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 |
|---|---|---|---|---|---|---|---|---|
| E213M1146 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.975 | 2.0 |
| E213M1147 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.975 | 2.0 |
| E213M1148 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.975 | 2.0 |
| E213M1149 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.975 | 2.0 |
| E213M1150 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.025 |
| E213M1151 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.025 |
| E213M1152 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.025 |
| E213M1153 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.025 |
| E213M1154 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.025 |
| E213M1155 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.025 |
| E213M1156 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.025 |
| E213M1157 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.025 |
| E213M1158 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.025 |
| E213M1159 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 2.025 | 2.05 |
| E213M1160 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 2.025 | 2.05 |
| E213M1161 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 2.025 | 2.05 |
| E213M1162 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 2.025 | 2.05 |
| E213M1163 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 2.025 | 2.05 |
| E213M1164 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 2.025 | 2.05 |
| E213M1165 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 2.025 | 2.05 |
| E213M1166 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 2.025 | 2.05 |
| E213M1167 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 2.025 | 2.05 |
| E213M1168 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.075 |
| E213M1169 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.075 |
| E213M1170 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.075 |
| E213M1171 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.075 |
| E213M1172 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.075 |
| E213M1173 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.075 |
| E213M1174 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.075 |
| E213M1175 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.075 |
| E213M1176 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.075 |
| E213M1177 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 2.075 | 2.1 |
| E213M1178 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 2.075 | 2.1 |
| E213M1179 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 2.075 | 2.1 |
| E213M1180 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 2.075 | 2.1 |
| E213M1181 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 2.075 | 2.1 |
| E213M1182 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 2.075 | 2.1 |
| E213M1183 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 2.075 | 2.1 |
| E213M1184 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 2.075 | 2.1 |
| E213M1185 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 2.075 | 2.1 |
| E213M1186 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 2.1 | 2.125 |
| E213M1187 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 2.1 | 2.125 |
| E213M1188 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 2.1 | 2.125 |
| E213M1189 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 2.1 | 2.125 |
| E213M1190 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 2.1 | 2.125 |
| E213M1191 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 2.1 | 2.125 |
| E213M1192 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 2.1 | 2.125 |
| E213M1193 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 2.1 | 2.125 |
| E213M1194 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 2.1 | 2.125 |
| E213M1195 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.425 |
| E213M1196 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.425 |
| E213M1197 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.425 |
| E213M1198 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.425 |
| E213M1199 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.425 |
| E213M1200 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.425 |
| E213M1201 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.425 |
| E213M1202 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.425 |
| E213M1203 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.425 |
| E213M1204 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.425 | 1.45 |
| E213M1205 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.425 | 1.45 |
| E213M1206 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.425 | 1.45 |
| E213M1207 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.425 | 1.45 |
| E213M1208 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.425 | 1.45 |
| E213M1209 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.425 | 1.45 |
| E213M1210 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.425 | 1.45 |
| E213M1211 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.425 | 1.45 |
| E213M1212 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.425 | 1.45 |
| E213M1213 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.475 |
| E213M1214 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.475 |
| E213M1215 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.475 |
| E213M1216 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.475 |
| E213M1217 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.475 |
| E213M1218 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.475 |
| E213M1219 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.475 |
| E213M1220 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.475 |
| E213M1221 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.475 |
| E213M1222 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.475 | 1.5 |
| E213M1223 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.475 | 1.5 |
| E213M1224 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.475 | 1.5 |
| E213M1225 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.475 | 1.5 |
| E213M1226 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.475 | 1.5 |
| E213M1227 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.475 | 1.5 |
| E213M1228 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.475 | 1.5 |
| E213M1229 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.475 | 1.5 |
| E213M1230 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.475 | 1.5 |
| E213M1231 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.525 |
| E213M1232 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.525 |
| E213M1233 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.525 |
| E213M1234 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.525 |
| E213M1235 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.525 |
| E213M1236 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.525 |
| E213M1237 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.525 |
| E213M1238 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.525 |
| E213M1239 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.525 |
| E213M1240 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.525 | 1.55 |
| E213M1241 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.525 | 1.55 |
| E213M1242 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.525 | 1.55 |
| E213M1243 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.525 | 1.55 |
| E213M1244 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.525 | 1.55 |
| E213M1245 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.525 | 1.55 |