Showing 10 of 17 results
Measurements of hadron production in p+C interactions at 31 GeV/c are performed using the NA61/ SHINE spectrometer at the CERN SPS. The analysis is based on the full set of data collected in 2009 using a graphite target with a thickness of 4% of a nuclear interaction length. Inelastic and production cross sections as well as spectra of $\pi^\pm$, $K^\pm$, p, $K^0_S$ and $\Lambda$ are measured with high precision. These measurements are essential for improved calculations of the initial neutrino fluxes in the T2K long-baseline neutrino oscillation experiment in Japan. A comparison of the NA61/SHINE measurements with predictions of several hadroproduction models is presented.
The double differential $\pi^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\pi^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^+$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^-$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential proton production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential proton production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential proton production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential proton production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential proton production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential proton production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential proton production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential proton production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential proton production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential proton production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^0_S$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^0_S$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^0_S$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^0_S$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^0_S$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^0_S$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $K^0_S$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\Lambda$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\Lambda$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\Lambda$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\Lambda$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\Lambda$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\Lambda$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\Lambda$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
The double differential $\Lambda$ production cross section in the laboratory system for p+C interactions at 31 GeV$/c$. The results are presented as a function of momentum, $p$ (in [GeV/$c$]), in different angular intervals, $\theta$ (in [mrad]). The statistical and systematic errors are quoted.
Spectra of positively charged kaons in p+C interactions at 31 GeV/c were measured with the NA61/SHINE spectrometer at the CERN SPS. The analysis is based on the full set of data collected in 2007 with a graphite target with a thickness of 4% of a nuclear interaction length. Interaction cross sections and charged pion spectra were already measured using the same set of data. These new measurements in combination with the published ones are required to improve predictions of the neutrino flux for the T2K long baseline neutrino oscillation experiment in Japan. In particular, the knowledge of kaon production is crucial for precisely predicting the intrinsic electron neutrino component and the high energy tail of the T2K beam. The results are presented as a function of laboratory momentum in 2 intervals of the laboratory polar angle covering the range from 20 up to 240 mrad. The kaon spectra are compared with predictions of several hadron production models. Using the published pion results and the new kaon data, the K+/\pi+ ratios are computed.
The measured K+ production cross section and the K+/PI+ cross section ratio for the angular range 20 to 140 mrad. The errors on the ratios are statistical only.
The measured K+ production cross section and the K+/PI+ cross section ratio for the angular range 140 to 240 mrad. The errors on the ratios are statistical only.
Measurements of the $\pi^{\pm}$, $K^{\pm}$, and proton double differential yields emitted from the surface of the 90-cm-long carbon target (T2K replica) were performed for the incoming 31 GeV/c protons with the NA61/SHINE spectrometer at the CERN SPS using data collected during 2010 run. The double differential $\pi^{\pm}$ yields were measured with increased precision compared to the previously published NA61/SHINE results, while the $K^{\pm}$ and proton yields were obtained for the first time. A strategy for dealing with the dependence of the results on the incoming proton beam profile is proposed. The purpose of these measurements is to reduce significantly the (anti)neutrino flux uncertainty in the T2K long-baseline neutrino experiment by constraining the production of (anti)neutrino ancestors coming from the T2K target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 120 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 120 to 140 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 160 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 160 to 180 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 200 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 200 to 220 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 340 to 380 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged pions emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of positively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 120 to 180 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 280 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 60 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of negatively charged kaons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 120 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 100 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 300 to 380 mrad and in the longitudinal range from 0 to 18cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 100 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 300 to 380 mrad and in the longitudinal range from 18 to 36cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 100 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 300 to 380 mrad and in the longitudinal range from 36 to 54cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 100 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 300 to 380 mrad and in the longitudinal range from 54 to 72cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 100 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 300 to 380 mrad and in the longitudinal range from 72 to 89.99cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 60 to 100 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Double differential yiedls of protons emitted from the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and in the longitudinal range from 89.99 to 90.01cm, as a function of momentum. The normalization is per proton on target.
Measurements of particle emission from a replica of the T2K 90 cm-long carbon target were performed in the NA61/SHINE experiment at CERN SPS, using data collected during a high-statistics run in 2009. An efficient use of the long-target measurements for neutrino flux predictions in T2K requires dedicated reconstruction and analysis techniques. Fully-corrected differential yields of $\pi^\pm$-mesons from the surface of the T2K replica target for incoming 31 GeV/c protons are presented. A possible strategy to implement these results into the T2K neutrino beam predictions is discussed and the propagation of the uncertainties of these results to the final neutrino flux is performed.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of positively charged pions at the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and for longitudinal bin $z1$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and for longitudinal bin $z2$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and for longitudinal bin $z3$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and for longitudinal bin $z4$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and for longitudinal bin $z5$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 0 to 20 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 20 to 40 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 40 to 60 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 60 to 80 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 80 to 100 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 100 to 140 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 140 to 180 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 180 to 220 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 220 to 260 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 260 to 300 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Spectra of negatively charged pions at the surface of the T2K replica target, in the polar angle range from 300 to 340 mrad and for longitudinal bin $z6$, as a function of momentum. The normalization is per proton on target.
Interaction cross sections and charged pion spectra in p+C interactions at 31 GeV/c were measured with the large acceptance NA61/SHINE spectrometer at the CERN SPS. These data are required to improve predictions of the neutrino flux for the T2K long baseline neutrino oscillation experiment in Japan. A set of data collected during the first NA61/SHINE run in 2007 with an isotropic graphite target with a thickness of 4% of a nuclear interaction length was used for the analysis. The measured p+C inelastic and production cross sections are 257.2 +- 1.9 +- 8.9 mb and 229.3 +- 1.9 +- 9.0 mb, respectively. Inclusive production cross sections for negatively and positively charged pions are presented as a function of laboratory momentum in 10 intervals of the laboratory polar angle covering the range from 0 up to 420 mrad. The spectra are compared with predictions of several hadron production models.
The total inelastic cross section and production cross sections. The latter are obtained from the former by subtraction of the quasi-elastic contribution.
The differential PI+ PI- production cross section in the lab. system for the angular range 0 to 20 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 20 to 40 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 40 to 60 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 60 to 100 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 100 to 140 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 140 to 180 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 180 to 240 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 240 to 300 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 300 to 360 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 360 to 420 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 0 to 20 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 20 to 40 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 40 to 60 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 60 to 100 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 100 to 140 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 140 to 180 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 180 to 240 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 240 to 300 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 300 to 360 mrad.
The differential PI+ PI- production cross section in the lab. system for the angular range 360 to 420 mrad.
The fixed-target MIPP experiment, Fermilab E907, was designed to measure the production of hadrons from the collisions of hadrons of momenta ranging from 5 to 120 GeV/c on a variety of nuclei. These data will generally improve the simulation of particle detectors and predictions of particle beam fluxes at accelerators. The spectrometer momentum resolution is between 3 and 4%, and particle identification is performed for particles ranging between 0.3 and 80 GeV/c using $dE/dx$, time-of-flight and Cherenkov radiation measurements. MIPP collected $1.42 \times10^6$ events of 120 GeV Main Injector protons striking a target used in the NuMI facility at Fermilab. The data have been analyzed and we present here charged pion yields per proton-on-target determined in bins of longitudinal and transverse momentum between 0.5 and 80 GeV/c, with combined statistical and systematic relative uncertainties between 5 and 10%.
The production yields of PI+ and PI- and the ratio of these yields. The first uncertainty given on each value combines statistical uncertainties and systematic uncertainties from backgrounds.
The analyzing powers of π+ and π− were measured using an incident 22−GeV/c transversely polarized proton beam at the Brookhaven Alternating Gradient Synchrotron. A magnetic spectrometer measured π± inclusive asymmetries on a hydrogen and a carbon target. An elastic polarimeter with a CH2 target measured pp elastic-scattering asymmetries to determine the beam polarization using published data for the pp elastic analyzing power. Using the beam polarization determined from the elastic polarimeter and asymmetries from the inclusive spectrometer, analyzing powers AN for π± were determined in the xF and pT ranges (0.45–0.8) and (0.3–1.2 GeV/c), respectively. The analyzing power results are similar in both sign and character to other measurements at 200 and 11.7 GeV/c, confirming the expectation that high-energy pion inclusive analyzing powers remain large and relatively energy independent. This suggests that pion inclusive polarimetry may be a suitable method for measuring future beam polarizations at BNL RHIC or DESY HERA. Analyzing powers of π+ and π− produced on hydrogen and carbon targets are the same. Various models to explain inclusive analyzing powers are also discussed.
Analyzing power measurements for PI+ and PI- production on the carbon target at incident momentum 21.6 GeV. See text of article for definitions of method 'A' and 'B'.
Analyzing power measurements for inclusive PI- production from the hydrogen target.
Analyzing power measurements for inclusive PI+ production from the hydrogen target.
Analyzing power measurement for inclusive proton production from the carbon target using method A.
Analyzing power measurements for PI- PI+ and proton production with the carbon target.
Analyzing power measurements for PI- and PI+ production with the hydrogen target.
Analyzing power measurements for PI- and PI+ production using a CH2 target.
Double differential K+cross sections have been measured in p+C collisions at 1.2, 1.5 and 2.5 GeV beam energy and in p+Pb collisions at 1.2 and 1.5 GeV. The K+ spectrum taken at 2.5 GeV can be reproduced quantitatively by a model calculation which takes into account first chance proton-nucleon collisions and internal momentum with energy distribution of nucleons according to the spectral function. At 1.2 and 1.5 GeV beam energy the K+ data excess significantly the model predictions for first chance collisions. When taking secondary processes into account the results of the calculations are in much better agreement with the data.
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The excitation of theΔ resonance is observed in proton collisions on C, Nb and Pb targets at 0.8 and 1.6 GeV incident energies. The mass E0 and widthΓ of the resonance are determined from the invariant mass spectra of correlated (p, π±)-pairs in the final state of the collision: The mass E0 is smaller than that of the free resonance, however by comparing to intra-nuclear cascade calculations, this reduction is traced back to the effects of Fermi motion, NN scattering and pion reabsorption in nuclear matter.
WITHIN THE DETECTORS ACCEPTANCE RESULTS.
WITHIN THE DETECTORS ACCEPTANCE RESULTS.
WITHIN THE DETECTORS ACCEPTANCE RESULTS.
WITHIN THE DETECTORS ACCEPTANCE RESULTS.
WITHIN THE DETECTORS ACCEPTANCE RESULTS.
WITHIN THE DETECTORS ACCEPTANCE RESULTS.
WITHIN THE DETECTORS ACCEPTANCE RESULTS.
WITHIN THE DETECTORS ACCEPTANCE RESULTS.
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WITHIN THE DETECTORS ACCEPTANCE RESULTS.
WITHIN THE DETECTORS ACCEPTANCE RESULTS.
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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.
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