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.

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.

Single differential cross section DSIG/DCOS(THETA).

Double differential cross section D2SIG/DM/DPT in the diphoton mass range 30 TO 50 GeV.

Double differential cross section D2SIG/DM/DPHI in the diphoton mass range 30 TO 50 GeV.

Double differential cross section D2SIG/DM/DCOS(THETA) in the diphoton mass range 30 TO 50 GeV.

Double differential cross section D2SIG/DM/DPT in the diphoton mass range 50 TO 80 GeV.

Double differential cross section D2SIG/DM/DPHI in the diphoton mass range 50 TO 80 GeV.

Double differential cross section D2SIG/DM/DCOS(THETA) in the diphoton mass range 50 TO 80 GeV.

Double differential cross section D2SIG/DM/DPT in the diphoton mass range 80 TO 350 GeV.

Double differential cross section D2SIG/DM/DPHI in the diphoton mass range 80 TO 350 GeV.

Double differential cross section D2SIG/DM/DCOS(THETA) in the diphoton mass range 80 TO 350 GeV.

Differential cross section for XI- production as a function of the invariant mass of the XI- with either of the K+ mesons for incident photon energy 3.09 Gev.

Differential cross section for XI- production as a function of the invariant mass of the XI- with either of the K+ mesons for incident photon energy 3.19 Gev.

Differential cross section for XI- production as a function of the invariant mass of the XI- with either of the K+ mesons for incident photon energy 3.29 Gev.

Differential cross section for XI- production as a function of the invariant mass of the XI- with either of the K+ mesons for incident photon energy 3.39 Gev.

Differential cross section for XI- production as a function of the invariant mass of the XI- with either of the K+ mesons for incident photon energy 3.49 Gev.

Differential cross section for XI- production as a function of the invariant mass of the XI- with either of the K+ mesons for incident photon energy 3.59 Gev.

Differential cross section for XI- production as a function of the invariant mass of the XI- with either of the K+ mesons for incident photon energy 3.69 Gev.

Differential cross section for XI- production as a function of the invariant mass of the XI- with either of the K+ mesons for incident photon energy 3.79 Gev.

Differential cross section for XI- production as a function of the invariant mass of the K+ meson pair for incident photon energy 2.79 Gev.

Differential cross section for XI- production as a function of the invariant mass of the K+ meson pair for incident photon energy 2.89 Gev.

Differential cross section for XI- production as a function of the invariant mass of the K+ meson pair for incident photon energy 2.99 Gev.

Differential cross section for XI- production as a function of the invariant mass of the K+ meson pair for incident photon energy 3.09 Gev.

Differential cross section for XI- production as a function of the invariant mass of the K+ meson pair for incident photon energy 3.19 Gev.

Differential cross section for XI- production as a function of the invariant mass of the K+ meson pair for incident photon energy 3.29 Gev.

Differential cross section for XI- production as a function of the invariant mass of the K+ meson pair for incident photon energy 3.39 Gev.

Differential cross section for XI- production as a function of the invariant mass of the K+ meson pair for incident photon energy 3.49 Gev.

Differential cross section for XI- production as a function of the invariant mass of the K+ meson pair for incident photon energy 3.59 Gev.

Differential cross section for XI- production as a function of the invariant mass of the K+ meson pair for incident photon energy 3.69 Gev.

Differential cross section for XI- production as a function of the invariant mass of the K+ meson pair for incident photon energy 3.79 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of the XI- in the photon-proton cm frame for incident photon energy 2.79 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of the XI- in the photon-proton cm frame for incident photon energy 2.89 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of the XI- in the photon-proton cm frame for incident photon energy 2.99 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of the XI- in the photon-proton cm frame for incident photon energy 3.09 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of the XI- in the photon-proton cm frame for incident photon energy 3.19 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of the XI- in the photon-proton cm frame for incident photon energy 3.29 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of the XI- in the photon-proton cm frame for incident photon energy 3.39 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of the XI- in the photon-proton cm frame for incident photon energy 3.49 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of the XI- in the photon-proton cm frame for incident photon energy 3.59 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of the XI- in the photon-proton cm frame for incident photon energy 3.69 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of the XI- in the photon-proton cm frame for incident photon energy 3.79 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of each K+ in the photon-proton cm frame for incident photon energy 2.79 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of each K+ in the photon-proton cm frame for incident photon energy 2.89 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of each K+ in the photon-proton cm frame for incident photon energy 2.99 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of each K+ in the photon-proton cm frame for incident photon energy 3.09 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of each K+ in the photon-proton cm frame for incident photon energy 3.19 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of each K+ in the photon-proton cm frame for incident photon energy 3.29 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of each K+ in the photon-proton cm frame for incident photon energy 3.39 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of each K+ in the photon-proton cm frame for incident photon energy 3.49 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of each K+ in the photon-proton cm frame for incident photon energy 3.59 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of each K+ in the photon-proton cm frame for incident photon energy 3.69 Gev.

Differential cross section for XI- production as a function of the cosine of the polar angle of each K+ in the photon-proton cm frame for incident photon energy 3.79 Gev.

Total cross section fo XI- production.

Differential cross section for XI(1530)- production as a function of the cosine of the polar angle of the XI(1530)- in the photon-proton cm frame for incident photon energy 3.35 to 4.75 GeV.

Total cross section for XI(1530)- production.

Measured cross section DSIG/DM(PI+PI-) for the W range 1475 to 1500GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1500 to 1525GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1525 to 1550GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1550 to 1575GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1575 to 1600GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1600 to 1625GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1625 to 1650GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1650 to 1675GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1675 to 1700GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1700 to 1725GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1725 to 1750GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1750 to 1775GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1775 to 1800GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1800 to 1825GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1825 to 1850GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1850 to 1875GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1875 to 1900GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1900 to 1925GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1925 to 1950GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1950 to 1975GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 1975 to 2000GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 2000 to 2025GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 2025 to 2050GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 2050 to 2075GeV.

Measured cross section DSIG/DM(PI+PI-) for the W range 2075 to 2100GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1400 to 1425GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1425 to 1450GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1450 to 1475GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1475 to 1500GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1500 to 1525GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1525 to 1550GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1550 to 1575GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1575 to 1600GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1600 to 1625GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1625 to 1650GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1650 to 1675GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1675 to 1700GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1700 to 1725GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1725 to 1750GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1750 to 1775GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1775 to 1800GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1800 to 1825GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1825 to 1850GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1850 to 1875GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1875 to 1900GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1900 to 1925GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1925 to 1950GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1950 to 1975GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 1975 to 2000GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 2000 to 2025GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 2025 to 2050GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 2050 to 2075GeV.

Measured cross section DSIG/DM(PI+Proton) for the W range 2075 to 2100GeV.

Measured c.m. angular distribution of the PI- for the W range 1400 to 1425GeV.

Measured c.m. angular distribution of the PI- for the W range 1425 to 1450GeV.

Measured c.m. angular distribution of the PI- for the W range 1450 to 1475GeV.

Measured c.m. angular distribution of the PI- for the W range 1475 to 1500GeV.

Measured c.m. angular distribution of the PI- for the W range 1500 to 1525GeV.

Measured c.m. angular distribution of the PI- for the W range 1525 to 1550GeV.

Measured c.m. angular distribution of the PI- for the W range 1550 to 1575GeV.

Measured c.m. angular distribution of the PI- for the W range 1575 to 1600GeV.

Measured c.m. angular distribution of the PI- for the W range 1600 to 1625GeV.

Measured c.m. angular distribution of the PI- for the W range 1625 to 1650GeV.

Measured c.m. angular distribution of the PI- for the W range 1650 to 1675GeV.

Measured c.m. angular distribution of the PI- for the W range 1675 to 1700GeV.

Measured c.m. angular distribution of the PI- for the W range 1700 to 1725GeV.

Measured c.m. angular distribution of the PI- for the W range 1725 to 1750GeV.

Measured c.m. angular distribution of the PI- for the W range 1750 to 1775GeV.

Measured c.m. angular distribution of the PI- for the W range 1775 to 1800GeV.

Measured c.m. angular distribution of the PI- for the W range 1800 to 1825GeV.

Measured c.m. angular distribution of the PI- for the W range 1825 to 1850GeV.

Measured c.m. angular distribution of the PI- for the W range 1850 to 1875GeV.

Measured c.m. angular distribution of the PI- for the W range 1875 to 1900GeV.

Measured c.m. angular distribution of the PI- for the W range 1900 to 1925GeV.

Measured c.m. angular distribution of the PI- for the W range 1925 to 1950GeV.

Measured c.m. angular distribution of the PI- for the W range 1950 to 1975GeV.

Measured c.m. angular distribution of the PI- for the W range 1975 to 2000GeV.

Measured c.m. angular distribution of the PI- for the W range 2000 to 2025GeV.

Measured c.m. angular distribution of the PI- for the W range 2025 to 2050GeV.

Measured c.m. angular distribution of the PI- for the W range 2050 to 2075GeV.

Measured c.m. angular distribution of the PI- for the W range 2075 to 2100GeV.

The ratio of the inclusive single jet cross sections for ABS(ETARAP) < 0.5 at c.m. energies 630 and 1800 GeV.

Dijet angular distributions at c.m. energy 1800 GeV in the mass bin 260 to 425 and 425 to 475 GeV. The variable CHI is defined as:. CHI = (1+ABS(COS(THETA**)))/(1-ABS(COS(THETA*))). = EXP(ABS(ETARAP(JET1)-ETARAP(JET2))). where THETA is the cm scattering angle and ETARAP the jet pseudorapidity.

Dijet angular distributions at c.m. energy 1800 GeV in the mass bin 475 to 635 and > 635 GeV. The variable CHI is defined as:. CHI = (1+ABS(COS(THETA**)))/(1-ABS(COS(THETA*))). = EXP(ABS(ETARAP(JET1)-ETARAP(JET2))). where THETA is the cm scattering angle and ETARAP the jet pseudorapidity.

The dijet mass spectrum of events where both jets have ABS(ETARAP) < 1.0 for c.m. energy 1800 GeV.

The dijet mass spectrum of events where both jets have ABS(ETARAP) < 0.5 for c.m. energy 1800 GeV.

The dijet mass spectrum of events where both jets have ABS(ETARAP) 0.5 to 1.0 for c.m. energy 1800 GeV.

The ratio of cross sections of dijet data for ABS(ETARAP) < 0.5 and 0.5 to 1.0 as a function of the dijet mass for c.m. energy 1800 GeV.

Differential jet mass distribution for the jet mass difference using methodM. The data are corrected for the finite acceptance and resolution of the detec tor and for initial state photon radiation.

Distribution of C-parameter. The data are corrected for the finite acceptance and resolution of the detector and for initial state photon radiation.

Distribution of Oblateness. The data are corrected for the finite acceptance and resolution of the detector and for initial state photon radiation.

Distribution of Thrust. The data are corrected for the finite acceptance and resolution of the detector and for initial state photon radiation.

Measured n-jet production rates in percentage of the total hadronic cross section, corrected for detector acceptance and resolution, and for initial state radiation, using the E0 recombination scheme. Errors include statistical and experimental systematic uncertainties. No correction for hadronization effects are applied. YCUT is the cutoff parameter in the jet algorithm.

Measured n-jet production rates in percentage of the total hadronic cross section, corrected for detector acceptance and resolution, and for initial state radiation, using the E0 recombination scheme. Errors include statistical and experimental systematic uncertainties. No correction for hadronization effects are applied. YCUT is the cutoff parameter in the jet algorithm.

Measured n-jet production rates in percentage of the total hadronic cross section, corrected for detector acceptance and resolution, and for initial state radiation, using the E0 recombination scheme. Errors include statistical and experimental systematic uncertainties. No correction for hadronization effects are applied. YCUT is the cutoff parameter in the jet algorithm.

Measured n-jet production rates in percentage of the total hadronic cross section, corrected for detector acceptance and resolution, and for initial state radiation, using the E0 recombination scheme. Errors include statistical and experimental systematic uncertainties. No correction for hadronization effects are applied. YCUT is the cutoff parameter in the jet algorithm.

Measured n-jet production rates in percentage of the total hadronic cross section, corrected for detector acceptance and resolution, and for initial state radiation, using the D recombination scheme. Errors include statistical and experimental systematic uncertainties. No correction for hadronization effects are applied. YCUT is the cutoff parameter in the jet algorithm.

Measured n-jet production rates in percentage of the total hadronic cross section, corrected for detector acceptance and resolution, and for initial state radiation, using the D recombination scheme. Errors include statistical and experimental systematic uncertainties. No correction for hadronization effects are applied. YCUT is the cutoff parameter in the jet algorithm.

Measured n-jet production rates in percentage of the total hadronic cross section, corrected for detector acceptance and resolution, and for initial state radiation, using the D recombination scheme. Errors include statistical and experimental systematic uncertainties. No correction for hadronization effects are applied. YCUT is the cutoff parameter in the jet algorithm.

Measured n-jet production rates in percentage of the total hadronic cross section, corrected for detector acceptance and resolution, and for initial state radiation, using the D recombination scheme. Errors include statistical and experimental systematic uncertainties. No correction for hadronization effects are applied. YCUT is the cutoff parameter in the jet algorithm.

Value of alpha_s obtained by combining all observables.