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 $\sigma_{\mathrm{incl}}-\sigma_p^{\mathrm{bound}}$.

Double-spin azimuthal asymmetries for a transversely (T) polarised target and a longitudinally (L) polarised beam.

Double-spin azimuthal asymmetries for a transversely (T) polarised target and a longitudinally (L) polarised beam.

Double-spin azimuthal asymmetries for a transversely (T) polarised target and a longitudinally (L) polarised beam.

Inclusive energy distribution for incident photon energy 1.550 to 2.200 GeV.

Inclusive angular distribution for C12.

Inclusive angular distribution for CA40.

Inclusive angular distribution for NB93.

Inclusive angular distribution for PB.

Exclusive single ETA production cross section.

Inclusive single ETA production cross section.

V0 V0 cross section for PI- on C target.

V0 V0 cross section for SIGMA- on CU target.

V0 V0 cross section for SIGMA- on C target.

Feynman X distributions of the first LAMBDA in LAMBDA LAMBDA production from SIGMA- on C and CU targets.

Feynman X distributions of the second LAMBDA in LAMBDA LAMBDA production from SIGMA- on C and CU targets.

Feynman X distributions of the first LAMBDA in LAMBDA LAMBDA production from PI- on C and CU targets.

Feynman X distributions of the second LAMBDA in LAMBDA LAMBDA production from PI- on C and CU targets.

Feynman X distributions of the first LAMBDA in LAMBDA LAMBDA production from N on C and CU targets.

Feynman X distributions of the second LAMBDA in LAMBDA LAMBDA production from N on C and CU targets.

Feynman X distributions of the LAMBDA in LAMBDA K0S production from SIGMA- on C and CU targets.

Feynman X distributions of the K0S in LAMBDA K0S production from SIGMA- on C and CU targets.

Feynman X distributions of the LAMBDA in LAMBDA K0S production from PI- on C and CU targets.

Feynman X distributions of the K0S in LAMBDA K0S production from PI- on C and CU targets.

Feynman X distributions of the LAMBDA in LAMBDA K0S production from N on C and CU targets.

Feynman X distributions of the K0S in LAMBDA K0S production from N on C and CU targets.

Feynman X distributions of the LAMBDA in LAMBDA LAMBDABAR production from SIGMA- on C and CU targets.

Feynman X distributions of the LAMBDABAR in LAMBDA LAMBDABAR production from SIGMA- on C and CU targets.

Feynman X distributions of the LAMBDA in LAMBDA LAMBDABAR production from PI- on C and CU targets.

Feynman X distributions of the LAMBDABAR in LAMBDA LAMBDABAR production from PI- on C and CU targets.

Feynman X distributions of the LAMBDA in LAMBDA LAMBDABAR production from N on C and CU targets.

Feynman X distributions of the LAMBDABAR in LAMBDA LAMBDABAR production from N on C and CU targets.

Feynman X distributions of the first K0s in K0S K0S production from SIGMA- on C and CU targets.

Feynman X distributions of the second K0s in K0S K0S production from SIGMA- on C and CU targets.

Feynman X distributions of the first K0s in K0S K0S production from PI- on C and CU targets.

Feynman X distributions of the second K0s in K0S K0S production from PI- on C and CU targets.

Feynman X distributions of the first K0s in K0S K0S production from N on C and CU targets.

Feynman X distributions of the second K0s in K0S K0S production from N on C and CU targets.

Feynman X distributions of the LAMBDABAR in LAMBDABAR K0S production from SIGMA- on C and CU targets.

Feynman X distributions of the K0S in LAMBDABAR K0S production from SIGMA- on C and CU targets.

Feynman X distributions of the LAMBDABAR in LAMBDABAR K0S production from PI- on C and CU targets.

Feynman X distributions of the K0S in LAMBDABAR K0S production from PI- on C and CU targets.

Feynman X distributions of the LAMBDABAR in LAMBDABAR K0S production from N on C and CU targets.

Feynman X distributions of the K0S in LAMBDABAR K0S production from N on C and CU targets.

Feynman X distributions of the first LAMBDABAR in LAMBDABAR LAMBDABAR production from SIGMA- on C and CU targets.

Feynman X distributions of the second LAMBDABAR in LAMBDABAR LAMBDABAR production from SIGMA- on C and CU targets.

Feynman X distributions of the first LAMBDABAR in LAMBDABAR LAMBDABAR production from PI- on C and CU targets.

Feynman X distributions of the second LAMBDABAR in LAMBDABAR LAMBDABAR production from PI- on C and CU targets.

Feynman X distributions of the first LAMBDABAR in LAMBDABAR LAMBDABAR production from N on C and CU targets.

Feynman X distributions of the second LAMBDABAR in LAMBDABAR LAMBDABAR production from N on C and CU targets.

Transverse momentum distributions of the first LAMBDA in LAMBDA LAMBDA production for SIGMA- on C and CU targets.

Transverse momentum distributions of the second LAMBDA in LAMBDA LAMBDA production for SIGMA- on C and CU targets.

Transverse momentum distributions of the first LAMBDA in LAMBDA LAMBDA production for PI- on C and CU targets.

Transverse momentum distributions of the second LAMBDA in LAMBDA LAMBDA production for PI- on C and CU targets.

Transverse momentum distributions of the first LAMBDA in LAMBDA LAMBDA production for N on C and CU targets.

Transverse momentum distributions of the second LAMBDA in LAMBDA LAMBDA production for N on C and CU targets.

Transverse momentum distributions of the LAMBDA in LAMBDA LAMBDABAR production for SIGMA- on C and CU targets.

Transverse momentum distributions of the LAMBDABAR in LAMBDA LAMBDABAR production for SIGMA- on C and CU targets.

Transverse momentum distributions of the LAMBDA in LAMBDA LAMBDABAR production for PI- on C and CU targets.

Transverse momentum distributions of the LAMBDABAR in LAMBDA LAMBDABAR production for PI- on C and CU targets.

Transverse momentum distributions of the LAMBDA in LAMBDA LAMBDABAR production for N on C and CU targets.

Transverse momentum distributions of the LAMBDABAR in LAMBDA LAMBDABAR production for N on C and CU targets.

Transverse momentum distributions of the LAMBDA in LAMBDA K0S production for SIGMA- on C and CU targets.

Transverse momentum distributions of the K0S in LAMBDA K0S production for SIGMA- on C and CU targets.

Transverse momentum distributions of the LAMBDA in LAMBDA K0S production for PI- on C and CU targets.

Transverse momentum distributions of the K0S in LAMBDA K0S production for PI- on C and CU targets.

Transverse momentum distributions of the LAMBDA in LAMBDA K0S production for N on C and CU targets.

Transverse momentum distributions of the K0S in LAMBDA K0S production for N on C and CU targets.

Transverse momentum distributions of the first K0S in K0S K0S production for SIGMA- on C and CU targets.

Transverse momentum distributions of the second K0S in K0S K0S production for SIGMA- on C and CU targets.

Transverse momentum distributions of the first K0S in K0S K0S production for PI- on C and CU targets.

Transverse momentum distributions of the second K0S in K0S K0S production for PI- on C and CU targets.

Transverse momentum distributions of the first K0S in K0S K0S production for N on C and CU targets.

Transverse momentum distributions of the second K0S in K0S K0S production for N on C and CU targets.

Transverse momentum distributions of the first LAMBDABAR in LAMBDABAR LAMBDABAR production for SIGMA- on C and CU targets.

Transverse momentum distributions of the second LAMBDABAR in LAMBDABAR LAMBDABAR production for SIGMA- on C and CU targets.

Transverse momentum distributions of the first LAMBDABAR in LAMBDABAR LAMBDABAR production for PI- on C and CU targets.

Transverse momentum distributions of the second LAMBDABAR in LAMBDABAR LAMBDABAR production for PI- on C and CU targets.

Transverse momentum distributions of the first LAMBDABAR in LAMBDABAR LAMBDABAR production for N on C and CU targets.

Transverse momentum distributions of the second LAMBDABAR in LAMBDABAR LAMBDABAR production for N on C and CU targets.

Transverse momentum distributions of the LAMBDABAR in LAMBDABAR K0S production for SIGMA- on C and CU targets.

Transverse momentum distributions of the K0S in LAMBDABAR K0S production for SIGMA- on C and CU targets.

Transverse momentum distributions of the LAMBDABAR in LAMBDABAR K0S production for PI- on C and CU targets.

Transverse momentum distributions of the K0S in LAMBDABAR K0S production for PI- on C and CU targets.

Transverse momentum distributions of the LAMBDABAR in LAMBDABAR K0S production for N on C and CU targets.

Transverse momentum distributions of the K0S in LAMBDABAR K0S production for N on C and CU targets.

Differential cross section for LAMBDA LAMBDA production as a function of the difference in XF between the fast (P=3,first LAMBDA) and the slow (P=4,second LAMBDA) member of the pair for N on C and CU targets.

Differential cross section for LAMBDA LAMBDA production as a function of the difference in XF between the fast (P=3,first LAMBDA) and the slow (P=4,second LAMBDA) member of the pair for PI- on C and CU targets.

Differential cross section for LAMBDA LAMBDA production as a function of the difference in XF between the fast (P=3,first LAMBDA) and the slow (P=4,second LAMBDA) member of the pair for SIGMA- on C and CU targets.

Differential cross section for LAMBDA LAMBDABAR production as a function of the difference in XF between the fast (P=3,LAMBDA) and the slow (P=4,LAMBDABAR) member of the pair for N on C and CU targets.

Differential cross section for LAMBDA LAMBDABAR production as a function of the difference in XF between the fast (P=3,LAMBDA) and the slow (P=4,LAMBDABAR) member of the pair for PI- on C and CU targets.

Differential cross section for LAMBDA LAMBDABAR production as a function of the difference in XF between the fast (P=3,LAMBDA) and the slow (P=4,LAMBDABAR) member of the pair for SIGMA- on C and CU targets.

Differential cross section for LAMBDA K0S production as a function of the difference in XF between the fast (P=3,LAMBDA) and the slow (P=4,K0S) member of the pair for N on C and CU targets.

Differential cross section for LAMBDA K0S production as a function of the difference in XF between the fast (P=3,LAMBDA) and the slow (P=4,K0S) member of the pair for PI- on C and CU targets.

Differential cross section for LAMBDA K0S production as a function of the difference in XF between the fast (P=3,LAMBDA) and the slow (P=4,K0S) member of the pair for SIGMA- on C and CU targets.

Differential cross section for LAMBDABAR LAMBDABAR production as a function of the difference in XF between the fast (P=3,first LAMBDABAR) and the slow (P=4,second LAMBDABAR) member of the pair for N on C and CU targets.

Differential cross section for LAMBDABAR LAMBDABAR production as a function of the difference in XF between the fast (P=3,first LAMBDABAR) and the slow (P=4,second LAMBDABAR) member of the pair for PI- on C and CU targets.

Differential cross section for LAMBDABAR LAMBDABAR production as a function of the difference in XF between the fast (P=3,first LAMBDABAR) and the slow (P=4,second LAMBDABAR) member of the pair for SIGMA- on C and CU targets.

Differential cross section for LAMBDABAR K0S production as a function of the difference in XF between the fast (P=3,LAMBDABAR) and the slow (P=4,K0S) member of the pair for N on C and CU targets.

Differential cross section for LAMBDABAR K0S production as a function of the difference in XF between the fast (P=3,LAMBDABAR) and the slow (P=4,K0S) member of the pair for PI- on C and CU targets.

Differential cross section for LAMBDABAR K0S production as a function of the difference in XF between the fast (P=3,LAMBDABAR) and the slow (P=4,K0S) member of the pair for SIGMA- on C and CU targets.

Differential cross section for K0S K0S production as a function of the difference in XF between the fast (P=3,first K0S) and the slow (P=4,second K0S) member of the pair for N on C and CU targets.

Differential cross section for K0S K0S production as a function of the difference in XF between the fast (P=3,first K0S) and the slow (P=4,second K0S) member of the pair for PI- on C and CU targets.

Differential cross section for K0S K0S production as a function of the difference in XF between the fast (P=3,first K0S) and the slow (P=4,second K0S) member of the pair for SIGMA- on C and CU targets.

Cross section as a function of Feynman X for F2PRIME(1525) production with SIGMA- on CU and C targets.

Cross section as a function of transverse momentum for F2PRIME(1525) production with SIGMA- on CU and C targets.

Measured values of the LAMBDA polarization as a function of PT in the XL range 0.4 to 0.5.

Measured values of the LAMBDA polarization as a function of PT in the XL range 0.5 to 0.6.

Measured values of the LAMBDA polarization as a function of PT in the XL range 0.6 to 0.7.

Measured values of the LAMBDA polarization as a function of PT in the XL range 0.7 to 0.8.

Measured values of the LAMBDA polarization as a function of PT in the XL range 0.8 to 0.9.

Total inclusive LAMBDA LAMBDA pair production cross sections for the Neutron beam on the Carbon target.

PROJECTILE ASSOCIATED HE-FRAGMENTS.

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