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 |
|---|---|---|---|---|---|---|---|---|
| E216M427 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.65 | 1.7 |
| E216M428 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.65 | 1.7 |
| E216M429 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.65 | 1.7 |
| E216M430 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.65 | 1.7 |
| E216M431 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.65 | 1.7 |
| E216M432 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.65 | 1.7 |
| E216M433 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.7 | 1.75 |
| E216M434 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.7 | 1.75 |
| E216M435 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.7 | 1.75 |
| E216M436 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.7 | 1.75 |
| E216M437 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.7 | 1.75 |
| E216M438 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.7 | 1.75 |
| E216M439 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.7 | 1.75 |
| E216M440 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.7 | 1.75 |
| E216M441 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.7 | 1.75 |
| E216M442 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.8 |
| E216M443 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.8 |
| E216M444 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.8 |
| E216M445 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.8 |
| E216M446 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.8 |
| E216M447 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.8 |
| E216M448 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.8 |
| E216M449 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.8 |
| E216M450 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.75 | 1.8 |
| E216M451 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.85 |
| E216M452 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.85 |
| E216M453 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.85 |
| E216M454 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.85 |
| E216M455 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.85 |
| E216M456 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.85 |
| E216M457 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.85 |
| E216M458 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.85 |
| E216M459 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.8 | 1.85 |
| E216M460 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.9 |
| E216M461 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.9 |
| E216M462 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.9 |
| E216M463 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.9 |
| E216M464 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.9 |
| E216M465 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.9 |
| E216M466 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.9 |
| E216M467 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.9 |
| E216M468 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.85 | 1.9 |
| E216M469 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.95 |
| E216M470 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.95 |
| E216M471 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.95 |
| E216M472 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.95 |
| E216M473 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.95 |
| E216M474 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.95 |
| E216M475 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.95 |
| E216M476 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.95 |
| E216M477 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.9 | 1.95 |
| E216M478 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 2.0 |
| E216M479 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 2.0 |
| E216M480 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 2.0 |
| E216M481 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 2.0 |
| E216M482 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 2.0 |
| E216M483 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 2.0 |
| E216M484 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 2.0 |
| E216M485 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 2.0 |
| E216M486 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 1.95 | 2.0 |
| E216M487 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.05 |
| E216M488 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.05 |
| E216M489 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.05 |
| E216M490 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.05 |
| E216M491 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.05 |
| E216M492 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.05 |
| E216M493 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.05 |
| E216M494 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.05 |
| E216M495 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 2.0 | 2.05 |
| E216M496 | dσ/dM(π−,p) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.1 |
| E216M497 | dσ/dM(π+,π−) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.1 |
| E216M498 | dσ/dM(π+,p) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.1 |
| E216M499 | dσ/dψ(π−) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.1 |
| E216M500 | dσ/dψ(π+) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.1 |
| E216M501 | dσ/dψ(p) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.1 |
| E216M502 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.1 |
| E216M503 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.1 |
| E216M504 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 3.5 | 4.2 | 2.05 | 2.1 |
| E216M505 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.45 |
| E216M506 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.45 |
| E216M507 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.45 |
| E216M508 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.45 |
| E216M509 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.45 |
| E216M510 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.45 |
| E216M511 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.45 |
| E216M512 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.45 |
| E216M513 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.4 | 1.45 |
| E216M514 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.5 |
| E216M515 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.5 |
| E216M516 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.5 |
| E216M517 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.5 |
| E216M518 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.5 |
| E216M519 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.5 |
| E216M520 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.5 |
| E216M521 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.5 |
| E216M522 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.45 | 1.5 |
| E216M523 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.55 |
| E216M524 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.55 |
| E216M525 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.55 |
| E216M526 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.55 |