The \sigma(E_{\nu}) results from Figure 20 are given with the total uncertainty. Each row is a bin of neutrino energy (MeV) labeled according to its low edge. Bin (MeV) | Result (10^{-39} cm^2) 500 | 6.1 +/- 0.8 600 | 11.5 +/- 1.3 650 | 15.8 +/- 1.7 700 | 19.6 +/- 2.1 750 | 24.1 +/- 2.5 800 | 28.3 +/- 2.9 850 | 32.5 +/- 3.3 900 | 37.3 +/- 3.9 950 | 41.6 +/- 4.4 1000 | 46.6 +/- 5.0 1050 | 49.7 +/- 5.6 1100 | 52.9 +/- 6.1 1150 | 56.3 +/- 7.0 1200 | 59.1 +/- 7.6 1250 | 62.3 +/- 8.4 1300 | 66.7 +/- 9.4 1350 | 70.3 +/- 10.5 1400 | 72.3 +/- 11.4 1450 | 77.6 +/- 12.8 1500 | 80.8 +/- 13.9 1550 | 83.7 +/- 14.9 1600 | 86.4 +/- 15.9 1650 | 88.5 +/- 16.9 1700 | 93.0 +/- 18.5 1750 | 92.6 +/- 19.3 1800 | 97.1 +/- 21.4 1900 | 99.2 +/- 23.7 The \partial\sigma/\partial(KE_{\pi}) results from Figure 23 are given with the total uncertainty. Each row is a bin of pion kinetic energy (MeV) labeled according to its low edge. Bin (MeV) | Result (10^{-41} cm^2/MeV) 0 | 3.6 +/- 0.5 50 | 8.9 +/- 1.2 75 | 10.8 +/- 1.4 100 | 10.8 +/- 1.2 125 | 9.7 +/- 1.2 150 | 8.6 +/- 1.1 175 | 7.6 +/- 1.1 200 | 7.0 +/- 1.0 225 | 6.1 +/- 1.0 250 | 5.3 +/- 0.9 275 | 4.5 +/- 0.8 300 | 3.9 +/- 0.7 325 | 3.2 +/- 0.6 350 | 2.7 +/- 0.5 375 | 2.3 +/- 0.4 The \partial\sigma/\partial(Q^2) results from Figure 21 are given with the total uncertainty. Each row is a bin of Q^2 (GeV^2/c^4) labeled according to its low edge. Bin (GeV^2/c^4) | Result (10^{-45} cm^2 c^4/MeV^2) 0.00 | 36.2 +/- 6.7 0.05 | 55.8 +/- 7.8 0.10 | 56.1 +/- 7.5 0.15 | 53.4 +/- 7.0 0.20 | 47.8 +/- 6.4 0.25 | 43.2 +/- 5.9 0.30 | 38.8 +/- 5.3 0.35 | 34.1 +/- 4.8 0.40 | 30.3 +/- 4.3 0.45 | 26.1 +/- 3.7 0.50 | 22.9 +/- 3.3 0.55 | 19.8 +/- 2.9 0.60 | 17.3 +/- 2.5 0.65 | 14.8 +/- 2.1 0.70 | 12.9 +/- 1.9 0.75 | 11.0 +/- 1.7 0.80 | 9.3 +/- 1.4 0.85 | 8.0 +/- 1.3 0.90 | 6.8 +/- 1.1 0.95 | 5.3 +/- 1.0 1.05 | 3.9 +/- 0.7 1.15 | 2.5 +/- 0.5 1.30 | 1.4 +/- 0.4 The \partial\sigma/\partial(KE_{\mu}) results from Figure 22 are given with the total uncertainty. Each row is a bin of muon kinetic energy (MeV) labeled according to its low edge. Bin (MeV) | Result (10^{-42} cm^2/MeV) 0 | 23.1 +/- 3.2 50 | 34.4 +/- 5.0 100 | 39.0 +/- 5.8 150 | 41.6 +/- 6.2 200 | 41.2 +/- 6.1 250 | 39.0 +/- 5.7 300 | 37.3 +/- 5.4 350 | 35.0 +/- 4.9 400 | 32.0 +/- 4.4 450 | 28.8 +/- 3.8 500 | 26.1 +/- 3.5 550 | 23.2 +/- 3.1 600 | 20.8 +/- 2.8 650 | 18.6 +/- 2.5 700 | 15.9 +/- 2.1 750 | 14.2 +/- 2.0 800 | 12.3 +/- 1.8 850 | 10.7 +/- 1.6 900 | 9.3 +/- 1.4 950 | 7.7 +/- 1.3 1000 | 5.9 +/- 1.0 1100 | 4.3 +/- 0.8 1200 | 2.2 +/- 0.6 The \partial\sigma(E_{\nu})/\partial(Q^2) results from Figure 26 are shown (10^{-44}cm^2 c^4/MeV^2). Each bin is labeled according to its low edge. The columns are bins of neutrino energy (MeV) and the rows are bins of Q^2 (GeV^2/c^4). Empty bins indicate regions where no measurement has been made. Bin | 500 | 600 | 650 | 700 | 750 | 800 | 850 | 900 | 950 | 1000 | 1050 | 1100 | 1150 | 1200 | 1250 | 1300 | 1350 | 1400 | 1450 | 1500 | 1550 | 1600 | 1650 1.15 | | | | | | | | | | | | | | | | | 1.1 | 1.0 | 1.2 | | | | 1.05 | | | | | | | | | | | | | | 0.9 | 1.1 | 1.2 | 1.5 | 1.8 | 1.8 | | | | 0.95 | | | | | | | | | | | | | 1.1 | 1.4 | 1.7 | 2.0 | 2.2 | 2.3 | 2.3 | 2.6 | 3.1 | 3.1 | 0.90 | | | | | | | | | | | | | 1.6 | 2.0 | 2.0 | 2.3 | 2.4 | 2.8 | 3.4 | | | | 0.85 | | | | | | | | | | | 1.2 | 1.5 | 1.8 | 2.2 | 2.6 | 2.8 | 2.8 | 3.1 | 3.5 | | | | 0.80 | | | | | | | | | | 1.1 | 1.6 | 2.0 | 2.6 | 2.7 | 2.9 | 3.4 | 3.4 | 3.4 | 3.8 | | | | 0.75 | | | | | | | | | | 1.8 | 2.2 | 2.5 | 2.7 | 3.2 | 3.4 | 3.5 | 3.8 | 4.6 | 4.3 | 4.8 | | | 0.70 | | | | | | | | | 1.6 | 2.2 | 2.6 | 2.9 | 3.2 | 3.4 | 3.8 | 4.0 | 4.3 | 4.5 | 5.5 | 5.0 | 5.1 | | 0.65 | | | | | | | | 1.7 | 2.2 | 2.7 | 2.9 | 3.1 | 4.0 | 3.6 | 4.1 | 4.7 | 4.8 | 5.2 | 5.2 | 5.6 | 5.3 | | 0.60 | | | | | | | 1.4 | 2.4 | 2.4 | 3.3 | 3.7 | 4.1 | 4.2 | 4.5 | 5.2 | 5.4 | 5.2 | 5.0 | 5.9 | 6.0 | 5.6 | 6.3 | 0.55 | | | | | | 1.3 | 1.9 | 2.4 | 3.0 | 3.8 | 4.1 | 4.6 | 4.7 | 5.2 | 5.1 | 5.7 | 5.6 | 6.1 | 5.8 | 7.0 | 7.4 | 7.6 | 7.4 0.50 | | | | | | 1.8 | 2.4 | 3.2 | 3.6 | 4.4 | 4.8 | 5.4 | 5.6 | 5.8 | 5.8 | 6.7 | 6.6 | 6.6 | 7.0 | 6.2 | 7.5 | 7.3 | 7.1 0.45 | | | | | 1.5 | 2.3 | 3.1 | 4.0 | 4.7 | 5.2 | 5.7 | 5.5 | 6.1 | 6.5 | 6.4 | 6.6 | 6.9 | 7.7 | 7.1 | 7.4 | 6.6 | 7.9 | 8.1 0.40 | | | | 1.3 | 2.5 | 3.2 | 4.2 | 4.8 | 5.1 | 6.1 | 6.5 | 6.7 | 6.7 | 7.1 | 7.1 | 7.3 | 7.5 | 7.1 | 8.1 | 7.9 | 8.6 | 8.4 | 9.3 0.35 | | | 1.1 | 2.0 | 3.1 | 4.0 | 4.8 | 5.7 | 6.4 | 6.8 | 6.8 | 7.0 | 7.4 | 7.8 | 7.6 | 8.2 | 8.1 | 8.1 | 8.7 | 9.1 | 8.7 | 8.9 | 8.8 0.30 | | | 1.9 | 3.1 | 4.1 | 5.1 | 6.0 | 6.1 | 7.4 | 7.4 | 7.4 | 8.0 | 8.0 | 8.1 | 8.6 | 9.1 | 9.2 | 9.0 | 8.7 | 8.7 | 8.9 | 8.7 | 9.8 0.25 | | 1.8 | 3.0 | 4.1 | 5.3 | 5.9 | 6.7 | 6.8 | 7.5 | 7.7 | 8.2 | 8.2 | 8.1 | 8.5 | 9.0 | 9.0 | 9.8 | 9.4 | 9.4 | 8.8 | 9.5 | 9.7 | 10.1 0.20 | 1.0 | 2.9 | 4.2 | 5.2 | 6.0 | 6.7 | 6.9 | 7.6 | 8.0 | 8.8 | 8.5 | 8.8 | 8.7 | 9.3 | 9.2 | 9.5 | 9.6 | 9.5 | 9.9 | 10.3 | 10.2 | 11.5 | 11.2 0.15 | 1.9 | 4.1 | 5.4 | 6.3 | 7.1 | 7.4 | 7.5 | 8.3 | 8.7 | 9.1 | 9.0 | 9.3 | 9.2 | 9.6 | 9.4 | 9.6 | 9.6 | 9.9 | 10.6 | 11.6 | 10.8 | 11.2 | 10.3 0.10 | 3.1 | 5.2 | 6.6 | 7.0 | 7.4 | 7.6 | 7.9 | 8.7 | 8.2 | 9.2 | 9.3 | 9.4 | 9.5 | 9.1 | 9.0 | 9.5 | 9.2 | 9.5 | 10.4 | 9.4 | 10.5 | 10.2 | 9.8 0.05 | 4.3 | 6.0 | 6.5 | 7.0 | 7.3 | 7.4 | 7.6 | 8.0 | 7.9 | 8.0 | 8.0 | 8.3 | 8.6 | 8.2 | 8.6 | 8.2 | 8.4 | 7.8 | 8.6 | 9.3 | 9.3 | 9.6 | 10.0 0.00 | 1.9 | 2.7 | 3.3 | 3.6 | 3.9 | 4.3 | 4.6 | 4.8 | 5.2 | 5.4 | 5.4 | 5.2 | 5.8 | 5.9 | 6.0 | 6.4 | 6.6 | 6.1 | 6.3 | 6.7 | 7.2 | | The percent uncertainty of the \partial\sigma(E_{\nu})/\partial(Q^2) results from Figure 26 is shown. Each bin is labeled according to its low edge. The columns are bins of neutrino energy (MeV) and the rows are bins of Q^2 (GeV^2/c^4). Empty bins indicate regions where no measurement has been made. Bin | 500 | 600 | 650 | 700 | 750 | 800 | 850 | 900 | 950 | 1000 | 1050 | 1100 | 1150 | 1200 | 1250 | 1300 | 1350 | 1400 | 1450 | 1500 | 1550 | 1600 | 1650 1.15 | | | | | | | | | | | | | | | | | 25.7 | 26.5 | 34.4 | | | | 1.05 | | | | | | | | | | | | | | 27.9 | 33.9 | 26.0 | 21.6 | 22.1 | 33.5 | | | | 0.95 | | | | | | | | | | | | | 22.7 | 23.5 | 20.8 | 21.9 | 21.5 | 21.5 | 20.6 | 25.1 | 22.0 | 21.9 | 0.90 | | | | | | | | | | | | | 21.8 | 25.5 | 22.6 | 19.8 | 21.7 | 21.1 | 22.8 | | | | 0.85 | | | | | | | | | | | 24.1 | 20.0 | 22.1 | 18.8 | 20.0 | 22.1 | 19.6 | 21.3 | 20.6 | | | | 0.80 | | | | | | | | | | 26.4 | 22.7 | 20.2 | 18.9 | 17.7 | 18.5 | 19.5 | 17.9 | 21.8 | 21.8 | | | | 0.75 | | | | | | | | | | 22.2 | 22.5 | 17.3 | 16.1 | 16.8 | 16.4 | 18.9 | 18.9 | 20.5 | 20.0 | 23.0 | | | 0.70 | | | | | | | | | 21.0 | 15.9 | 19.4 | 17.2 | 15.7 | 15.1 | 15.6 | 18.3 | 18.7 | 22.6 | 20.9 | 25.0 | 23.7 | | 0.65 | | | | | | | | 23.6 | 17.9 | 21.8 | 15.0 | 14.8 | 14.9 | 15.7 | 17.6 | 19.1 | 19.0 | 20.7 | 19.8 | 18.9 | 23.5 | | 0.60 | | | | | | | 25.6 | 24.0 | 15.3 | 16.3 | 14.7 | 13.6 | 16.4 | 15.5 | 17.0 | 18.2 | 17.7 | 18.0 | 19.9 | 22.2 | 25.7 | 23.2 | 0.55 | | | | | | 17.3 | 18.4 | 18.0 | 14.2 | 13.8 | 12.9 | 14.3 | 15.7 | 16.2 | 16.3 | 16.3 | 17.4 | 18.6 | 18.0 | 22.6 | 22.2 | 22.6 | 25.5 0.50 | | | | | | 22.0 | 14.5 | 14.3 | 13.3 | 12.8 | 14.2 | 14.8 | 15.3 | 14.3 | 15.5 | 16.7 | 17.7 | 19.7 | 19.1 | 21.4 | 22.7 | 25.2 | 29.9 0.45 | | | | | 19.7 | 13.9 | 13.4 | 13.1 | 13.3 | 13.5 | 13.9 | 13.9 | 14.4 | 16.7 | 15.3 | 16.4 | 16.9 | 18.2 | 19.0 | 20.8 | 22.8 | 27.1 | 29.2 0.40 | | | | 19.7 | 16.3 | 12.1 | 12.4 | 13.4 | 13.4 | 13.4 | 14.1 | 14.5 | 15.9 | 13.9 | 15.4 | 14.6 | 16.8 | 18.6 | 18.8 | 19.5 | 21.2 | 22.4 | 23.5 0.35 | | | 19.8 | 14.8 | 12.0 | 12.8 | 11.7 | 13.1 | 12.3 | 13.5 | 13.9 | 13.8 | 14.0 | 14.8 | 15.7 | 15.3 | 17.5 | 16.5 | 18.9 | 20.7 | 21.9 | 21.1 | 25.2 0.30 | | | 13.0 | 11.0 | 12.7 | 12.1 | 12.5 | 12.6 | 12.6 | 12.8 | 12.3 | 12.8 | 13.1 | 14.5 | 15.3 | 15.2 | 16.6 | 17.9 | 18.0 | 19.8 | 19.8 | 21.5 | 23.2 0.25 | | 14.1 | 12.3 | 12.8 | 11.9 | 12.0 | 11.9 | 11.7 | 11.6 | 11.9 | 11.9 | 12.7 | 13.7 | 13.9 | 14.4 | 15.4 | 16.8 | 17.0 | 18.7 | 18.6 | 19.3 | 23.2 | 22.4 0.20 | 14.8 | 13.3 | 11.2 | 11.5 | 11.6 | 11.2 | 11.1 | 11.1 | 11.5 | 12.3 | 12.8 | 12.7 | 13.4 | 14.3 | 14.8 | 15.2 | 15.0 | 17.0 | 18.2 | 18.2 | 21.7 | 22.8 | 27.1 0.15 | 10.9 | 10.6 | 11.2 | 11.0 | 10.9 | 11.1 | 10.9 | 12.0 | 11.8 | 11.9 | 12.4 | 12.3 | 13.7 | 14.0 | 15.0 | 14.4 | 16.4 | 16.2 | 19.4 | 19.0 | 20.6 | 21.7 | 22.6 0.10 | 10.3 | 11.2 | 10.8 | 10.9 | 11.2 | 12.1 | 11.9 | 11.5 | 12.1 | 11.9 | 12.0 | 12.1 | 13.6 | 14.5 | 14.8 | 15.7 | 16.1 | 16.7 | 17.6 | 18.4 | 19.0 | 21.5 | 23.1 0.05 | 12.2 | 12.8 | 12.2 | 13.9 | 13.8 | 13.3 | 12.8 | 11.8 | 11.9 | 11.7 | 12.8 | 13.0 | 13.7 | 14.8 | 15.8 | 17.5 | 18.4 | 21.1 | 20.4 | 19.1 | 21.4 | 20.9 | 23.9 0.00 | 20.0 | 18.6 | 19.1 | 18.9 | 17.7 | 17.2 | 16.2 | 14.9 | 14.8 | 13.6 | 15.8 | 15.3 | 14.9 | 14.7 | 15.3 | 17.3 | 20.9 | 20.7 | 21.9 | 24.0 | 21.2 | | The \partial\sigma(E_{\nu})/\partial(KE_{\mu}) results from Figure 27 are shown (10^{-41}cm^2/MeV). Each bin is labeled according to its low edge. The columns are bins of neutrino energy (MeV) and the rows are bins of muon kinetic energy (MeV). Empty bins indicate regions where no measurement has been made. Bin | 500 | 600 | 650 | 700 | 750 | 800 | 850 | 900 | 950 | 1000 | 1050 | 1100 | 1150 | 1200 | 1250 | 1300 | 1350 | 1400 | 1450 | 1500 | 1550 | 1600 | 1650 1200 | | | | | | | | | | | | | | | | | | | | | | | 1.9 1100 | | | | | | | | | | | | | | | | | | | | | 4.1 | 6.3 | 8.0 1000 | | | | | | | | | | | | | | | | | | 1.8 | 3.6 | 5.9 | 8.0 | 8.9 | 9.0 950 | | | | | | | | | | | | | | | | | 2.8 | 4.6 | 6.9 | 8.6 | 9.4 | 9.5 | 9.6 900 | | | | | | | | | | | | | | | | 2.5 | 4.9 | 6.9 | 8.8 | 9.4 | 9.8 | 9.1 | 9.5 850 | | | | | | | | | | | | | | | 2.5 | 4.2 | 6.8 | 8.4 | 9.1 | 10.3 | 9.7 | 9.5 | 9.1 800 | | | | | | | | | | | | | 1.2 | 2.4 | 4.7 | 7.1 | 7.9 | 9.5 | 9.4 | 9.6 | 9.5 | 8.5 | 9.2 750 | | | | | | | | | | | | 1.3 | 2.7 | 4.8 | 7.0 | 8.5 | 9.5 | 9.4 | 9.5 | 8.3 | 8.3 | 9.1 | 9.5 700 | | | | | | | | | | | 1.1 | 2.4 | 4.8 | 7.0 | 8.1 | 8.9 | 8.8 | 9.1 | 9.1 | 8.5 | 8.8 | 8.6 | 7.5 650 | | | | | | | | | | 1.2 | 2.5 | 4.6 | 6.9 | 8.4 | 9.7 | 9.7 | 9.9 | 9.2 | 8.9 | 8.0 | 8.1 | 7.3 | 7.4 600 | | | | | | | | | 1.2 | 2.5 | 4.8 | 7.0 | 8.7 | 9.1 | 9.0 | 9.1 | 9.2 | 9.3 | 8.4 | 8.4 | 7.8 | 7.9 | 550 | | | | | | | | 1.2 | 2.4 | 4.7 | 6.7 | 8.3 | 9.1 | 9.4 | 8.9 | 9.8 | 8.8 | 7.6 | 8.9 | 7.9 | 8.1 | 7.1 | 500 | | | | | | | 1.2 | 2.6 | 4.5 | 7.1 | 8.4 | 9.4 | 9.2 | 9.3 | 9.1 | 8.9 | 8.9 | 8.0 | 8.2 | 8.0 | 7.1 | 7.4 | 450 | | | | | | 1.1 | 2.4 | 4.5 | 7.1 | 8.3 | 9.1 | 9.8 | 9.7 | 9.0 | 8.7 | 8.6 | 8.2 | 8.9 | 7.4 | 7.7 | 7.6 | 6.3 | 400 | | | | | 1.0 | 2.2 | 4.3 | 7.0 | 8.7 | 9.6 | 9.9 | 9.4 | 8.9 | 9.1 | 9.1 | 8.4 | 7.9 | 7.5 | 7.9 | 7.0 | 6.5 | 6.2 | 350 | | | | 1.0 | 2.1 | 4.3 | 6.8 | 8.3 | 9.8 | 10.4 | 9.9 | 9.5 | 9.1 | 8.4 | 8.9 | 8.4 | 7.6 | 7.1 | 7.0 | 7.5 | 6.1 | | 300 | | 0.3 | 1.0 | 2.1 | 4.3 | 6.2 | 7.9 | 9.3 | 9.5 | 10.2 | 10.2 | 9.1 | 9.4 | 8.4 | 8.4 | 8.3 | 7.3 | 7.2 | 7.3 | 6.7 | 6.7 | | 250 | 0.2 | 0.9 | 2.0 | 3.9 | 6.2 | 7.8 | 8.5 | 9.5 | 9.8 | 9.4 | 9.4 | 9.0 | 8.5 | 8.3 | 7.6 | 7.7 | 6.7 | 6.8 | 6.6 | 6.0 | | | 200 | 0.5 | 1.8 | 4.0 | 6.0 | 7.7 | 8.5 | 9.3 | 9.5 | 9.6 | 9.3 | 8.9 | 8.3 | 8.0 | 7.5 | 6.8 | 6.4 | 6.8 | 6.0 | 5.7 | 5.8 | | | 150 | 1.3 | 3.7 | 5.7 | 7.6 | 8.5 | 9.3 | 9.3 | 8.9 | 8.5 | 8.2 | 7.5 | 7.4 | 6.7 | 6.7 | 6.2 | 5.7 | 5.4 | 4.7 | 4.9 | | | | 100 | 2.2 | 5.4 | 7.1 | 8.0 | 8.5 | 8.5 | 7.9 | 7.5 | 6.5 | 6.6 | 6.1 | 5.6 | 5.4 | 4.8 | 4.5 | 4.0 | 4.1 | | | | | | 50 | 4.0 | 6.7 | 7.5 | 7.2 | 7.0 | 6.2 | 5.6 | 5.1 | 4.5 | 4.2 | 3.9 | 3.6 | 3.4 | 3.2 | | | | | | | | | 0 | 4.5 | 4.8 | 4.6 | 3.8 | 3.5 | 3.1 | 2.7 | 2.6 | 2.4 | 2.4 | 2.2 | | | | | | | | | | | | The percent uncertainty of the \partial\sigma(E_{\nu})/\partial(KE_{\mu}) results from Figure 27 is shown. Each bin is labeled according to its low edge. The columns are bins of neutrino energy (MeV) and the rows are bins of muon kinetic energy (MeV). Empty bins indicate regions where no measurement has been made. Bin | 500 | 600 | 650 | 700 | 750 | 800 | 850 | 900 | 950 | 1000 | 1050 | 1100 | 1150 | 1200 | 1250 | 1300 | 1350 | 1400 | 1450 | 1500 | 1550 | 1600 | 1650 1200 | | | | | | | | | | | | | | | | | | | | | | | 28.6 1100 | | | | | | | | | | | | | | | | | | | | | 22.9 | 22.9 | 24.8 1000 | | | | | | | | | | | | | | | | | | 21.9 | 22.0 | 19.8 | 21.2 | 23.3 | 23.8 950 | | | | | | | | | | | | | | | | | 22.2 | 19.6 | 19.7 | 20.3 | 20.9 | 22.1 | 26.8 900 | | | | | | | | | | | | | | | | 19.2 | 19.5 | 20.1 | 19.5 | 20.1 | 22.4 | 23.3 | 25.2 850 | | | | | | | | | | | | | | | 20.7 | 19.0 | 17.9 | 17.9 | 18.8 | 19.8 | 23.3 | 23.7 | 25.9 800 | | | | | | | | | | | | | 21.2 | 20.6 | 19.9 | 16.8 | 17.4 | 17.7 | 19.2 | 21.5 | 22.0 | 24.5 | 25.8 750 | | | | | | | | | | | | 18.3 | 16.4 | 15.1 | 15.6 | 15.9 | 16.1 | 18.1 | 19.1 | 21.1 | 20.5 | 26.1 | 30.5 700 | | | | | | | | | | | 20.4 | 18.0 | 15.6 | 15.3 | 15.8 | 16.0 | 16.5 | 17.9 | 18.5 | 20.4 | 21.3 | 22.3 | 28.9 650 | | | | | | | | | | 20.0 | 18.4 | 15.6 | 15.1 | 14.3 | 15.3 | 16.1 | 18.0 | 17.9 | 19.6 | 21.0 | 21.9 | 22.0 | 25.8 600 | | | | | | | | | 15.8 | 14.9 | 13.6 | 12.9 | 13.9 | 15.6 | 14.9 | 15.5 | 17.2 | 19.2 | 20.1 | 20.8 | 22.6 | 25.6 | 550 | | | | | | | | 15.5 | 14.4 | 14.1 | 13.5 | 13.7 | 13.7 | 15.1 | 15.2 | 16.4 | 17.0 | 19.1 | 20.9 | 21.3 | 24.7 | 22.9 | 500 | | | | | | | 15.0 | 12.3 | 12.5 | 12.7 | 11.9 | 13.4 | 13.8 | 14.4 | 15.6 | 17.0 | 17.8 | 18.2 | 20.8 | 25.2 | 24.9 | 26.4 | 450 | | | | | | 17.0 | 13.7 | 12.3 | 11.8 | 10.8 | 11.7 | 12.3 | 13.5 | 14.2 | 14.8 | 15.5 | 16.4 | 19.2 | 19.2 | 21.7 | 23.0 | 22.8 | 400 | | | | | 18.8 | 16.3 | 13.7 | 11.8 | 11.5 | 11.5 | 11.8 | 12.3 | 13.8 | 13.7 | 16.5 | 16.8 | 17.0 | 18.7 | 20.9 | 20.5 | 23.5 | 23.9 | 350 | | | | 20.3 | 17.4 | 14.5 | 12.0 | 10.9 | 11.0 | 12.0 | 12.5 | 13.2 | 13.8 | 14.8 | 15.8 | 16.8 | 18.8 | 19.6 | 18.9 | 20.4 | 21.6 | | 300 | | 21.5 | 16.9 | 15.4 | 14.0 | 12.3 | 11.4 | 10.9 | 11.1 | 12.3 | 13.9 | 15.3 | 15.4 | 15.5 | 16.1 | 20.0 | 19.1 | 21.2 | 21.3 | 21.3 | 24.1 | | 250 | 22.5 | 16.5 | 13.6 | 12.6 | 12.0 | 11.9 | 10.4 | 11.0 | 11.7 | 12.4 | 13.3 | 14.7 | 15.6 | 16.3 | 18.4 | 17.4 | 19.4 | 22.9 | 22.8 | 23.0 | | | 200 | 18.2 | 14.1 | 11.7 | 10.4 | 10.7 | 10.8 | 10.9 | 12.3 | 12.2 | 12.7 | 14.4 | 15.0 | 16.2 | 17.7 | 17.9 | 20.0 | 19.3 | 19.4 | 21.4 | 24.2 | | | 150 | 14.6 | 12.6 | 10.8 | 10.7 | 11.0 | 11.5 | 11.3 | 12.0 | 13.4 | 13.7 | 15.4 | 14.8 | 15.7 | 17.0 | 18.9 | 18.7 | 20.3 | 21.7 | 20.6 | | | | 100 | 14.2 | 11.6 | 10.8 | 10.7 | 10.6 | 11.4 | 11.9 | 12.1 | 13.0 | 13.7 | 14.3 | 15.2 | 16.4 | 18.1 | 17.7 | 19.9 | 20.5 | | | | | | 50 | 13.3 | 12.9 | 11.2 | 12.0 | 11.9 | 11.7 | 13.8 | 14.9 | 13.9 | 15.4 | 16.7 | 17.5 | 17.9 | 18.5 | | | | | | | | | 0 | 12.8 | 11.9 | 13.5 | 12.7 | 14.3 | 14.6 | 15.6 | 16.2 | 16.9 | 18.2 | 18.4 | | | | | | | | | | | | The \partial\sigma(E_{\nu})/\partial(KE_{\pi}) results from Figure 28 are shown (10^{-41}cm^2/MeV). Each bin is labeled according to its low edge. The columns are bins of neutrino energy (MeV) and the rows are bins of pion kinetic energy (MeV). Empty bins indicate regions where no measurement has been made. Bin | 500 | 600 | 650 | 700 | 750 | 800 | 850 | 900 | 950 | 1000 | 1050 | 1100 | 1150 | 1200 | 1250 | 1300 | 1350 | 1400 | 1450 | 1500 | 1550 | 1600 | 1650 375 | | | | | | 1.6 | 1.8 | 2.3 | 2.7 | 3.5 | 4.3 | 4.8 | 5.1 | 5.2 | 6.0 | 6.8 | 7.0 | 7.5 | 8.0 | | | | 350 | | | | | 1.3 | 1.8 | 2.2 | 3.0 | 3.5 | 4.4 | 5.2 | 5.4 | 6.0 | 6.9 | 6.7 | 7.2 | 8.2 | 8.0 | 8.9 | 9.5 | | | 325 | | | | 1.1 | 1.9 | 2.6 | 3.2 | 4.0 | 5.0 | 5.2 | 6.0 | 7.0 | 6.8 | 7.5 | 7.9 | 8.6 | 9.2 | 10.1 | 10.9 | 10.9 | 11.5 | | 300 | | | 1.1 | 1.6 | 2.6 | 3.7 | 4.1 | 4.8 | 5.7 | 6.6 | 7.2 | 8.0 | 8.2 | 8.7 | 9.9 | 10.9 | 10.8 | 11.0 | 11.5 | 12.3 | 13.7 | 12.8 | 275 | | 0.9 | 1.6 | 2.7 | 3.6 | 4.4 | 5.2 | 6.4 | 7.3 | 7.8 | 8.4 | 8.7 | 9.4 | 10.4 | 10.6 | 11.7 | 10.9 | 12.0 | 14.4 | 13.5 | 14.2 | 15.8 | 13.6 250 | | 1.4 | 2.4 | 3.4 | 4.6 | 5.4 | 6.3 | 7.1 | 8.2 | 9.5 | 10.0 | 11.1 | 11.6 | 11.3 | 11.8 | 12.8 | 12.8 | 13.5 | 14.3 | 14.8 | 16.5 | 16.0 | 16.7 225 | 0.7 | 2.4 | 3.3 | 4.4 | 5.5 | 6.4 | 7.5 | 8.3 | 9.5 | 11.0 | 11.2 | 12.1 | 12.8 | 12.8 | 13.4 | 14.3 | 15.4 | 15.7 | 15.3 | 16.2 | 17.9 | 17.5 | 17.2 200 | 1.4 | 3.1 | 4.2 | 5.6 | 6.9 | 8.3 | 9.2 | 10.0 | 11.3 | 12.3 | 12.0 | 13.1 | 14.9 | 14.2 | 15.0 | 15.8 | 16.5 | 16.8 | 17.8 | 18.0 | 17.7 | 20.3 | 18.8 175 | 1.9 | 3.8 | 5.2 | 6.3 | 8.1 | 9.5 | 10.0 | 11.3 | 12.3 | 13.2 | 13.1 | 14.9 | 15.5 | 15.6 | 16.0 | 16.9 | 18.2 | 17.2 | 19.9 | 20.6 | 19.1 | 19.7 | 22.0 150 | 2.6 | 5.2 | 6.9 | 7.9 | 8.8 | 9.9 | 11.4 | 12.8 | 13.6 | 15.2 | 16.3 | 15.8 | 16.5 | 16.1 | 17.7 | 18.2 | 18.8 | 20.2 | 18.9 | 20.4 | 22.1 | 22.4 | 19.8 125 | 3.4 | 5.7 | 7.2 | 8.6 | 10.5 | 11.2 | 12.4 | 14.7 | 15.9 | 17.5 | 17.6 | 18.0 | 18.4 | 19.5 | 19.7 | 21.2 | 20.6 | 22.0 | 21.2 | 22.2 | 24.0 | 24.1 | 24.4 100 | 3.8 | 6.5 | 8.9 | 10.6 | 11.7 | 12.7 | 14.5 | 15.8 | 17.1 | 18.5 | 19.0 | 20.3 | 20.2 | 21.1 | 21.9 | 22.1 | 22.6 | 22.7 | 25.0 | 25.3 | 25.3 | 26.5 | 26.7 75 | 4.2 | 7.0 | 9.0 | 10.5 | 12.3 | 13.7 | 14.9 | 16.2 | 16.8 | 18.3 | 19.7 | 19.3 | 18.9 | 20.7 | 20.8 | 22.0 | 22.9 | 21.7 | 23.3 | 25.0 | 24.1 | 21.6 | 24.8 50 | 3.7 | 5.9 | 7.4 | 8.6 | 9.9 | 11.2 | 12.4 | 13.7 | 14.1 | 15.4 | 14.7 | 15.5 | 16.3 | 16.8 | 18.0 | 17.0 | 17.8 | 17.8 | 18.8 | 19.0 | 18.9 | 19.2 | 0 | | | 2.9 | 3.4 | 3.8 | 4.5 | 5.1 | 5.4 | 5.8 | 6.1 | 6.6 | 6.6 | 7.0 | 6.8 | 7.0 | 7.7 | 8.1 | 7.7 | | | | | The percent uncertainty of the \partial\sigma(E_{\nu})/\partial(KE_{\pi}) results from Figure 28 is shown. Each bin is labeled according to its low edge. The columns are bins of neutrino energy (MeV) and the rows are bins of pion kinetic energy (MeV). Empty bins indicate regions where no measurement has been made. Bin | 500 | 600 | 650 | 700 | 750 | 800 | 850 | 900 | 950 | 1000 | 1050 | 1100 | 1150 | 1200 | 1250 | 1300 | 1350 | 1400 | 1450 | 1500 | 1550 | 1600 | 1650 375 | | | | | | 22.5 | 20.1 | 20.9 | 19.5 | 20.8 | 20.5 | 20.8 | 20.8 | 20.6 | 21.2 | 20.3 | 23.3 | 23.2 | 24.2 | | | | 350 | | | | | 23.2 | 20.2 | 18.9 | 19.3 | 18.2 | 19.0 | 20.3 | 19.3 | 20.7 | 19.9 | 19.2 | 21.1 | 23.3 | 23.0 | 26.8 | 25.8 | | | 325 | | | | 20.6 | 19.4 | 18.8 | 19.3 | 18.8 | 18.2 | 18.4 | 17.2 | 18.6 | 19.3 | 19.9 | 20.1 | 20.2 | 22.3 | 21.3 | 22.5 | 24.3 | 23.5 | | 300 | | | 22.6 | 19.0 | 17.0 | 18.2 | 17.9 | 17.6 | 16.6 | 16.8 | 17.7 | 17.6 | 19.7 | 20.0 | 19.0 | 19.9 | 20.3 | 21.9 | 27.2 | 21.9 | 22.8 | 23.2 | 275 | | 23.0 | 19.9 | 17.6 | 17.3 | 17.3 | 16.4 | 17.2 | 16.0 | 17.0 | 17.1 | 17.5 | 18.4 | 18.4 | 17.9 | 18.9 | 19.9 | 19.7 | 19.6 | 24.3 | 21.6 | 23.0 | 25.5 250 | | 19.8 | 18.1 | 17.1 | 15.6 | 15.5 | 15.1 | 16.2 | 16.0 | 16.0 | 16.2 | 15.8 | 17.5 | 16.7 | 17.9 | 18.2 | 18.7 | 18.7 | 21.7 | 21.3 | 24.6 | 22.7 | 26.3 225 | 19.4 | 17.3 | 16.7 | 16.0 | 15.3 | 15.1 | 15.0 | 14.7 | 14.9 | 14.6 | 14.3 | 14.4 | 16.7 | 15.9 | 18.4 | 16.7 | 17.2 | 19.4 | 22.8 | 24.8 | 19.4 | 22.5 | 24.9 200 | 17.0 | 16.3 | 15.6 | 15.3 | 13.7 | 14.1 | 14.1 | 13.5 | 13.7 | 13.0 | 13.5 | 13.4 | 15.7 | 15.2 | 15.9 | 16.2 | 18.5 | 18.4 | 18.8 | 20.0 | 21.2 | 21.9 | 23.4 175 | 16.6 | 17.3 | 15.9 | 14.1 | 12.9 | 12.8 | 12.5 | 12.2 | 12.2 | 12.7 | 13.3 | 13.5 | 13.9 | 13.8 | 14.8 | 16.8 | 16.2 | 17.4 | 18.6 | 19.4 | 19.9 | 22.5 | 24.4 150 | 15.6 | 14.9 | 13.5 | 12.8 | 12.5 | 12.1 | 11.5 | 11.6 | 11.9 | 11.3 | 12.5 | 12.4 | 13.3 | 14.9 | 14.7 | 14.8 | 16.2 | 18.1 | 19.5 | 20.2 | 20.6 | 22.6 | 21.3 125 | 16.5 | 14.6 | 11.6 | 10.8 | 11.5 | 11.1 | 10.5 | 10.5 | 10.2 | 10.5 | 11.4 | 12.1 | 13.1 | 13.0 | 14.2 | 14.7 | 16.1 | 17.3 | 17.7 | 17.4 | 19.9 | 20.0 | 24.4 100 | 14.4 | 11.9 | 10.9 | 9.8 | 10.0 | 10.1 | 9.2 | 9.8 | 9.7 | 11.5 | 10.8 | 11.1 | 11.9 | 12.9 | 13.2 | 14.3 | 15.4 | 15.7 | 17.2 | 17.4 | 18.3 | 20.1 | 21.2 75 | 12.0 | 12.8 | 10.4 | 11.3 | 11.6 | 13.0 | 12.0 | 12.8 | 12.7 | 12.7 | 14.0 | 13.7 | 13.2 | 13.8 | 14.4 | 14.2 | 15.3 | 16.6 | 15.9 | 18.7 | 18.6 | 18.8 | 21.5 50 | 14.5 | 13.9 | 11.9 | 13.9 | 14.3 | 13.9 | 15.4 | 14.3 | 13.3 | 14.1 | 14.4 | 14.7 | 16.7 | 14.5 | 13.9 | 15.0 | 17.1 | 16.6 | 15.9 | 18.0 | 18.5 | 18.3 | 0 | | | 15.3 | 16.0 | 15.9 | 15.9 | 16.1 | 16.5 | 12.9 | 14.0 | 14.3 | 14.0 | 14.9 | 13.6 | 13.8 | 14.7 | 14.2 | 15.5 | | | | | The \partial^2\sigma/\partial(KE_{\mu})\partial(\cos(\theta_{\mu,\nu})) results from Figure 24 are shown (10^{-42}cm^2/MeV). Each bin is labeled according to its low edge. The columns are bins of muon kinetic energy (MeV) and the rows are bins of cos(muon, neutrino angle). Empty bins indicate regions where no measurement has been made. Bin | 150 | 200 | 250 | 300 | 350 | 400 | 450 | 500 | 550 | 600 | 650 | 700 | 750 | 800 | 850 | 900 | 950 | 1000 | 1100 | 1200 0.95 | 23.0 | 26.1 | 32.1 | 38.5 | 42.8 | 47.9 | 55.8 | 58.2 | 59.8 | 63.7 | 65.8 | 69.3 | 71.5 | 65.9 | 58.5 | 59.3 | 56.0 | 48.4 | 43.3 | 27.7 0.90 | 30.5 | 35.8 | 41.3 | 46.7 | 55.0 | 59.5 | 64.3 | 70.8 | 70.3 | 72.6 | 73.3 | 65.0 | 65.7 | 59.4 | 58.0 | 50.8 | 46.4 | 38.3 | 28.1 | 12.6 0.85 | 31.7 | 37.0 | 44.8 | 50.9 | 58.7 | 70.2 | 67.6 | 67.5 | 70.4 | 71.4 | 69.5 | 56.0 | 52.7 | 49.3 | 42.3 | 36.1 | 27.3 | 19.8 | 12.9 | 5.7 0.80 | 31.7 | 39.1 | 43.4 | 53.8 | 63.6 | 62.5 | 64.7 | 67.3 | 61.7 | 57.2 | 55.3 | 45.4 | 37.1 | 33.6 | 25.1 | 19.9 | 15.5 | 9.0 | | 0.75 | 33.7 | 40.0 | 45.5 | 53.3 | 57.3 | 58.6 | 58.5 | 60.4 | 53.0 | 44.9 | 37.0 | 33.1 | 25.8 | 18.7 | 13.7 | | | | | 0.70 | 37.8 | 40.5 | 48.6 | 58.5 | 57.3 | 58.2 | 53.8 | 52.4 | 42.4 | 35.5 | 28.8 | 22.0 | 15.4 | 12.3 | | | | | | 0.65 | 35.9 | 41.7 | 46.8 | 50.6 | 56.1 | 49.2 | 44.8 | 38.4 | 29.6 | 23.5 | 16.9 | 14.1 | 10.0 | | | | | | | 0.60 | 33.5 | 43.3 | 47.0 | 47.1 | 51.6 | 51.1 | 40.6 | 31.0 | 25.0 | 16.7 | 11.5 | 8.5 | | | | | | | | 0.55 | 35.0 | 41.7 | 46.1 | 49.4 | 42.3 | 37.3 | 33.2 | 24.1 | 17.1 | 11.1 | | | | | | | | | | 0.50 | 32.8 | 38.3 | 44.2 | 44.2 | 39.5 | 33.6 | 26.1 | 15.9 | 11.8 | | | | | | | | | | | 0.45 | 32.8 | 37.8 | 39.0 | 39.1 | 32.8 | 25.8 | 17.9 | 13.3 | 8.8 | | | | | | | | | | | 0.40 | 32.5 | 38.1 | 42.3 | 37.7 | 28.9 | 22.4 | 14.9 | 9.2 | | | | | | | | | | | | 0.35 | 36.9 | 40.5 | 36.9 | 31.6 | 27.1 | 17.0 | 12.1 | | | | | | | | | | | | | 0.30 | 31.1 | 34.7 | 29.9 | 28.8 | 20.9 | 12.3 | | | | | | | | | | | | | | 0.25 | 30.2 | 31.8 | 30.2 | 22.9 | 17.9 | 11.2 | | | | | | | | | | | | | | 0.20 | 27.2 | 31.6 | 27.1 | 22.3 | 14.2 | 10.6 | | | | | | | | | | | | | | 0.15 | 26.2 | 26.8 | 23.1 | 18.4 | 9.4 | | | | | | | | | | | | | | | 0.10 | 25.3 | 25.3 | 21.3 | 15.6 | | | | | | | | | | | | | | | | 0.05 | 24.7 | 25.4 | 20.6 | 13.3 | | | | | | | | | | | | | | | | 0.00 | 24.5 | 23.1 | 17.6 | 10.3 | | | | | | | | | | | | | | | | -0.05 | 24.6 | 18.6 | 13.1 | | | | | | | | | | | | | | | | | -0.10 | 21.3 | 17.9 | 12.4 | | | | | | | | | | | | | | | | | -0.20 | 21.0 | 16.7 | 10.2 | 5.4 | | | | | | | | | | | | | | | | -0.30 | 17.5 | 12.3 | 5.7 | | | | | | | | | | | | | | | | | -0.40 | 14.7 | 10.2 | 6.0 | | | | | | | | | | | | | | | | | -0.50 | 13.1 | 8.3 | | | | | | | | | | | | | | | | | | -0.60 | 11.6 | 5.7 | | | | | | | | | | | | | | | | | | -0.80 | 8.5 | 3.0 | | | | | | | | | | | | | | | | | | -1.00 | 3.9 | | | | | | | | | | | | | | | | | | | The percent uncertainty of the \partial^2\sigma/\partial(KE_{\mu})\partial(\cos(\theta_{\mu,\nu})) results from Figure 24 is shown. Each bin is labeled according to its low edge. The columns are bins of muon kinetic energy (MeV) and the rows are bins of cos(muon, neutrino angle). Empty bins indicate regions where no measurement has been made. Bin | 150 | 200 | 250 | 300 | 350 | 400 | 450 | 500 | 550 | 600 | 650 | 700 | 750 | 800 | 850 | 900 | 950 | 1000 | 1100 | 1200 0.95 | 27.0 | 25.9 | 20.7 | 19.0 | 17.5 | 17.1 | 14.7 | 16.2 | 16.3 | 14.5 | 15.0 | 13.9 | 13.9 | 15.2 | 16.3 | 15.9 | 15.8 | 15.8 | 15.6 | 19.7 0.90 | 18.9 | 18.1 | 17.6 | 16.7 | 16.0 | 14.6 | 13.9 | 15.0 | 14.3 | 14.5 | 14.3 | 15.4 | 14.6 | 13.8 | 14.4 | 14.0 | 16.8 | 16.8 | 20.6 | 25.0 0.85 | 20.3 | 16.9 | 16.0 | 17.0 | 16.4 | 16.0 | 13.8 | 14.7 | 13.6 | 14.8 | 14.5 | 13.8 | 14.3 | 15.4 | 17.6 | 18.1 | 19.4 | 20.3 | 24.6 | 36.6 0.80 | 18.5 | 16.6 | 16.7 | 15.1 | 15.8 | 15.9 | 14.2 | 14.5 | 13.2 | 14.0 | 14.3 | 14.7 | 15.1 | 15.7 | 18.2 | 22.4 | 27.1 | 33.1 | | 0.75 | 17.0 | 16.3 | 15.9 | 14.9 | 14.0 | 14.5 | 14.5 | 14.1 | 14.2 | 15.6 | 16.4 | 15.9 | 16.5 | 17.3 | 21.8 | | | | | 0.70 | 15.9 | 15.6 | 15.6 | 15.8 | 16.5 | 15.9 | 14.7 | 15.0 | 14.8 | 15.0 | 15.7 | 20.2 | 20.5 | 21.0 | | | | | | 0.65 | 16.4 | 15.4 | 14.5 | 15.7 | 15.4 | 14.8 | 15.4 | 15.0 | 16.2 | 16.5 | 16.1 | 20.1 | 26.5 | | | | | | | 0.60 | 15.9 | 15.1 | 15.3 | 16.1 | 16.0 | 16.2 | 15.1 | 15.4 | 16.1 | 20.7 | 21.0 | 23.9 | | | | | | | | 0.55 | 16.4 | 16.8 | 16.4 | 15.1 | 14.7 | 15.1 | 17.2 | 18.9 | 17.8 | 21.8 | | | | | | | | | | 0.50 | 16.4 | 17.4 | 15.1 | 17.1 | 16.4 | 17.1 | 16.8 | 19.1 | 25.5 | | | | | | | | | | | 0.45 | 15.5 | 17.8 | 17.0 | 16.3 | 15.6 | 17.8 | 19.0 | 17.6 | 26.0 | | | | | | | | | | | 0.40 | 16.4 | 16.8 | 17.1 | 17.0 | 16.0 | 17.2 | 18.7 | 26.3 | | | | | | | | | | | | 0.35 | 19.1 | 20.3 | 17.7 | 16.2 | 17.3 | 22.5 | 25.2 | | | | | | | | | | | | | 0.30 | 18.1 | 20.6 | 17.2 | 15.5 | 18.1 | 20.8 | | | | | | | | | | | | | | 0.25 | 17.1 | 16.9 | 16.2 | 16.8 | 18.5 | 24.5 | | | | | | | | | | | | | | 0.20 | 17.1 | 17.8 | 18.0 | 20.2 | 19.2 | 35.3 | | | | | | | | | | | | | | 0.15 | 17.9 | 16.6 | 16.9 | 21.1 | 22.2 | | | | | | | | | | | | | | | 0.10 | 16.4 | 17.1 | 17.7 | 21.1 | | | | | | | | | | | | | | | | 0.05 | 18.7 | 18.5 | 21.0 | 24.0 | | | | | | | | | | | | | | | | 0.00 | 18.4 | 21.1 | 22.5 | 27.8 | | | | | | | | | | | | | | | | -0.05 | 20.1 | 20.0 | 20.8 | | | | | | | | | | | | | | | | | -0.10 | 21.8 | 17.7 | 25.6 | | | | | | | | | | | | | | | | | -0.20 | 19.1 | 18.9 | 26.1 | 36.8 | | | | | | | | | | | | | | | | -0.30 | 17.7 | 21.6 | 28.3 | | | | | | | | | | | | | | | | | -0.40 | 18.7 | 20.4 | 35.2 | | | | | | | | | | | | | | | | | -0.50 | 21.7 | 27.5 | | | | | | | | | | | | | | | | | | -0.60 | 24.0 | 32.9 | | | | | | | | | | | | | | | | | | -0.80 | 24.2 | 29.5 | | | | | | | | | | | | | | | | | | -1.00 | 25.4 | | | | | | | | | | | | | | | | | | | The \partial^2\sigma/\partial(KE_{\pi})\partial(\cos(\theta_{\pi,\nu})) results from Figure 25 are shown (10^{-41}cm^2/MeV). Each bin is labeled according to its low edge. The columns are bins of pion kinetic energy (MeV) and the rows are bins of cos(pion, neutrino angle). Empty bins indicate regions where no measurement has been made. Bin | 150 | 175 | 200 | 225 | 250 | 275 | 300 | 325 | 350 | 375 0.95 | 7.9 | 8.9 | 10.3 | 10.7 | 10.0 | 10.3 | 9.4 | 8.0 | 6.8 | 6.0 0.90 | 8.5 | 9.6 | 10.1 | 9.9 | 9.9 | 9.1 | 8.8 | 7.5 | 6.3 | 5.4 0.85 | 9.7 | 10.0 | 10.8 | 10.0 | 9.2 | 8.5 | 7.5 | 6.7 | 5.5 | 4.7 0.80 | 9.2 | 9.8 | 9.6 | 9.2 | 8.4 | 7.5 | 6.9 | 5.9 | 5.3 | 4.4 0.75 | 9.6 | 9.0 | 9.1 | 8.6 | 7.8 | 7.2 | 6.3 | 5.3 | 4.2 | 4.1 0.70 | 9.2 | 9.7 | 8.9 | 8.2 | 7.4 | 6.3 | 5.4 | 4.3 | 3.9 | 3.4 0.65 | 9.4 | 8.7 | 8.2 | 7.6 | 6.5 | 5.8 | 4.9 | 4.1 | 3.2 | 2.9 0.60 | 9.3 | 8.4 | 8.4 | 7.0 | 5.9 | 5.0 | 3.9 | 3.4 | 3.0 | 2.5 0.55 | 9.0 | 7.7 | 7.2 | 6.1 | 5.5 | 4.6 | 3.5 | 3.1 | 2.4 | 2.2 0.50 | 8.4 | 7.5 | 6.4 | 5.6 | 5.0 | 3.8 | 3.2 | 2.6 | 2.1 | 0.45 | 7.5 | 6.7 | 5.8 | 4.9 | 4.2 | 3.3 | 2.7 | | | 0.40 | 7.5 | 6.2 | 5.4 | 4.4 | 3.5 | 2.6 | 2.2 | | | 0.35 | 7.0 | 5.8 | 4.9 | 3.6 | 3.1 | 2.5 | | | | 0.30 | 6.8 | 5.5 | 4.3 | 3.3 | 2.5 | | | | | 0.25 | 6.1 | 5.1 | 3.6 | 2.6 | 2.3 | | | | | 0.20 | 5.7 | 4.2 | 3.4 | 2.7 | | | | | | 0.15 | 5.1 | 3.7 | 2.8 | 1.9 | | | | | | 0.10 | 4.5 | 3.5 | 2.3 | 1.7 | | | | | | 0.05 | 4.3 | 2.9 | 2.4 | | | | | | | 0.00 | 3.7 | 2.4 | 2.0 | | | | | | | -0.05 | 3.1 | 2.1 | | | | | | | | -0.10 | 2.8 | 1.8 | | | | | | | | -0.15 | 2.3 | | | | | | | | | -0.20 | 2.1 | | | | | | | | | -0.25 | 2.0 | | | | | | | | | The percent uncertainty of the \partial^2\sigma/\partial(KE_{\pi})\partial(\cos(\theta_{\pi,\nu})) results from Figure 25 is shown. Each bin is labeled according to its low edge. The columns are bins of pion kinetic energy (MeV) and the rows are bins of cos(pion, neutrino angle). Empty bins indicate regions where no measurement has been made. Bin | 150 | 175 | 200 | 225 | 250 | 275 | 300 | 325 | 350 | 375 0.95 | 16.5 | 16.7 | 17.3 | 17.8 | 19.7 | 20.8 | 21.3 | 22.6 | 22.1 | 22.8 0.90 | 14.4 | 16.1 | 15.9 | 17.4 | 18.1 | 19.2 | 19.8 | 20.1 | 22.0 | 21.4 0.85 | 12.8 | 13.5 | 14.8 | 16.0 | 17.4 | 18.1 | 19.0 | 18.3 | 19.1 | 20.0 0.80 | 13.8 | 14.3 | 14.8 | 15.6 | 17.5 | 19.8 | 19.2 | 19.5 | 20.1 | 19.8 0.75 | 13.5 | 15.3 | 15.9 | 15.8 | 17.3 | 17.7 | 19.6 | 18.7 | 21.5 | 20.3 0.70 | 14.3 | 16.0 | 15.3 | 17.1 | 17.6 | 17.8 | 19.9 | 18.0 | 19.0 | 19.8 0.65 | 14.0 | 16.0 | 15.5 | 16.8 | 16.8 | 17.7 | 17.1 | 22.4 | 19.2 | 21.8 0.60 | 14.0 | 16.9 | 16.4 | 17.6 | 19.6 | 19.7 | 22.2 | 20.3 | 21.7 | 23.3 0.55 | 15.7 | 17.4 | 20.4 | 19.4 | 18.6 | 19.7 | 19.8 | 21.2 | 32.3 | 21.1 0.50 | 16.2 | 17.9 | 18.8 | 18.1 | 19.2 | 19.0 | 22.6 | 23.5 | 20.0 | 0.45 | 17.0 | 18.2 | 19.3 | 19.4 | 19.4 | 23.1 | 23.0 | | | 0.40 | 17.1 | 16.7 | 19.5 | 23.2 | 22.5 | 20.8 | 25.2 | | | 0.35 | 16.8 | 16.3 | 18.4 | 21.7 | 21.9 | 23.8 | | | | 0.30 | 17.8 | 19.0 | 19.7 | 20.8 | 22.2 | | | | | 0.25 | 16.9 | 18.7 | 21.3 | 22.9 | 22.0 | | | | | 0.20 | 18.3 | 18.8 | 21.9 | 20.8 | | | | | | 0.15 | 18.5 | 19.7 | 18.5 | 20.9 | | | | | | 0.10 | 17.3 | 16.6 | 17.8 | 20.5 | | | | | | 0.05 | 17.1 | 16.4 | 17.5 | | | | | | | 0.00 | 17.4 | 20.4 | 18.4 | | | | | | | -0.05 | 16.8 | 17.6 | | | | | | | | -0.10 | 18.4 | 20.1 | | | | | | | | -0.15 | 21.5 | | | | | | | | | -0.20 | 18.9 | | | | | | | | | -0.25 | 20.4 | | | | | | | | |