E1-6, 2025
- Spokespersons
- R.W. Gothe, A. Trivedi
- Year
- 2001
- Comment
- Experiment year: 2001—2002
- Quantities
- σ dσ/dM(π−,p) dσ/dM(π+,p) dσ/dM(π+,π−) dσ/d(−cos(θ(π−))) dσ/d(−cos(θ(π+))) dσ/d(−cos(θ(p))) dσ/dψ(π−) dσ/dψ(π+) dσ/dψ(p)
Measurements
| ID | Quantity | Beam | Target | Final state |
Q2min, GeV2 |
Q2max, GeV2 |
Wmin, GeV |
Wmax, GeV |
|---|---|---|---|---|---|---|---|---|
| E213M1046 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.7 | 1.725 |
| E213M1047 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.7 | 1.725 |
| E213M1048 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.7 | 1.725 |
| E213M1049 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.7 | 1.725 |
| E213M1050 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.7 | 1.725 |
| E213M1051 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.725 | 1.75 |
| E213M1052 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.725 | 1.75 |
| E213M1053 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.725 | 1.75 |
| E213M1054 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.725 | 1.75 |
| E213M1055 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.725 | 1.75 |
| E213M1056 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.725 | 1.75 |
| E213M1057 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.725 | 1.75 |
| E213M1058 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.725 | 1.75 |
| E213M1059 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.725 | 1.75 |
| E213M1060 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.775 |
| E213M1061 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.775 |
| E213M1062 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.775 |
| E213M1063 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.775 |
| E213M1064 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.775 |
| E213M1065 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.775 |
| E213M1066 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.775 |
| E213M1067 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.775 |
| E213M1068 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.775 |
| E213M1069 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.775 | 1.8 |
| E213M1070 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.775 | 1.8 |
| E213M1071 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.775 | 1.8 |
| E213M1072 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.775 | 1.8 |
| E213M1073 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.775 | 1.8 |
| E213M1074 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.775 | 1.8 |
| E213M1075 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.775 | 1.8 |
| E213M1076 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.775 | 1.8 |
| E213M1077 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.775 | 1.8 |
| E213M1078 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.825 |
| E213M1079 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.825 |
| E213M1080 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.825 |
| E213M1081 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.825 |
| E213M1082 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.825 |
| E213M1083 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.825 |
| E213M1084 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.825 |
| E213M1085 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.825 |
| E213M1086 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.825 |
| E213M1087 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.825 | 1.85 |
| E213M1088 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.825 | 1.85 |
| E213M1089 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.825 | 1.85 |
| E213M1090 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.825 | 1.85 |
| E213M1091 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.825 | 1.85 |
| E213M1092 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.825 | 1.85 |
| E213M1093 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.825 | 1.85 |
| E213M1094 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.825 | 1.85 |
| E213M1095 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.825 | 1.85 |
| E213M1096 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.875 |
| E213M1097 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.875 |
| E213M1098 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.875 |
| E213M1099 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.875 |
| E213M1100 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.875 |
| E213M1101 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.875 |
| E213M1102 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.875 |
| E213M1103 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.875 |
| E213M1104 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.875 |
| E213M1105 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.875 | 1.9 |
| E213M1106 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.875 | 1.9 |
| E213M1107 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.875 | 1.9 |
| E213M1108 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.875 | 1.9 |
| E213M1109 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.875 | 1.9 |
| E213M1110 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.875 | 1.9 |
| E213M1111 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.875 | 1.9 |
| E213M1112 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.875 | 1.9 |
| E213M1113 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.875 | 1.9 |
| E213M1114 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.925 |
| E213M1115 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.925 |
| E213M1116 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.925 |
| E213M1117 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.925 |
| E213M1118 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.925 |
| E213M1119 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.925 |
| E213M1120 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.925 |
| E213M1121 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.925 |
| E213M1122 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.925 |
| E213M1123 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.925 | 1.95 |
| E213M1124 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.925 | 1.95 |
| E213M1125 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.925 | 1.95 |
| E213M1126 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.925 | 1.95 |
| E213M1127 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.925 | 1.95 |
| E213M1128 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.925 | 1.95 |
| E213M1129 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.925 | 1.95 |
| E213M1130 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.925 | 1.95 |
| E213M1131 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.925 | 1.95 |
| E213M1132 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 1.975 |
| E213M1133 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 1.975 |
| E213M1134 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 1.975 |
| E213M1135 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 1.975 |
| E213M1136 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 1.975 |
| E213M1137 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 1.975 |
| E213M1138 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 1.975 |
| E213M1139 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 1.975 |
| E213M1140 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 1.975 |
| E213M1141 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.975 | 2.0 |
| E213M1142 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.975 | 2.0 |
| E213M1143 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.975 | 2.0 |
| E213M1144 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.975 | 2.0 |
| E213M1145 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.975 | 2.0 |