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We present a measurement of the differential cross section for $t\bar{t}$ events produced in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV as a function of the transverse momentum ($p_T$) of the top quark. The selected events contain a high-$p_T$ lepton ($\ell$), four or more jets, and a large imbalance in $p_T$, and correspond to 1 fb${}^{-1}$ of integrated luminosity recorded with the D0 detector. Each event must have at least one candidate for a $b$ jet. Objects in the event are associated through a constrained kinematic fit to the $t\bar{t}\to WbW\bar{b} \to \ell\nu b q\bar{q}'\bar{b}$ process. Results from next-to-leading-order perturbative QCD calculations agree with the measured differential cross section. Comparisons are also provided to predictions from Monte Carlo event generators using QCD calculations at different levels of precision.
Total cross section for TOP TOPBAR production integrating over PT.
The inclusive PT spectra for TOP TOPBAR production.
We report on double-differential inclusive cross-sections of the production of secondary protons, charged pions, and deuterons, in the interactions with a 5% nuclear interaction length thick stationary lead target, of proton and pion beams with momentum from +/-3 GeV/c to +/-15 GeV/c. Results are given for secondary particles with production angles 20 to 125 degrees. Cross-sections on lead nuclei are compared with cross-sections on beryllium, copper, and tantalum nuclei.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
The production of prompt photons is measured in the photoproduction regime of electron-proton scattering at HERA. The analysis is based on a data sample corresponding to a total integrated luminosity of 340 pb^-1 collected by the H1 experiment. Cross sections are measured for photons with transverse momentum and pseudorapidity in the range 6 < Et < 15 GeV and -1.0 < eta < 2.4, respectively. Cross sections for events with an additional jet are measured as a function of the transverse energy and pseudorapidity of the jet, and as a function of the fractional momenta x_gamma and x_p carried by the partons entering the hard scattering process. The correlation between the photon and the jet is also studied. The results are compared with QCD predictions based on the collinear and on the k_T factorisation approaches.
Measured inclusive prompt photon cross section in the defined phase space.
Measured prompt photon plus jet cross section in the defined phase space.
Bin averaged differential cross section as a function of ET in the defined phase space.
Bin averaged differential cross section as a function of ET in the defined phase space.
Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range -1.00 to -0.57.
Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range -0.57 to 0.20.
Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range 0.20 to 0.94.
Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range 0.94 to 1.42.
Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range 1.42 to 2.43.
Bin averaged differential cross section for prompt photon plus jet as a function of the photon transverse energy.
Bin averaged differential cross section for prompt photon plus jet as a function of the photon pseudorapidity.
Bin averaged differential cross section for prompt photon plus jet as a function of the jet transverse energy.
Bin averaged differential cross section for prompt photon plus jet as a function of the jet pseudorapidity.
Bin averaged differential cross section for prompt photon plus jet as a function of X(C=GAMMA,LO) thelongitudinal momentum fraction of the partons in the photon in LO approximation.
Bin averaged differential cross section for prompt photon plus jet as a function of X(C=P,LO) thelongitudinal momentum fraction of the partons in the proton in LO approximation.
Bin averaged differential cross section for prompt photon plus jet as a function of the photons transverse momentum perpendicular to the jet direction separated into two regions of X(C=GAMMA,LO).
Bin averaged differential cross section for prompt photon plus jet as a function of the difference in azimuthal angle between the photon and the jet separated into two regions of X(C=GAMMA,LO).
Beauty production in deep inelastic scattering with events in which a muon and a jet are observed in the final state has been measured with the ZEUS detector at HERA using an integrated luminosity of 114 pb^-1. The fraction of events with beauty quarks in the data was determined using the distribution of the transverse momentum of the muon relative to the jet. The cross section for beauty production was measured in the kinematic range of photon virtuality, Q^2 > 2 Gev^2, and inelasticity, 0.05 < y < 0.7, with the requirement of a muon and a jet. Total and differential cross sections are presented and compared to QCD predictions. The beauty contribution to the structure function F_2 was extracted and is compared to theoretical predictions.
Total visible cross section for BBAR production and decay into MUON+JET.
Measured differential cross section as a function of Q**2.
Measured differential cross section as a function of the muon transverse momentum.
Measured differential cross section as a function of the muon pseudorapidity.
Measured differential cross section as a function of the jet transverse momentum.
Measured differential cross section as a function of the jet pseudorapidity.
Measured cross sections for beauty production with a muon and jet for the Q**2 bin 2 to 4 GeV**2.
Measured cross sections for beauty production with a muon and jet for the Q**2 bin 4 to 20 GeV**2.
Measured cross sections for beauty production with a muon and jet for the Q**2 bin 20 to 45 GeV**2.
Measured cross sections for beauty production with a muon and jet for the Q**2 bin 45 to 100 GeV**2.
Measured cross sections for beauty production with a muon and jet for the Q**2 bin 100 to 250 GeV**2.
Measured cross sections for beauty production with a muon and jet for the Q**2 bin 250 to 3000 GeV**2.
Extracted values of F2 for B-BBAR production at an X value of 0.00013. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.
Extracted values of F2 for B-BBAR production at an X value of 0.0002. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.
Extracted values of F2 for B-BBAR production at an X value of 0.0005. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.
Extracted values of F2 for B-BBAR production at an X value of 0.002. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.
Extracted values of F2 for B-BBAR production at an X value 0.005.
Extracted values of F2 for B-BBAR production at an X value of 0.013. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.
We report on double-differential inclusive cross-sections of the production of secondary protons, charged pions, and deuterons, in the interactions with a 5% nuclear interaction length thick stationary carbon target, of proton and pion beams with momentum from \pm 3 GeV/c to \pm 15 GeV/c. Results are given for secondary particles with production angles between 20 and 125 degrees. Cross-sections on carbon nuclei are compared with cross-sections on beryllium, copper, tantalum and lead nuclei.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 20 to 30 degrees.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 30 to 45 degrees.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 45 to 60 degrees.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 65 to 90 degrees.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 90 to 125 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Charged particle production has been studied in neutral current deep inelastic ep scattering with the ZEUS detector at HERA using an integrated luminosity of 0.44 fb^-1. Distributions of scaled momenta in the Breit frame are presented for particles in the current fragmentation region. The evolution of these spectra with the photon virtuality, Q^2, is described in the kinematic region 10<Q^2<41000 GeV^2. Next-to-leading-order and modified leading-log-approximation QCD calculations as well as predictions from Monte Carlo models are compared to the data. The results are also compared to e+e- annihilation data. The dependences of the pseudorapidity distribution of the particles on Q^2 and on the energy in the \gamma p system, W, are presented and interpreted in the context of the hypothesis of limiting fragmentation.
Bin averaged scaled momentum spectra in the Q**2 ranges 160 to 320 and 320 to 640 GeV**2.
Bin averaged scaled momentum spectra in the Q**2 ranges 640 to 1280 and 1280 to 2560 GeV**2.
Bin averaged scaled momentum spectra in the Q**2 ranges 2560 to 5120 and 51200 to 10240 GeV**2.
Bin averaged scaled momentum spectra in the Q**2 range 10240 to 20480 GeV**2.
Bin averaged scaled momentum spectra in the Q**2 range 20480 to 40960 GeV**2.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0 to 0.02.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.02 to 0.05.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.05 to 0.1.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.1 to 0.2.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.2 to 0.3.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.3 to 0.4.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.4 to 0.5.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.5 to 0.7.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.7 to 1.0.
The normalized charged particle density for the Q**2 range 5120 to 10240 GeV in three W ranges.
The normalized charged particle density for the Q**2 range 2560 to 5120 GeV in three W ranges.
The normalized charged particle density for the Q**2 range 1280 to 2560 GeV in four W ranges.
The normalized charged particle density for the Q**2 range 640 to 1280 GeV in four W ranges.
The normalized charged particle density for the Q**2 range 320 to 640GeV in three W ranges.
The normalized charged particle density for the Q**2 range 160 to 320 GeV in four W ranges.
The normalized charged particle density for the Q**2 range 60 to 160 GeV in three W ranges.
The normalized charged particle density for the Q**2 range 50 to 60 GeV in three W ranges.
The normalized charged particle density for the Q**2 range 40 to 50 GeV in three W ranges.
The normalized charged particle density for the Q**2 range 30 to 40 GeV in three W ranges.
The normalized charged particle density for the Q**2 range 20 to 30 GeV in two W ranges.
The normalized charged particle density for the Q**2 range 10 to 20 GeV in two W ranges.
A measurement of the underlying activity in scattering processes with transverse momentum scale in the GeV region is performed in proton-proton collisions at sqrt(s) = 0.9 TeV, using data collected by the CMS experiment at the LHC. Charged hadron production is studied with reference to the direction of a leading object, either a charged particle or a set of charged particles forming a jet. Predictions of several QCD-inspired models as implemented in PYTHIA are compared, after full detector simulation, to the data. The models generally predict too little production of charged hadrons with pseudorapidity eta < 2, p_T > 0.5 GeV/c, and azimuthal direction transverse to that of the leading object.
Average multiplicity of charged particles per unit of pseudorapidity as a function of pseudorapidity for events with leading track-jet transverse momenta > 1 and > 3 GeV. Statistical errors only.
Average scalar sum of the transverse momenta of charged particles per unit of pseusdorapidity and per radian as a function of DELTA(PHI) for events with leading track-jet transverse momenta > 1 and > 2 GeV. Statistical errors only. Typical systematic error of 1.8 PCT at a leading track-jet PT of 3.5 GeV.
The average multiplicity and average scalar sum of transverse momenta of charge particles per unit of pseudorapidity and per radian as a function of the leading track transverse momenta. Statistical errors only. Typical systematic error of 1.8 PCT at a leading track-jet PT of 3.5 GeV.
The average multiplicity and average scalar sum of transverse momenta of charge particles per unit of pseudorapidity and per radian as a function of the leading track-jet transverse momenta. Statistical errors only. Typical systematic error of 1.8 PCT at a leading track-jet PT of 3.5 GeV.
The normalized multiplicity distribution (PROB) of charged particles. Statistical error only. Typical systematic error of 2.3 PCT at a multiplicity of 4.
The normalized distribution of the scalar sum of the transverse momenta of charged particles. Statistical errors only. Typical systematic error of 1.6 PCT at a SUM(PT) of 4.5 GeV.
The transverse momenta spectrum of charged particles. Statistical error only. Typical systematic error of 2.0 PCT at a PT of 1 GeV.
The production of leading neutrons, where the neutron carries a large fraction x_L of the incoming proton's longitudinal momentum, is studied in deep-inelastic positron-proton scattering at HERA. The data were taken with the H1 detector in the years 2006 and 2007 and correspond to an integrated luminosity of 122 pb^{-1}. The semi-inclusive cross section is measured in the phase space defined by the photon virtuality 6 < Q^2 < 100 GeV^2, Bjorken scaling variable 1.5x10^{-4} < x < 3x10^{-2}, longitudinal momentum fraction 0.32 < x_L < 0.95 and neutron transverse momentum p_T < 0.2 GeV. The leading neutron structure function, F_2^{LN(3)}(Q^2,x,x_L), and the fraction of deep-inelastic scattering events containing a leading neutron are studied as a function of Q^2, x and x_L. Assuming that the pion exchange mechanism dominates leading neutron production, the data provide constraints on the shape of the pion structure function.
Differential cross section of leading neutron production.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The inclusive double-spin asymmetry, $A^p_1$, has been measured at COMPASS in deepinelastic polarised muon scattering off a large polarised NH3 target. The data, collected in the year 2007, cover the range $Q^2 > 1 (GeV/c)^2, 0.004 < x < 0.7$ and improve the statistical precision of $g^p_1(x)$ by a factor of two in the region $x < 0.02$. The new proton asymmetries are combined with those previously published for the deuteron to extract the non-singlet spin-dependent structure function $g^{NS}_1(x,Q^2)$. The isovector quark density, $\Delta_{q3}(x,Q^2)$, is evaluated from a NLO QCD fit of $g^{NS}_1$. The first moment of $\Delta_{q3}$ is in good agreement with the value predicted by the Bjorken sum rule and corresponds to a ratio of the axial and vector coupling constants $|g_A/g_V$ = $1.28\pm 0.07(stat)\pm 0.10$(syst).
Values of A1P and G1P as a function of X with corresponding average values of Q**2.
Values of $A_1^p$ and $g_1^p$ as a function of $x$ with corresponding average values of $Q^2$.
Values of $g_1^p$ for the 2007 COMPASS proton data at 160 GeV in ($x$, $Q^2$) bins.
We present the results of an elliptic flow analysis of Cu+Cu collisions recorded with the STAR detector at 62.4 and 200GeV. Elliptic flow as a function of transverse momentum is reported for different collision centralities for charged hadrons and strangeness containing hadrons $K_{S}^{0}$, $\Lambda$, $\Xi$, $\phi$ in the midrapidity region $|eta|<1.0$. Significant reduction in systematic uncertainty of the measurement due to non-flow effects has been achieved by correlating particles at midrapidity, $|\eta|<1.0$, with those at forward rapidity, $2.5<|\eta|<4.0$. We also present azimuthal correlations in p+p collisions at 200 GeV to help estimating non-flow effects. To study the system-size dependence of elliptic flow, we present a detailed comparison with previously published results from Au+Au collisions at 200 GeV. We observe that $v_{2}$($p_{T}$) of strange hadrons has similar scaling properties as were first observed in Au+Au collisions, i.e.: (i) at low transverse momenta, $p_T<2GeV/c$, $v_{2}$ scales with transverse kinetic energy, $m_{T}-m$, and (ii) at intermediate $p_T$, $2<p_T<4GeV/c$, it scales with the number of constituent quarks, $n_q$. We have found that ideal hydrodynamic calculations fail to reproduce the centrality dependence of $v_{2}$($p_{T}$) for $K_{S}^{0}$ and $\Lambda$. Eccentricity scaled $v_2$ values, $v_{2}/\epsilon$, are larger in more central collisions, suggesting stronger collective flow develops in more central collisions. The comparison with Au+Au collisions which go further in density shows $v_{2}/\epsilon$ depend on the system size, number of participants $N_{part}$. This indicates that the ideal hydrodynamic limit is not reached in Cu+Cu collisions, presumably because the assumption of thermalization is not attained.
Charged hadron azimuthal correlations as a function of pT in 0-60% Cu+Cu and p+p collisions at 200 GeV using TPC and FTPC flow vectors.
Charged hadron azimuthal anisotropy v2 as a function of pT in 0-60% Cu+Cu collisions at 200 GeV using TPC flow vectors, and those with subtracting the azimuthal correlations in p+p collisions.
Charged hadron azimuthal anisotropy v2 as a function of pT in 0-60% Cu+Cu collisions at 200 GeV using FTPC flow vectors, and those with subtracting the azimuthal correlations in p+p collisions.
Charged hadron azimuthal anisotropy v2 as a function of pT in 50-60% Cu+Cu collisions at 200 GeV using FTPC flow vectors, and that with subtracting the azimuthal correlations in p+p collisions.
Charged hadron azimuthal anisotropy v2 as a function of pT in 40-50% Cu+Cu collisions at 200 GeV using FTPC flow vectors, and that with subtracting the azimuthal correlations in p+p collisions.
Charged hadron azimuthal anisotropy v2 as a function of pT in 30-40% Cu+Cu collisions at 200 GeV using FTPC flow vectors, and that with subtracting the azimuthal correlations in p+p collisions.
Charged hadron azimuthal anisotropy v2 as a function of pT in 20-30% Cu+Cu collisions at 200 GeV using FTPC flow vectors, and that with subtracting the azimuthal correlations in p+p collisions.
Charged hadron azimuthal anisotropy v2 as a function of pT in 10-20% Cu+Cu collisions at 200 GeV using FTPC flow vectors, and that with subtracting the azimuthal correlations in p+p collisions.
Charged hadron azimuthal anisotropy v2 as a function of pT in 0-10% Cu+Cu collisions at 200 GeV using FTPC flow vectors, and that with subtracting the azimuthal correlations in p+p collisions.
Charged hadron azimuthal anisotropy v2 integrated over pT and eta vs centrality in Cu+Cu collisions at 200 GeV for the various methods.
Charged hadron azimuthal anisotropy v2 integrated over pT and eta vs centrality in Cu+Cu collisions at 62.4 GeV for the various methods.
Charged hadron azimuthal anisotropy v2 as a function of pT in 50-60% Cu+Cu collisions at 62.4 GeV. Data tables for 200 GeV are shown in Fig.4.
Charged hadron azimuthal anisotropy v2 as a function of pT in 40-50% Cu+Cu collisions at 62.4 GeV using FTPC flow vectors. Data tables for 200 GeV are shown in Fig.4.
Charged hadron azimuthal anisotropy v2 as a function of pT in 30-40% Cu+Cu collisions at 62.4 GeV using FTPC flow vectors. Data tables for 200 GeV are shown in Fig.4.
Charged hadron azimuthal anisotropy v2 as a function of pT in 20-30% Cu+Cu collisions at 62.4 GeV using FTPC flow vectors. Data tables for 200 GeV are shown in Fig.4.
Charged hadron azimuthal anisotropy v2 as a function of pT in 10-20% Cu+Cu collisions at 62.4 GeV using FTPC flow vectors. Data tables for 200 GeV are shown in Fig.4.
Charged hadron azimuthal anisotropy v2 as a function of pT in 0-10% Cu+Cu collisions at 62.4 GeV using FTPC flow vectors. Data tables for 200 GeV are shown in Fig.4.
Charged hadron azimuthal anisotropy v2 as a function of pT in 0-60% Cu+Cu collisions at 62.4 GeV using FTPC flow vectors. Data tables for 200 GeV are shown in Fig.3.
K0S azimuthal anisotropy v2 vs pT in 0-60% central Cu+Cu collisions at 200 GeV.
K0S azimuthal anisotropy v2 vs pT in 0-20% central Cu+Cu collisions at 200 GeV.
K0S azimuthal anisotropy v2 vs pT in 20-60% central Cu+Cu collisions at 200 GeV.
Lambda azimuthal anisotropy v2 vs pT in 0-60% central Cu+Cu collisions at 200 GeV.
Lambda azimuthal anisotropy v2 vs pT in 0-20% central Cu+Cu collisions at 200 GeV.
Lambda azimuthal anisotropy v2 vs pT in 20-60% central Cu+Cu collisions at 200 GeV.
Xi azimuthal anisotropy v2 vs pT in 0-60% central Cu+Cu collisions at 200 GeV.
phi azimuthal anisotropy v2 vs pT in 0-60% central Cu+Cu collisions at 200 GeV.
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