised distribution in XP for NC and CC dijet events. XP is the ratio X/PSI where PSI is the fraction of the protons for momentacarried by the parton entering the hard scattering process.

Normalised distribution in ET(C=FOWARD) for NC and CC dijet events. ET(C=FORWARD) is the transverse energy of the most (non-remnant) forward jet.

Normalised distribution in THETA(C=FORWARD) for NC and CC dijet events. THETA(C=FORWARD) is the polar angle of the most (non-remnant) forward jet.

Normalised distribution in dijet mass for CC and NC events with Q**2 > 5000GeV**2.

No description provided.

No description provided.

Transverse energy flow outside the jets in the rapidity region abs(etarap*)<1.

Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R in the region of mean ET from 3 to 6 GeV.

Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R in the region of mean ET from 6 to 9 GeV.

Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R in the region of mean ET from 9 to 12 GeV.

Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R in the region of mean ET from 12 to 20 GeV.

Fraction of the transverse energy of the jets inside a cone of radious 0.5 around the jet axis as a function of the mean ET of the jets.

Fraction of the transverse energy of the jets inside a cone of radious 0.5 around the jet axis as a function of the jet rapidity.

Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R for X(C=GAMMA)+- <0.8.

Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R for X(C=GAMMA)+- > 0.8.

The ET differential jet cross section in the virtual-photon CM frame.

The ET differential jet cross section in the virtual-photon CM frame.

The ET differential jet cross section in the virtual-photon CM frame.

The ET differential jet cross section in the virtual-photon CM frame.

The ET differential jet cross section in the virtual-photon CM frame.

The ET differential jet cross section in the virtual-photon CM frame.

The ETARAP differential jet cross section in the virtual-photon CM frame.

The ETARAP differential jet cross section in the virtual-photon CM frame.

The ETARAP differential jet cross section in the virtual-photon CM frame.

The ETARAP differential jet cross section in the virtual-photon CM frame.

The ETARAP differential jet cross section in the virtual-photon CM frame.

The ETARAP differential jet cross section in the virtual-photon CM frame.

The ETARAP differential jet cross section in the virtual-photon CM frame.

The ETARAP differential jet cross section in the virtual-photon CM frame.

The ETARAP differential jet cross section in the virtual-photon CM frame.

The inclusive virtual photon-proton jet cross section.

The inclusive virtual photon-proton jet cross section.

The inclusive virtual photon-proton jet cross section.

The inclusive virtual photon-proton jet cross section.