Showing 10 of 73 results
We present results from a high momentum resolution measurement of the π − p elastic differential cross section near the η production threshold. By analysing the cusp discontinuity in the elastic cross section we deduce the non-spin-flip elastic amplitude and compare it with solutions from phase-shift analyses.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
None
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
Cross sections for pi+-p elastic scattering have been measured to high precision, for beam momenta between 800 and 1240 MeV/c, by the EPECUR Collaboration, using the ITEP proton synchrotron. The data precision allows comparisons of the existing partial-wave analyses (PWA) on a level not possible previously. These comparisons imply that updated PWA are required.
Differential cross section of elastic $\pi^+$p-scattering at P= 800.25 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 803.75 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 807.25 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 810.75 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 814.54 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 818.13 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 822.17 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 825.83 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 829.92 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 833.58 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 837.67 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 841.33 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 845.17 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 848.83 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 852.67 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 856.33 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 859.96 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 863.71 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 867.58 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 871.42 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 874.88 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 878.79 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 882.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 886.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 890.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 894.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 897.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 901.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 905.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 909.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 912.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 916.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 919.04 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 923.38 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 927.33 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 931.92 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 936.25 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 940.58 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 948.08 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 952.75 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 957.42 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 963.33 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 968.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 972.67 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 978.33 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 983.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 987.67 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 993.58 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P= 998.25 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1002.92 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1008.58 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1013.25 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1017.92 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1023.58 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1028.25 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1032.92 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1038.58 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1043.25 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1047.92 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1053.58 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1058.25 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1062.92 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1068.58 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1073.25 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1077.92 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1083.33 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1088.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1092.67 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1097.83 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1102.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1107.17 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1111.83 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1116.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1121.17 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1125.83 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1130.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1135.17 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1139.83 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1144.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1149.17 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1154.83 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1159.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1164.17 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1170.83 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1175.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1180.17 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1186.33 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1191.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1195.67 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1201.33 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1206.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1210.67 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1216.33 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1221.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1225.67 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1231.17 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1236.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1240.83 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1247.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1252.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1257.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1262.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1267.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1272.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1276.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1281.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1286.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1291.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1296.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1301.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1306.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1311.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1316.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1320.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1325.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^+$p-scattering at P=1330.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 800.25 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 803.75 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 807.25 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 810.75 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 814.54 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 818.13 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 822.17 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 825.83 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 829.92 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 833.58 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 837.67 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 841.33 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 845.17 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 848.83 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 852.67 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 856.33 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 859.96 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 863.71 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 867.58 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 871.42 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 874.88 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 878.79 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 882.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 886.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 890.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 894.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 897.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 901.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 905.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 909.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 912.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 916.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 919.75 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 923.75 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 927.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 931.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 934.75 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 938.17 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 940.75 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 943.21 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 946.79 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 950.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 953.44 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 956.75 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 960.58 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 964.17 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 968.08 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 971.67 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 975.58 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 979.29 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 983.19 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 986.85 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 990.63 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 993.92 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P= 998.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1001.54 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1005.71 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1008.25 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1010.92 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1014.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1017.79 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1022.13 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1026.21 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1029.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1032.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1035.96 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1039.54 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1043.77 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1047.48 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1052.33 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1056.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1060.42 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1063.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1066.58 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1070.42 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1074.35 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1078.23 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1082.29 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1086.21 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1090.04 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1093.96 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1098.04 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1102.29 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1104.92 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1108.21 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1112.58 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1116.92 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1120.83 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1124.08 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1127.77 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1132.23 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1134.75 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1137.44 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1140.33 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1143.60 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1147.81 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1152.02 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1157.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1162.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1167.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1172.29 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1177.38 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1182.46 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1187.33 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1192.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1197.67 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1202.58 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1207.75 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1212.92 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1217.02 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1222.31 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1227.60 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1232.38 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1237.63 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1242.88 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1247.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1252.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1257.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1262.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1267.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1272.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1276.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1281.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1286.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1291.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1296.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1301.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1306.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1311.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1316.00 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1320.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1325.50 MeV/c. Errors shown are statistical only.
Differential cross section of elastic $\pi^-$p-scattering at P=1330.50 MeV/c. Errors shown are statistical only.
Differential cross sections have been measured for π − p elastic scattering at laboratory momenta in the range 1.2 to 3.0 GeV/ c for the c.m. range 0.97 > cos θ ∗ > −0.98 . The corresponding mass range is 1.78 to 2.56 GeV/ c 2 . The data was obtained from a counter experiment in which the scattered pions and protons were detected in coincidence by arrays of scintillation counters.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
RENORMALIZED TO ESTERL66. RELATIVE NORM STABLE TO 1PC IN 5 FITS.
No description provided.
No description provided.
No description provided.
RENORMALIZED TO FELLIN70. ORIGINALLY NORMALIZED TO FORWARD.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
pp-elastic differential cross sections are reported at 492 MeV from 40° to 90°, and at 576, 642, 728, and 793 MeV from 75° to 90° c.m., with an absolute accuracy of less than 1%. These data, obtained with polyethylene targets, agree with recent measurements at the same energies obtained with a liquid-hydrogen target. © 1996 The American Physical Society.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
Absolute pp-elastic-differential cross sections were measured at incident energies 492, 576, 642, 728, and 793 MeV from about 30° to 90° c.m. The total uncertainty was determined to be less than 1%, made possible by particle counting for beam normalization and extensive cross-checks of systematic effects. These new data are consistent with previous data above 600 MeV but have uncertainties about a factor of 10 smaller. Near 500 MeV these data are consistent with 90° data from TRIUMF, but differ significantly from similar data from PSI; the cause of this discrepancy is discussed.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
An experimental study of the elastic scattering of negative pions off protons at 2.0 GeV/ c is presented. The differential cross section is fitted to a polynomial in cos θ c.m. and the forward angular region as a diffraction peak. The results are compared with those from other bubble chamber experiments at neighbouring energies and discussed in terms of optical model and possible exchange trajectories.
No description provided.
We have measured the differential cross section of the reaction π − p→ π − p in the range 0.92 ⩽ cos θ c.m. ⩽ 0.99 at 15 momenta between 0.875 and 1.580 GeV/ c . The results we report complete the available data; previous measurements of this reaction do not extend beyond cos θ c.m. =0.90. We compare our experimental results with dispersion relation predictions. A comparison of our results for B , the slope of the differential cross section, with earlier results shows many discrepancies.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
In this paper we present the π + p differential elastic scattering cross sections at five momenta between 0.6 and 0.8 GeV/ c . The data were collected in a bubble chamber exposure and consequently are susceptible to different systematic errors from counter experiments. Our results are generally in good agreement with those of counter experiments in the same momentum range and with the predictions of the various elastic partial wave analyses. The majority of partial wave analyses do not however yield parameters which fit our data in detail without modification.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
Differential cross sections for π + p and π − p elastic scattering have been measured with an accuracy of typically ±2% at 10 and 9 energies respectively in the range 88 to 292 MeV of lab kinetic energy.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
When you search on a word, e.g. 'collisions', we will automatically search across everything we store about a record. But, sometimes you may wish to be more specific. Here we show you how.
Guidance and examples on the query string syntax can be found in the Elasticsearch documentation.
About HEPData Submitting to HEPData HEPData File Formats HEPData Coordinators HEPData Terms of Use HEPData Cookie Policy
Status Email Forum Twitter GitHub
Copyright ~1975-Present, HEPData | Powered by Invenio, funded by STFC, hosted and originally developed at CERN, supported and further developed at IPPP Durham.