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 |
|---|---|---|---|---|---|---|---|---|
| E213M1346 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.8 | 1.825 |
| E213M1347 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.8 | 1.825 |
| E213M1348 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.825 | 1.85 |
| E213M1349 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.825 | 1.85 |
| E213M1350 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.825 | 1.85 |
| E213M1351 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.825 | 1.85 |
| E213M1352 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.825 | 1.85 |
| E213M1353 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.825 | 1.85 |
| E213M1354 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.825 | 1.85 |
| E213M1355 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.825 | 1.85 |
| E213M1356 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.825 | 1.85 |
| E213M1357 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.875 |
| E213M1358 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.875 |
| E213M1359 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.875 |
| E213M1360 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.875 |
| E213M1361 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.875 |
| E213M1362 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.875 |
| E213M1363 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.875 |
| E213M1364 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.875 |
| E213M1365 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.875 |
| E213M1366 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.875 | 1.9 |
| E213M1367 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.875 | 1.9 |
| E213M1368 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.875 | 1.9 |
| E213M1369 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.875 | 1.9 |
| E213M1370 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.875 | 1.9 |
| E213M1371 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.875 | 1.9 |
| E213M1372 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.875 | 1.9 |
| E213M1373 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.875 | 1.9 |
| E213M1374 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.875 | 1.9 |
| E213M1375 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.925 |
| E213M1376 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.925 |
| E213M1377 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.925 |
| E213M1378 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.925 |
| E213M1379 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.925 |
| E213M1380 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.925 |
| E213M1381 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.925 |
| E213M1382 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.925 |
| E213M1383 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.925 |
| E213M1384 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.925 | 1.95 |
| E213M1385 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.925 | 1.95 |
| E213M1386 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.925 | 1.95 |
| E213M1387 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.925 | 1.95 |
| E213M1388 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.925 | 1.95 |
| E213M1389 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.925 | 1.95 |
| E213M1390 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.925 | 1.95 |
| E213M1391 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.925 | 1.95 |
| E213M1392 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.925 | 1.95 |
| E213M1393 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 1.975 |
| E213M1394 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 1.975 |
| E213M1395 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 1.975 |
| E213M1396 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 1.975 |
| E213M1397 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 1.975 |
| E213M1398 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 1.975 |
| E213M1399 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 1.975 |
| E213M1400 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 1.975 |
| E213M1401 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 1.975 |
| E213M1402 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.975 | 2.0 |
| E213M1403 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.975 | 2.0 |
| E213M1404 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.975 | 2.0 |
| E213M1405 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.975 | 2.0 |
| E213M1406 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.975 | 2.0 |
| E213M1407 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.975 | 2.0 |
| E213M1408 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.975 | 2.0 |
| E213M1409 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.975 | 2.0 |
| E213M1410 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.975 | 2.0 |
| E213M1411 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.025 |
| E213M1412 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.025 |
| E213M1413 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.025 |
| E213M1414 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.025 |
| E213M1415 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.025 |
| E213M1416 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.025 |
| E213M1417 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.025 |
| E213M1418 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.025 |
| E213M1419 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.025 |
| E213M1420 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 2.025 | 2.05 |
| E213M1421 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 2.025 | 2.05 |
| E213M1422 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 2.025 | 2.05 |
| E213M1423 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 2.025 | 2.05 |
| E213M1424 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 2.025 | 2.05 |
| E213M1425 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 2.025 | 2.05 |
| E213M1426 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 2.025 | 2.05 |
| E213M1427 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 2.025 | 2.05 |
| E213M1428 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 2.025 | 2.05 |
| E213M1429 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 2.05 | 2.075 |
| E213M1430 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 2.05 | 2.075 |
| E213M1431 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 2.05 | 2.075 |
| E213M1432 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 2.05 | 2.075 |
| E213M1433 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 2.05 | 2.075 |
| E213M1434 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 2.05 | 2.075 |
| E213M1435 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 2.05 | 2.075 |
| E213M1436 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 2.05 | 2.075 |
| E213M1437 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 2.05 | 2.075 |
| E213M1438 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 2.075 | 2.1 |
| E213M1439 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 2.075 | 2.1 |
| E213M1440 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 2.075 | 2.1 |
| E213M1441 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 2.075 | 2.1 |
| E213M1442 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 2.075 | 2.1 |
| E213M1443 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 2.075 | 2.1 |
| E213M1444 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 2.075 | 2.1 |
| E213M1445 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 2.075 | 2.1 |