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 cross section as a function of ET(JET1) for X(C=GAMMA) > 0.75 for:. 0 < ETARAP(JET1) < 1. 0 < ETARAP(JET2) < 1.

Measured cross section as a function of ET(JET1) for X(C=GAMMA) > 0.75 for:. 1 < ETARAP(JET1) < 2.4. -1 < ETARAP(JET2) < 0.

Measured cross section as a function of ET(JET1) for X(C=GAMMA) > 0.75 for:. 1 < ETARAP(JET1) < 2.4. 0 < ETARAP(JET2) < 1.

Measured cross section as a function of ET(JET1) for X(C=GAMMA) > 0.75 for:. 1 < ETARAP(JET1) < 2.4. 1 < ETARAP(JET2) < 2.4.

Measured cross section as a function of ET(JET1) for X(C=GAMMA) < 0.75 for:. -1 < ETARAP(JET1) < 0. -1 < ETARAP(JET2) < 0.

Measured cross section as a function of ET(JET1) for X(C=GAMMA) < 0.75 for:. 0 < ETARAP(JET1) < 1. -1 < ETARAP(JET2) < 0.

Measured cross section as a function of ET(JET1) for X(C=GAMMA) < 0.75 for:. 0 < ETARAP(JET1) < 1. 0 < ETARAP(JET2) < 1.

Measured cross section as a function of ET(JET1) for X(C=GAMMA) < 0.75 for:. 1 < ETARAP(JET1) < 2.4. -1 < ETARAP(JET2) < 0.

Measured cross section as a function of ET(JET1) for X(C=GAMMA) < 0.75 for:. 1 < ETARAP(JET1) < 2.4. 0 < ETARAP(JET2) < 1.

Measured cross section as a function of ET(JET1) for X(C=GAMMA) < 0.75 for:. 1 < ETARAP(JET1) < 2.4. 1 < ETARAP(JET2) < 2.4.

Measured cross section as a function of ETARAP(JET2) for X(C=GAMMA) > 0.75 for:. -1 < ETARAP(JET1) < 0.

Measured cross section as a function of ETARAP(JET2) for X(C=GAMMA) > 0.75 for:. 0 < ETARAP(JET1) < 1.

Measured cross section as a function of ETARAP(JET2) for X(C=GAMMA) > 0.75 for:. 1 < ETARAP(JET1) < 2.4.

Measured cross section as a function of ETARAP(JET2) for X(C=GAMMA) < 0.75 for:. -1 < ETARAP(JET1) < 0.

Measured cross section as a function of ETARAP(JET2) for X(C=GAMMA) < 0.75 for:. 0 < ETARAP(JET1) < 1.

Measured cross section as a function of ETARAP(JET2) for X(C=GAMMA) < 0.75 for:. 1 < ETARAP(JET1) < 2.4.

Measured cross section as a function of X(C=GAMMA) for:. 14 < ET(JET1) < 17 GEV.

Measured cross section as a function of X(C=GAMMA) for:. 17 < ET(JET1) < 25 GEV.

No description provided.

Measured cross section as a function of X(C=GAMMA) for:. 25 < ET(JET1) < 35 GEV.

Measured cross section as a function of X(C=GAMMA) for:. 35 < ET(JET1) < 90 GEV.

The differential dijet cross section dsig/dM.

The differential dijet cross section dsig/dET of the leading jet in the Breit frame.

The differential cross section dsig/detarap of the leading jet in the Breitframe.

The differential cross section dsig/dET of the non-leading jet in the Breitframe.

The differential cross section dsig/detarap of the non-leading jet in the Breit frame.

The differential inclusive cross section dsig/dQ**2.

The differential dijet cross section dsig/dQ**2.

The dijet fraction.

The measured values of ALPHA_S determined from the QCD fit to the measured dijet fraction. The first systematic (DSYS) error is the systematic uncertainty not associated with the energy scales of the jets, the second is associated with the energy scales and the third DSYS error is the total theoretical uncertainty.

The measured value of ALPHA_S at the Z0 mass determined from the QCD fit tothe measured dijet spectrum. The first DSYS error is the total experimental systematic uncertainty and the second is the total theoretical systematic uncertainty.

The differential dijet cross section as a function of ETARAP for the neutron-tagged data set. The second DSYS error is due to the uncertainty in the calorimeter energy scale.

Differential cross section as a function of X(C=PI,OBS), the function of the exchanged pion's momentum participating in the production of the dijet system for the neutral-tagged sample. The errors shown have the statistical and main systematic errors added in quadrature. The DSYS error is the systematic error due to the uncertainty in thecalorimeter energy scale. In addition for the neutron-tagged data there is an extra 9 PCT overall error (not shown).

The combined differential cross sections (DSIG/DET,OUT) separately for the low and high Q**2 regions. The data are corrected using the HERWIG-kt model.

The combined differential cross sections (DSIG/DET,OUT) separately for the low and high Q**2 regions. The data are corrected using the PHOJET model.

The combined differential cross sections (DSIG/DN,TRK) separately for the low and high Q**2 regions. The data are corrected using the HERWIG-kt model.

The combined differential cross sections (DSIG/DN,TRK) separately for the low and high Q**2 regions. The data are corrected using the PHOJET model.

The combined differential cross sections (DSIG/DPT,TRK) separately for the low and high Q**2 regions. The data are corrected using the HERWIG-kt model.

The combined differential cross sections (DSIG/DPT,TRK) separately for the low and high Q**2 regions. The data are corrected using the PHOJET model.

The combined energy flow (DE/DETARAP) separately for the low and high Q**2 regions. The data are corrected using the HERWIG-kt model.

The combined energy flow (DE/DETARAP) separately for the low and high Q**2 regions. The data are corrected using the PHOJET model.

The dijet cross section for the full x(gamma) range as a function of the ET of the leading jet.

The dijet cross section for the full x(gamma) range as a function of the ET of the leading jet.

The dijet cross section for the full x(gamma) range as a function of the ET of the leading jet.

The dijet cross section for the x(gamma)>0.75 range as a function of the ET of the leading jet.

The dijet cross section for the x(gamma)>0.75 range as a function of the ET of the leading jet.

The dijet cross section for the x(gamma)>0.75 range as a function of the ET of the leading jet.

The dijet cross section for the x(gamma)>0.75 range as a function of the ET of the leading jet.

The dijet cross section for the x(gamma)>0.75 range as a function of the ET of the leading jet.

The dijet cross section for the x(gamma)>0.75 range as a function of the ET of the leading jet.

The dijet cross section for the full x(gamma) range as a function of the pseudorapidity of the jet with the other jet fixed.

The dijet cross section for the full x(gamma) range as a function of the pseudorapidity of the jet with the other jet fixed.

The dijet cross section for the full x(gamma) range as a function of the pseudorapidity of the jet with the other jet fixed.

The dijet cross section for the x(gamma)>0.75 range as a function of the pseudorapidity of the jet with the other jet fixed.

The dijet cross section for the x(gamma)>0.75 range as a function of the pseudorapidity of the jet with the other jet fixed.

The dijet cross section for the x(gamma)>0.75 range as a function of the pseudorapidity of the jet with the other jet fixed.

The dijet cross section for the full x(gamma) range as a function of the pseudorapidity of the jet with the other jet fixed. This data is for a restricted range of y, (W = 212 to 277 GeV).

The dijet cross section for the full x(gamma) range as a function of the pseudorapidity of the jet with the other jet fixed. This data is for a restricted range of y, (W = 212 to 277 GeV).

The dijet cross section for the full x(gamma) range as a function of the pseudorapidity of the jet with the other jet fixed. This data is for a restricted range of y, (W = 212 to 277 GeV).

The dijet cross section for the x(gamma)>0.75 range as a function of the pseudorapidity of the jet with the other jet fixed. This data is for a restricted range of y, (W = 212 to 277 GeV).

The dijet cross section for the x(gamma)>0.75 range as a function of the pseudorapidity of the jet with the other jet fixed. This data is for a restricted range of y, (W = 212 to 277 GeV).

The dijet cross section for the x(gamma)>0.75 range as a function of the pseudorapidity of the jet with the other jet fixed. This data is for a restricted range of y, (W = 212 to 277 GeV).

Second systematic error is uncertainty in the ET scale.

Second systematic error is uncertainty in the ET scale.

No description provided.