THESE ARE CORRECTED DATA FROM YF 40, 34. PROPER TABLES IN YF 40, 34 MUST. BE REPLACED BY THE GOOD ONES.

THESE ARE CORRECTED DATA FROM YF 40, 34. PROPER TABLES IN YF 40, 34 MUST. BE REPLACED BY THE GOOD ONES.

No description provided.

Differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.200-1.250 GeV.

Differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.250-1.300 GeV.

Differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.300-1.350 GeV.

Differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.350-1.400 GeV.

Differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.400-1.450 GeV.

Differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.450-1.500 GeV.

Differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.500-1.550 GeV.

Differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.550-1.600 GeV.

Differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.600-1.650 GeV.

Differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.650-1.700 GeV.

Differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.700-1.800 GeV.

Differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.800-1.900 GeV.

Differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.900-2.000 GeV.

Inclusive differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.125-1.150 GeV.

Inclusive differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.150-1.175 GeV.

Inclusive differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.175-1.20 GeV.

Inclusive differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.200-1.250 GeV.

Inclusive differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.250-1.300 GeV.

Inclusive differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.300-1.350 GeV.

Inclusive differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.350-1.400 GeV.

Inclusive differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.400-1.450 GeV.

Inclusive differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.450-1.500 GeV.

Inclusive differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.500-1.550 GeV.

Inclusive differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.550-1.600 GeV.

Inclusive differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.600-1.650 GeV.

Inclusive differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.650-1.700 GeV.

Inclusive differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.700-1.800 GeV.

Inclusive differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.800-1.900 GeV.

Inclusive differential cross-sections of $\omega$ mesons produced off the free proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.900-2.000 GeV.

Total cross-section as a function of the incident photon energy for $\omega$ mesons produced off the free proton obtained from exclusive and inclusive analysis$.

Slope parameter and horizontal level from the fits to the differential cross-sections $d\sigma/dt$ for $\omega$ mesons produced off the free proton.

Differential cross-sections of $\omega$ mesons produced off the bound proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.158-1.208 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.208-1.233 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.233-1.258 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.258-1.308 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.308-1.358 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.358-1.408 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.408-1.508 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.508-1.608 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.608-1.708 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.708-1.808 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.808-1.908 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound proton versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.908-2.008 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.158-1.208 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.208-1.233 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.233-1.258 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.258-1.308 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.308-1.358 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.358-1.408 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.408-1.508 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.508-1.608 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.608-1.708 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.708-1.808 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.808-1.908 GeV.

Differential cross-sections of $\omega$ mesons produced off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.908-2.008 GeV.

Slope parameter and horizontal level from the fits to the differential cross-sections $d\sigma/dt$ for $\omega$ mesons produced off the bound proton.

Slope parameter and horizontal level from the fits to the differential cross-sections $d\sigma/dt$ for $\omega$ mesons produced off the bound neutron.

Inclusive differential cross-sections of $\omega$ mesons produced off deuterium versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.158-1.208 GeV.

Inlusive differential cross-sections of $\omega$ mesons produced off deuterium versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.208-1.233 GeV.

Inlusive differential cross-sections of $\omega$ mesons produced off deuterium versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.233-1.258 GeV.

Inlusive differential cross-sections of $\omega$ mesons produced off deuterium versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.258-1.308 GeV.

Inlusive differential cross-sections of $\omega$ mesons produced off deuterium versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.308-1.358 GeV.

Inlusive differential cross-sections of $\omega$ mesons produced off deuterium versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.358-1.408 GeV.

Inlusive differential cross-sections of $\omega$ mesons produced off deuterium versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.408-1.508 GeV.

Inlusive differential cross-sections of $\omega$ mesons produced off deuterium versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.508-1.608 GeV.

Inlusive differential cross-sections of $\omega$ mesons produced off deuterium versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.608-1.708 GeV.

Inlusive differential cross-sections of $\omega$ mesons produced off deuterium versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.708-1.808 GeV.

Inlusive differential cross-sections of $\omega$ mesons produced off deuterium versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.808-1.908 GeV.

Inlusive differential cross-sections of $\omega$ mesons produced off deuterium versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.908-2.008 GeV.

Sum of the exclusive differential cross-sections of $\omega$ mesons produced off the bound proton and off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.158-1.208 GeV.

Sum of the exclusive differential cross-sections of $\omega$ mesons produced off the bound proton and off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.208-1.233 GeV.

Sum of the exclusive differential cross-sections of $\omega$ mesons produced off the bound proton and off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.233-1.258 GeV.

Sum of the exclusive differential cross-sections of $\omega$ mesons produced off the bound proton and off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.258-1.308 GeV.

Sum of the exclusive differential cross-sections of $\omega$ mesons produced off the bound proton and off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.308-1.358 GeV.

Sum of the exclusive differential cross-sections of $\omega$ mesons produced off the bound proton and off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.358-1.408 GeV.

Sum of the exclusive differential cross-sections of $\omega$ mesons produced off the bound proton and off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.408-1.508 GeV.

Sum of the exclusive differential cross-sections of $\omega$ mesons produced off the bound proton and off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.508-1.608 GeV.

Sum of the exclusive differential cross-sections of $\omega$ mesons produced off the bound proton and off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.608-1.708 GeV.

Sum of the exclusive differential cross-sections of $\omega$ mesons produced off the bound proton and off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.708-1.808 GeV.

Sum of the exclusive differential cross-sections of $\omega$ mesons produced off the bound proton and off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.808-1.908 GeV.

Sum of the exclusive differential cross-sections of $\omega$ mesons produced off the bound proton and off the bound neutron versus $\cos(\theta^\omega_{\mathrm{c.m.}})$ and versus the momentum transfer to the nucleon, $t$, for incident photon energy $E_\gamma$ = 1.908-2.008 GeV.

Total cross-section as a function of the incident photon energy for $\omega$ mesons produced off the bound proton $\sigma_p^{\mathrm{bound}}$, off the bound neutron $\sigma_n^{\mathrm{bound}}$, the sum of the two exclusive cross-sections $\sigma_p^{\mathrm{bound}}+\sigma_n^{\mathrm{bound}}$, the quasi-free inclusive cross-section $\sigma_{\mathrm{incl}}$ and the cross-section off the neutron calculated by $\sigma_{\mathrm{incl}}-\sigma_p^{\mathrm{bound}}$.

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Diphoton production cross section as a function of the diphoton rapidity.

Diphoton production cross section differential in the cosine of the polar angle in the Collins-Soper frame.

Diphoton production cross section differential in the sub-leading to leading photon transverse momentum ratio (z).

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 the W range 1.75 to 1.76 GeV.

Differential cross section for the W range 1.76 to 1.77 GeV.

Differential cross section for the W range 1.77 to 1.78 GeV.

Differential cross section for the W range 1.78 to 1.79 GeV.

Differential cross section for the W range 1.79 to 1.80 GeV.

Differential cross section for the W range 1.80 to 1.81 GeV.

Differential cross section for the W range 1.81 to 1.82 GeV.

Differential cross section for the W range 1.82 to 1.83 GeV.

Differential cross section for the W range 1.83 to 1.84 GeV.

Differential cross section for the W range 1.84 to 1.85 GeV.

Differential cross section for the W range 1.85 to 1.86 GeV.

Differential cross section for the W range 1.86 to 1.87 GeV.

Differential cross section for the W range 1.87 to 1.88 GeV.

Differential cross section for the W range 1.88 to 1.89 GeV.

Differential cross section for the W range 1.89 to 1.90 GeV.

Differential cross section for the W range 1.90 to 1.91 GeV.

Differential cross section for the W range 1.91 to 1.92 GeV.

Differential cross section for the W range 1.92 to 1.93 GeV.

Differential cross section for the W range 1.93 to 1.94 GeV.

Differential cross section for the W range 1.94 to 1.95 GeV.

Differential cross section for the W range 1.96 to 1.97 GeV.

Differential cross section for the W range 1.97 to 1.98 GeV.

Differential cross section for the W range 1.98 to 1.99 GeV.

Differential cross section for the W range 1.99 to 2.00 GeV.

Differential cross section for the W range 2.00 to 2.01 GeV.

Differential cross section for the W range 2.01 to 2.02 GeV.

Differential cross section for the W range 2.02 to 2.03 GeV.

Differential cross section for the W range 2.03 to 2.04 GeV.

Differential cross section for the W range 2.04 to 2.05 GeV.

Differential cross section for the W range 2.05 to 2.06 GeV.

Differential cross section for the W range 2.06 to 2.07 GeV.

Differential cross section for the W range 2.07 to 2.08 GeV.

Differential cross section for the W range 2.08 to 2.09 GeV.

Differential cross section for the W range 2.09 to 2.10 GeV.

Differential cross section for the W range 2.10 to 2.11 GeV.

Differential cross section for the W range 2.11 to 2.12 GeV.

Differential cross section for the W range 2.12 to 2.13 GeV.

Differential cross section for the W range 2.13 to 2.14 GeV.

Differential cross section for the W range 2.14 to 2.15 GeV.

Differential cross section for the W range 2.15 to 2.16 GeV.

Differential cross section for the W range 2.16 to 2.17 GeV.

Differential cross section for the W range 2.17 to 2.18 GeV.

Differential cross section for the W range 2.18 to 2.19 GeV.

Differential cross section for the W range 2.19 to 2.20 GeV.

Differential cross section for the W range 2.20 to 2.21 GeV.

Differential cross section for the W range 2.21 to 2.22 GeV.

Differential cross section for the W range 2.22 to 2.23 GeV.

Differential cross section for the W range 2.23 to 2.24 GeV.

Differential cross section for the W range 2.24 to 2.25 GeV.

Differential cross section for the W range 2.25 to 2.26 GeV.

Differential cross section for the W range 2.26 to 2.27 GeV.

Differential cross section for the W range 2.27 to 2.28 GeV.

Differential cross section for the W range 2.28 to 2.29 GeV.

Differential cross section for the W range 2.29 to 2.30 GeV.

Differential cross section for the W range 2.30 to 2.31 GeV.

Differential cross section for the W range 2.31 to 2.32 GeV.

Differential cross section for the W range 2.32 to 2.33 GeV.

Differential cross section for the W range 2.33 to 2.34 GeV.

Differential cross section for the W range 2.34 to 2.35 GeV.

Differential cross section for the W range 2.35 to 2.36 GeV.

Differential cross section for the W range 2.36 to 2.37 GeV.

Differential cross section for the W range 2.37 to 2.38 GeV.

Differential cross section for the W range 2.38 to 2.39 GeV.

Differential cross section for the W range 2.39 to 2.40 GeV.

Differential cross section for the W range 2.40 to 2.41 GeV.

Differential cross section for the W range 2.41 to 2.42 GeV.

Differential cross section for the W range 2.42 to 2.43 GeV.

Differential cross section for the W range 2.43 to 2.44 GeV.

Differential cross section for the W range 2.44 to 2.45 GeV.

Differential cross section for the W range 2.45 to 2.46 GeV.

Differential cross section for the W range 2.46 to 2.47 GeV.

Differential cross section for the W range 2.47 to 2.48 GeV.

Differential cross section for the W range 2.48 to 2.49 GeV.

Differential cross section for the W range 2.49 to 2.50 GeV.

Differential cross section for the W range 2.50 to 2.51 GeV.

Differential cross section for the W range 2.51 to 2.52 GeV.

Differential cross section for the W range 2.52 to 2.53 GeV.

Differential cross section for the W range 2.53 to 2.54 GeV.

Differential cross section for the W range 2.54 to 2.55 GeV.

Differential cross section for the W range 2.55 to 2.56 GeV.

Differential cross section for the W range 2.56 to 2.57 GeV.

Differential cross section for the W range 2.57 to 2.58 GeV.

Differential cross section for the W range 2.58 to 2.59 GeV.

Differential cross section for the W range 2.59 to 2.60 GeV.

Differential cross section for the W range 2.60 to 2.61 GeV.

Differential cross section for the W range 2.61 to 2.62 GeV.

Differential cross section for the W range 2.62 to 2.63 GeV.

Differential cross section for the W range 2.63 to 2.64 GeV.

Differential cross section for the W range 2.64 to 2.65 GeV.

Differential cross section for the W range 2.65 to 2.66 GeV.

Differential cross section for the W range 2.66 to 2.67 GeV.

Differential cross section for the W range 2.67 to 2.68 GeV.

Differential cross section for the W range 2.68 to 2.69 GeV.

Differential cross section for the W range 2.69 to 2.70 GeV.

Differential cross section for the W range 2.70 to 2.71 GeV.

Differential cross section for the W range 2.71 to 2.72 GeV.

Differential cross section for the W range 2.72 to 2.73 GeV.

Differential cross section for the W range 2.75 to 2.76 GeV.

Differential cross section for the W range 2.76 to 2.77 GeV.

Differential cross section for the W range 2.77 to 2.78 GeV.

Differential cross section for the W range 2.78 to 2.79 GeV.

Differential cross section for the W range 2.79 to 2.80 GeV.

Differential cross section for the W range 2.80 to 2.81 GeV.

Differential cross section for the W range 2.81 to 2.82 GeV.

Differential cross section for the W range 2.82 to 2.83 GeV.

Differential cross section for the W range 2.83 to 2.84 GeV.

Spin density matrix elements for the W range 1.72 to 1.73 GeV.

Spin density matrix elements for the W range 1.73 to 1.74 GeV.

Spin density matrix elements for the W range 1.74 to 1.75 GeV.

Spin density matrix elements for the W range 1.75 to 1.76 GeV.

Spin density matrix elements for the W range 1.76 to 1.77 GeV.

Spin density matrix elements for the W range 1.77 to 1.78 GeV.

Spin density matrix elements for the W range 1.78 to 1.79 GeV.

Spin density matrix elements for the W range 1.79 to 1.80 GeV.

Spin density matrix elements for the W range 1.80 to 1.81 GeV.

Spin density matrix elements for the W range 1.81 to 1.82 GeV.

Spin density matrix elements for the W range 1.82 to 1.83 GeV.

Spin density matrix elements for the W range 1.83 to 1.84 GeV.

Spin density matrix elements for the W range 1.84 to 1.85 GeV.

Spin density matrix elements for the W range 1.85 to 1.86 GeV.

Spin density matrix elements for the W range 1.86 to 1.87 GeV.

Spin density matrix elements for the W range 1.87 to 1.88 GeV.

Spin density matrix elements for the W range 1.88 to 1.89 GeV.

Spin density matrix elements for the W range 1.89 to 1.90 GeV.

Spin density matrix elements for the W range 1.90 to 1.91 GeV.

Spin density matrix elements for the W range 1.91 to 1.92 GeV.

Spin density matrix elements for the W range 1.92 to 1.93 GeV.

Spin density matrix elements for the W range 1.93 to 1.94 GeV.

Spin density matrix elements for the W range 1.94 to 1.95 GeV.

Spin density matrix elements for the W range 1.95 to 1.96 GeV.

Spin density matrix elements for the W range 1.96 to 1.97 GeV.

Spin density matrix elements for the W range 1.97 to 1.98 GeV.

Spin density matrix elements for the W range 1.98 to 1.99 GeV.

Spin density matrix elements for the W range 1.99 to 2.00 GeV.

Spin density matrix elements for the W range 2.00 to 2.01 GeV.

Spin density matrix elements for the W range 2.01 to 2.02 GeV.

Spin density matrix elements for the W range 2.02 to 2.03 GeV.

Spin density matrix elements for the W range 2.03 to 2.04 GeV.

Spin density matrix elements for the W range 2.04 to 2.05 GeV.

Spin density matrix elements for the W range 2.05 to 2.06 GeV.

Spin density matrix elements for the W range 2.06 to 2.07 GeV.

Spin density matrix elements for the W range 2.07 to 2.08 GeV.

Spin density matrix elements for the W range 2.08 to 2.09 GeV.

Spin density matrix elements for the W range 2.09 to 2.10 GeV.

Spin density matrix elements for the W range 2.10 to 2.11 GeV.

Spin density matrix elements for the W range 2.11 to 2.12 GeV.

Spin density matrix elements for the W range 2.12 to 2.13 GeV.

Spin density matrix elements for the W range 2.13 to 2.14 GeV.

Spin density matrix elements for the W range 2.14 to 2.15 GeV.

Spin density matrix elements for the W range 2.15 to 2.16 GeV.

Spin density matrix elements for the W range 2.16 to 2.17 GeV.

Spin density matrix elements for the W range 2.17 to 2.18 GeV.

Spin density matrix elements for the W range 2.18 to 2.19 GeV.

Spin density matrix elements for the W range 2.19 to 2.20 GeV.

Spin density matrix elements for the W range 2.20 to 2.21 GeV.

Spin density matrix elements for the W range 2.21 to 2.22 GeV.

Spin density matrix elements for the W range 2.22 to 2.23 GeV.

Spin density matrix elements for the W range 2.23 to 2.24 GeV.

Spin density matrix elements for the W range 2.24 to 2.25 GeV.

Spin density matrix elements for the W range 2.25 to 2.26 GeV.

Spin density matrix elements for the W range 2.26 to 2.27 GeV.

Spin density matrix elements for the W range 2.27 to 2.28 GeV.

Spin density matrix elements for the W range 2.28 to 2.29 GeV.

Spin density matrix elements for the W range 2.29 to 2.30 GeV.

Spin density matrix elements for the W range 2.30 to 2.31 GeV.

Spin density matrix elements for the W range 2.31 to 2.32 GeV.

Spin density matrix elements for the W range 2.32 to 2.33 GeV.

Spin density matrix elements for the W range 2.33 to 2.34 GeV.

Spin density matrix elements for the W range 2.34 to 2.35 GeV.

Spin density matrix elements for the W range 2.35 to 2.36 GeV.

Spin density matrix elements for the W range 2.36 to 2.37 GeV.

Spin density matrix elements for the W range 2.37 to 2.38 GeV.

Spin density matrix elements for the W range 2.38 to 2.39 GeV.

Spin density matrix elements for the W range 2.39 to 2.40 GeV.

Spin density matrix elements for the W range 2.40 to 2.41 GeV.

Spin density matrix elements for the W range 2.41 to 2.42 GeV.

Spin density matrix elements for the W range 2.42 to 2.43 GeV.

Spin density matrix elements for the W range 2.43 to 2.44 GeV.

Spin density matrix elements for the W range 2.44 to 2.45 GeV.

Spin density matrix elements for the W range 2.45 to 2.46 GeV.

Spin density matrix elements for the W range 2.46 to 2.47 GeV.

Spin density matrix elements for the W range 2.47 to 2.48 GeV.

Spin density matrix elements for the W range 2.48 to 2.49 GeV.

Spin density matrix elements for the W range 2.49 to 2.50 GeV.

Spin density matrix elements for the W range 2.50 to 2.51 GeV.

Spin density matrix elements for the W range 2.51 to 2.52 GeV.

Spin density matrix elements for the W range 2.52 to 2.53 GeV.

Spin density matrix elements for the W range 2.53 to 2.54 GeV.

Spin density matrix elements for the W range 2.54 to 2.55 GeV.

Spin density matrix elements for the W range 2.55 to 2.56 GeV.

Spin density matrix elements for the W range 2.56 to 2.57 GeV.

Spin density matrix elements for the W range 2.57 to 2.58 GeV.

Spin density matrix elements for the W range 2.58 to 2.59 GeV.

Spin density matrix elements for the W range 2.59 to 2.60 GeV.

Spin density matrix elements for the W range 2.60 to 2.61 GeV.

Spin density matrix elements for the W range 2.61 to 2.62 GeV.

Spin density matrix elements for the W range 2.62 to 2.63 GeV.

Spin density matrix elements for the W range 2.63 to 2.64 GeV.

Spin density matrix elements for the W range 2.64 to 2.65 GeV.

Spin density matrix elements for the W range 2.65 to 2.66 GeV.

Spin density matrix elements for the W range 2.66 to 2.67 GeV.

Spin density matrix elements for the W range 2.67 to 2.68 GeV.

Spin density matrix elements for the W range 2.68 to 2.69 GeV.

Spin density matrix elements for the W range 2.69 to 2.70 GeV.

Spin density matrix elements for the W range 2.70 to 2.71 GeV.

Spin density matrix elements for the W range 2.71 to 2.72 GeV.

Spin density matrix elements for the W range 2.72 to 2.73 GeV.

Spin density matrix elements for the W range 2.73 to 2.74 GeV.

Spin density matrix elements for the W range 2.74 to 2.75 GeV.

Spin density matrix elements for the W range 2.75 to 2.76 GeV.

Spin density matrix elements for the W range 2.76 to 2.77 GeV.

Spin density matrix elements for the W range 2.77 to 2.78 GeV.

Spin density matrix elements for the W range 2.78 to 2.79 GeV.

Spin density matrix elements for the W range 2.79 to 2.80 GeV.

Spin density matrix elements for the W range 2.80 to 2.81 GeV.

Spin density matrix elements for the W range 2.81 to 2.82 GeV.

Spin density matrix elements for the W range 2.82 to 2.83 GeV.

Spin density matrix elements for the W range 2.83 to 2.84 GeV.

Differential cross section for events with at least 3-jets as a function of the pseudorapidity of each jet.

Differential cross section for events with at least 3-jets as a function of the pseudorapidity of each jet.

Differential cross section for events with at least 3-jets as a function of X1.

Differential cross section for events with at least 3-jets as a function of X2.

Differential cross section for events with at least 3-jets as a function of the three jet angle THETA (see text of article).

Differential cross section for events with at least 3-jets as a function of the three jet angle PHI (see text of article).

Differential cross section for events with at least 3-jets as a function of the PT of the leading jet in GAMMA P centre of mass frame.

Differential cross section for events with at least 3-jets as a function of the pseudorapidity difference between the two leading.

Differential cross section as a function of x for events with at least 3 jets with one forward jet and two central jets.

Differential cross section as a function of the pseudorapidity of the leading jet for events with at least 3 jets with one forward jet and two central jets.

Differential cross section as a function of the PT of the leading jet in the GAMMA* P rest frame for events with at least 3 jets with one forward jet and two central jets.

Differential cross section as a function of X for events with at least 3 jets with two forward jets and one central jet.

Differential cross section as a function of the pseudorapidity of the leading jet for events with at least 3 jets with two forward jets and one central jet.

Differential cross section as a function of the PT of the leading jet in the GAMMA* P rest frame for events with at least 3 jets with two forward jets and one central jet.

Differential cross section as a function of the pseudorapidity of the leading jet for events with at least 3 jets and the PT of the leading jet in the GAMMA* P rest frame > 20 GeV.

Differential cross section as a function of X for events with at least 3 jets and the PT of the leading jet in the GAMMA* P rest frame > 20 GeV.

Differential cross section as a function of the difference in the pseudorapidity of the leading and fourth jets for events with at least 4 jets.

Differential cross section as a function X2 for events with at least 4 jets.

Differential cross section as a function the jet angle THETA for events with at least 4 jets.

Differential cross section as a function the PT of the leading jet in GAMMA* P rest frame for events with at least 4 jets.

COS(THETA*) distribution for leptonic W decay in lepton+jets events.. The data in this table are PRELIMINARY and taken from D0 Note 5722-CONF. Data are read from plots and errors are statistcial (sqrt(N)).

COS(THETA*) distribution for hadronic W decay in lepton+jets events.. The data in this table are PRELIMINARY and taken from D0 Note 5722-CONF. Data are read from plots and errors are statistcial (sqrt(N)).

COS(THETA*) distribution for W decay in dilepton events.. The data in this table are PRELIMINARY and taken from D0 Note 5722-CONF. Data are read from plots and errors are statistcial (sqrt(N)).