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 |
|---|---|---|---|---|---|---|---|---|
| E216M527 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.55 |
| E216M528 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.55 |
| E216M529 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.55 |
| E216M530 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.55 |
| E216M531 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.55 |
| E216M532 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.55 | 1.6 |
| E216M533 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.55 | 1.6 |
| E216M534 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.55 | 1.6 |
| E216M535 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.55 | 1.6 |
| E216M536 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.55 | 1.6 |
| E216M537 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.55 | 1.6 |
| E216M538 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.55 | 1.6 |
| E216M539 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.55 | 1.6 |
| E216M540 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.55 | 1.6 |
| E216M541 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.6 | 1.65 |
| E216M542 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.6 | 1.65 |
| E216M543 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.6 | 1.65 |
| E216M544 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.6 | 1.65 |
| E216M545 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.6 | 1.65 |
| E216M546 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.6 | 1.65 |
| E216M547 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.6 | 1.65 |
| E216M548 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.6 | 1.65 |
| E216M549 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.6 | 1.65 |
| E216M550 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.65 | 1.7 |
| E216M551 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.65 | 1.7 |
| E216M552 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.65 | 1.7 |
| E216M553 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.65 | 1.7 |
| E216M554 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.65 | 1.7 |
| E216M555 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.65 | 1.7 |
| E216M556 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.65 | 1.7 |
| E216M557 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.65 | 1.7 |
| E216M558 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.65 | 1.7 |
| E216M559 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.7 | 1.75 |
| E216M560 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.7 | 1.75 |
| E216M561 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.7 | 1.75 |
| E216M562 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.7 | 1.75 |
| E216M563 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.7 | 1.75 |
| E216M564 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.7 | 1.75 |
| E216M565 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.7 | 1.75 |
| E216M566 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.7 | 1.75 |
| E216M567 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.7 | 1.75 |
| E216M568 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.75 | 1.8 |
| E216M569 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.75 | 1.8 |
| E216M570 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.75 | 1.8 |
| E216M571 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.75 | 1.8 |
| E216M572 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.75 | 1.8 |
| E216M573 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.75 | 1.8 |
| E216M574 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.75 | 1.8 |
| E216M575 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.75 | 1.8 |
| E216M576 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.75 | 1.8 |
| E216M577 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.8 | 1.85 |
| E216M578 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.8 | 1.85 |
| E216M579 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.8 | 1.85 |
| E216M580 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.8 | 1.85 |
| E216M581 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.8 | 1.85 |
| E216M582 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.8 | 1.85 |
| E216M583 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.8 | 1.85 |
| E216M584 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.8 | 1.85 |
| E216M585 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.8 | 1.85 |
| E216M586 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.9 |
| E216M587 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.9 |
| E216M588 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.9 |
| E216M589 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.9 |
| E216M590 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.9 |
| E216M591 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.9 |
| E216M592 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.9 |
| E216M593 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.9 |
| E216M594 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.9 |
| E216M595 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.95 |
| E216M596 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.95 |
| E216M597 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.95 |
| E216M598 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.95 |
| E216M599 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.95 |
| E216M600 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.95 |
| E216M601 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.95 |
| E216M602 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.95 |
| E216M603 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.95 |
| E216M604 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 2.0 |
| E216M605 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 2.0 |
| E216M606 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 2.0 |
| E216M607 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 2.0 |
| E216M608 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 2.0 |
| E216M609 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 2.0 |
| E216M610 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 2.0 |
| E216M611 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 2.0 |
| E216M612 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 2.0 |
| E216M613 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.05 |
| E216M614 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.05 |
| E216M615 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.05 |
| E216M616 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.05 |
| E216M617 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.05 |
| E216M618 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.05 |
| E216M619 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.05 |
| E216M620 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.05 |
| E216M621 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 2.0 | 2.05 |
| E216M622 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 2.05 | 2.1 |
| E216M623 | dσ/dM(π+,π−) | e | p | π+π−p | 4.2 | 5.0 | 2.05 | 2.1 |
| E216M624 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 2.05 | 2.1 |
| E216M625 | dσ/dψ(π−) | e | p | π+π−p | 4.2 | 5.0 | 2.05 | 2.1 |
| E216M626 | dσ/dψ(π+) | e | p | π+π−p | 4.2 | 5.0 | 2.05 | 2.1 |