CLAS12 Run Group A
- Spokesperson
- Krishna Chandra
- Year
- 2018
- 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 |
|---|---|---|---|---|---|---|---|---|
| E216M327 | dσ/dM(π+,p) | e | p | π+π−p | 3.0 | 3.5 | 1.8 | 1.85 |
| E216M328 | dσ/dψ(π−) | e | p | π+π−p | 3.0 | 3.5 | 1.8 | 1.85 |
| E216M329 | dσ/dψ(π+) | e | p | π+π−p | 3.0 | 3.5 | 1.8 | 1.85 |
| E216M330 | dσ/dψ(p) | e | p | π+π−p | 3.0 | 3.5 | 1.8 | 1.85 |
| E216M331 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.0 | 3.5 | 1.8 | 1.85 |
| E216M332 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.0 | 3.5 | 1.8 | 1.85 |
| E216M333 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.0 | 3.5 | 1.8 | 1.85 |
| E216M334 | dσ/dM(π−,p) | e | p | π+π−p | 3.0 | 3.5 | 1.85 | 1.9 |
| E216M335 | dσ/dM(π+,π−) | e | p | π+π−p | 3.0 | 3.5 | 1.85 | 1.9 |
| E216M336 | dσ/dM(π+,p) | e | p | π+π−p | 3.0 | 3.5 | 1.85 | 1.9 |
| E216M337 | dσ/dψ(π−) | e | p | π+π−p | 3.0 | 3.5 | 1.85 | 1.9 |
| E216M338 | dσ/dψ(π+) | e | p | π+π−p | 3.0 | 3.5 | 1.85 | 1.9 |
| E216M339 | dσ/dψ(p) | e | p | π+π−p | 3.0 | 3.5 | 1.85 | 1.9 |
| E216M340 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.0 | 3.5 | 1.85 | 1.9 |
| E216M341 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.0 | 3.5 | 1.85 | 1.9 |
| E216M342 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.0 | 3.5 | 1.85 | 1.9 |
| E216M343 | dσ/dM(π−,p) | e | p | π+π−p | 3.0 | 3.5 | 1.9 | 1.95 |
| E216M344 | dσ/dM(π+,π−) | e | p | π+π−p | 3.0 | 3.5 | 1.9 | 1.95 |
| E216M345 | dσ/dM(π+,p) | e | p | π+π−p | 3.0 | 3.5 | 1.9 | 1.95 |
| E216M346 | dσ/dψ(π−) | e | p | π+π−p | 3.0 | 3.5 | 1.9 | 1.95 |
| E216M347 | dσ/dψ(π+) | e | p | π+π−p | 3.0 | 3.5 | 1.9 | 1.95 |
| E216M348 | dσ/dψ(p) | e | p | π+π−p | 3.0 | 3.5 | 1.9 | 1.95 |
| E216M349 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.0 | 3.5 | 1.9 | 1.95 |
| E216M350 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.0 | 3.5 | 1.9 | 1.95 |
| E216M351 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.0 | 3.5 | 1.9 | 1.95 |
| E216M352 | dσ/dM(π−,p) | e | p | π+π−p | 3.0 | 3.5 | 1.95 | 2.0 |
| E216M353 | dσ/dM(π+,π−) | e | p | π+π−p | 3.0 | 3.5 | 1.95 | 2.0 |
| E216M354 | dσ/dM(π+,p) | e | p | π+π−p | 3.0 | 3.5 | 1.95 | 2.0 |
| E216M355 | dσ/dψ(π−) | e | p | π+π−p | 3.0 | 3.5 | 1.95 | 2.0 |
| E216M356 | dσ/dψ(π+) | e | p | π+π−p | 3.0 | 3.5 | 1.95 | 2.0 |
| E216M357 | dσ/dψ(p) | e | p | π+π−p | 3.0 | 3.5 | 1.95 | 2.0 |
| E216M358 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.0 | 3.5 | 1.95 | 2.0 |
| E216M359 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.0 | 3.5 | 1.95 | 2.0 |
| E216M360 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.0 | 3.5 | 1.95 | 2.0 |
| E216M361 | dσ/dM(π−,p) | e | p | π+π−p | 3.0 | 3.5 | 2.0 | 2.05 |
| E216M362 | dσ/dM(π+,π−) | e | p | π+π−p | 3.0 | 3.5 | 2.0 | 2.05 |
| E216M363 | dσ/dM(π+,p) | e | p | π+π−p | 3.0 | 3.5 | 2.0 | 2.05 |
| E216M364 | dσ/dψ(π−) | e | p | π+π−p | 3.0 | 3.5 | 2.0 | 2.05 |
| E216M365 | dσ/dψ(π+) | e | p | π+π−p | 3.0 | 3.5 | 2.0 | 2.05 |
| E216M366 | dσ/dψ(p) | e | p | π+π−p | 3.0 | 3.5 | 2.0 | 2.05 |
| E216M367 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.0 | 3.5 | 2.0 | 2.05 |
| E216M368 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.0 | 3.5 | 2.0 | 2.05 |
| E216M369 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.0 | 3.5 | 2.0 | 2.05 |
| E216M370 | dσ/dM(π−,p) | e | p | π+π−p | 3.0 | 3.5 | 2.05 | 2.1 |
| E216M371 | dσ/dM(π+,π−) | e | p | π+π−p | 3.0 | 3.5 | 2.05 | 2.1 |
| E216M372 | dσ/dM(π+,p) | e | p | π+π−p | 3.0 | 3.5 | 2.05 | 2.1 |
| E216M373 | dσ/dψ(π−) | e | p | π+π−p | 3.0 | 3.5 | 2.05 | 2.1 |
| E216M374 | dσ/dψ(π+) | e | p | π+π−p | 3.0 | 3.5 | 2.05 | 2.1 |
| E216M375 | dσ/dψ(p) | e | p | π+π−p | 3.0 | 3.5 | 2.05 | 2.1 |
| E216M376 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.0 | 3.5 | 2.05 | 2.1 |
| E216M377 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.0 | 3.5 | 2.05 | 2.1 |
| E216M378 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.0 | 3.5 | 2.05 | 2.1 |
| E216M379 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.4 | 1.45 |
| E216M380 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.4 | 1.45 |
| E216M381 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.4 | 1.45 |
| E216M382 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.4 | 1.45 |
| E216M383 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.4 | 1.45 |
| E216M384 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.4 | 1.45 |
| E216M385 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.4 | 1.45 |
| E216M386 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.4 | 1.45 |
| E216M387 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.4 | 1.45 |
| E216M388 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.45 | 1.5 |
| E216M389 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.45 | 1.5 |
| E216M390 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.45 | 1.5 |
| E216M391 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.45 | 1.5 |
| E216M392 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.45 | 1.5 |
| E216M393 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.45 | 1.5 |
| E216M394 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.45 | 1.5 |
| E216M395 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.45 | 1.5 |
| E216M396 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.45 | 1.5 |
| E216M397 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.5 | 1.55 |
| E216M398 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.5 | 1.55 |
| E216M399 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.5 | 1.55 |
| E216M400 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.5 | 1.55 |
| E216M401 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.5 | 1.55 |
| E216M402 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.5 | 1.55 |
| E216M403 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.5 | 1.55 |
| E216M404 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.5 | 1.55 |
| E216M405 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.5 | 1.55 |
| E216M406 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.55 | 1.6 |
| E216M407 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.55 | 1.6 |
| E216M408 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.55 | 1.6 |
| E216M409 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.55 | 1.6 |
| E216M410 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.55 | 1.6 |
| E216M411 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.55 | 1.6 |
| E216M412 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.55 | 1.6 |
| E216M413 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.55 | 1.6 |
| E216M414 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.55 | 1.6 |
| E216M415 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.6 | 1.65 |
| E216M416 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.6 | 1.65 |
| E216M417 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.6 | 1.65 |
| E216M418 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.6 | 1.65 |
| E216M419 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.6 | 1.65 |
| E216M420 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.6 | 1.65 |
| E216M421 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.6 | 1.65 |
| E216M422 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.6 | 1.65 |
| E216M423 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.6 | 1.65 |
| E216M424 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.65 | 1.7 |
| E216M425 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.65 | 1.7 |
| E216M426 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.65 | 1.7 |