E-94-005 CLAS experiment
- Spokesperson
- L. Elouadrhiri
- Year
- 2006
- Abstract
- Determination of the ND Axial Vector Tansition Form Factor from the ep -> e' Δ++π-
- Publication
-
- G.V.Fedotov, V.I.Mokeev, V.D.Burkert, L.Elouadrhiri, E.N.Golovatch, B.S.Ishkhanov, E.L.Isupov, N.V.Shvedunov, and CLAS Collaboration Electroproduction of pπ+π− off Protons at 0.2<Q2<0.6 GeV2 and 1.3<W<1.57 GeV with CLAS // PRC 79, 015204 (2009)
- 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/dφ(π−) dσ/dφ(π+) dσ/dφ(p) dσ/dψ(π−) dσ/dψ(π+) dσ/dψ(p) Aπ+ Bπ+ Cπ+ Aπ− Bπ− Cπ− Ap Bp Cp
Measurements
ID | Quantity | Beam | Target | Final state |
Q2min, GeV2 |
Q2max, GeV2 |
Wmin, GeV |
Wmax, GeV |
---|---|---|---|---|---|---|---|---|
E62M501 | dσ/dψ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.45 | 1.475 |
E62M502 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.4 | 0.45 | 1.45 | 1.475 |
E62M503 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.4 | 0.45 | 1.45 | 1.475 |
E62M504 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.4 | 0.45 | 1.45 | 1.475 |
E62M505 | dσ/dM(π−,p) | e | p | π+π−p | 0.4 | 0.45 | 1.475 | 1.5 |
E62M506 | dσ/dM(π+,π−) | e | p | π+π−p | 0.4 | 0.45 | 1.475 | 1.5 |
E62M507 | dσ/dM(π+,p) | e | p | π+π−p | 0.4 | 0.45 | 1.475 | 1.5 |
E62M508 | dσ/dφ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.475 | 1.5 |
E62M509 | dσ/dφ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.475 | 1.5 |
E62M510 | dσ/dφ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.475 | 1.5 |
E62M511 | dσ/dψ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.475 | 1.5 |
E62M512 | dσ/dψ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.475 | 1.5 |
E62M513 | dσ/dψ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.475 | 1.5 |
E62M514 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.4 | 0.45 | 1.475 | 1.5 |
E62M515 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.4 | 0.45 | 1.475 | 1.5 |
E62M516 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.4 | 0.45 | 1.475 | 1.5 |
E62M517 | dσ/dM(π−,p) | e | p | π+π−p | 0.4 | 0.45 | 1.5 | 1.525 |
E62M518 | dσ/dM(π+,π−) | e | p | π+π−p | 0.4 | 0.45 | 1.5 | 1.525 |
E62M519 | dσ/dM(π+,p) | e | p | π+π−p | 0.4 | 0.45 | 1.5 | 1.525 |
E62M520 | dσ/dφ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.5 | 1.525 |
E62M521 | dσ/dφ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.5 | 1.525 |
E62M522 | dσ/dφ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.5 | 1.525 |
E62M523 | dσ/dψ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.5 | 1.525 |
E62M524 | dσ/dψ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.5 | 1.525 |
E62M525 | dσ/dψ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.5 | 1.525 |
E62M526 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.4 | 0.45 | 1.5 | 1.525 |
E62M527 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.4 | 0.45 | 1.5 | 1.525 |
E62M528 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.4 | 0.45 | 1.5 | 1.525 |
E62M529 | dσ/dM(π−,p) | e | p | π+π−p | 0.45 | 0.5 | 1.3 | 1.325 |
E62M530 | dσ/dM(π+,π−) | e | p | π+π−p | 0.45 | 0.5 | 1.3 | 1.325 |
E62M531 | dσ/dM(π+,p) | e | p | π+π−p | 0.45 | 0.5 | 1.3 | 1.325 |
E62M532 | dσ/dφ(π−) | e | p | π+π−p | 0.45 | 0.5 | 1.3 | 1.325 |
E62M533 | dσ/dφ(π+) | e | p | π+π−p | 0.45 | 0.5 | 1.3 | 1.325 |
E62M534 | dσ/dφ(p) | e | p | π+π−p | 0.45 | 0.5 | 1.3 | 1.325 |
E62M535 | dσ/dψ(π−) | e | p | π+π−p | 0.45 | 0.5 | 1.3 | 1.325 |
E62M536 | dσ/dψ(π+) | e | p | π+π−p | 0.45 | 0.5 | 1.3 | 1.325 |
E62M537 | dσ/dψ(p) | e | p | π+π−p | 0.45 | 0.5 | 1.3 | 1.325 |
E62M538 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.45 | 0.5 | 1.3 | 1.325 |
E62M539 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.45 | 0.5 | 1.3 | 1.325 |
E62M540 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.45 | 0.5 | 1.3 | 1.325 |
E62M541 | dσ/dM(π−,p) | e | p | π+π−p | 0.45 | 0.5 | 1.325 | 1.35 |
E62M542 | dσ/dM(π+,π−) | e | p | π+π−p | 0.45 | 0.5 | 1.325 | 1.35 |
E62M543 | dσ/dM(π+,p) | e | p | π+π−p | 0.45 | 0.5 | 1.325 | 1.35 |
E62M544 | dσ/dφ(π−) | e | p | π+π−p | 0.45 | 0.5 | 1.325 | 1.35 |
E62M545 | dσ/dφ(π+) | e | p | π+π−p | 0.45 | 0.5 | 1.325 | 1.35 |
E62M546 | dσ/dφ(p) | e | p | π+π−p | 0.45 | 0.5 | 1.325 | 1.35 |
E62M547 | dσ/dψ(π−) | e | p | π+π−p | 0.45 | 0.5 | 1.325 | 1.35 |
E62M548 | dσ/dψ(π+) | e | p | π+π−p | 0.45 | 0.5 | 1.325 | 1.35 |
E62M549 | dσ/dψ(p) | e | p | π+π−p | 0.45 | 0.5 | 1.325 | 1.35 |
E62M550 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.45 | 0.5 | 1.325 | 1.35 |
E62M551 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.45 | 0.5 | 1.325 | 1.35 |
E62M552 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.45 | 0.5 | 1.325 | 1.35 |
E62M553 | dσ/dM(π−,p) | e | p | π+π−p | 0.45 | 0.5 | 1.35 | 1.375 |
E62M554 | dσ/dM(π+,π−) | e | p | π+π−p | 0.45 | 0.5 | 1.35 | 1.375 |
E62M555 | dσ/dM(π+,p) | e | p | π+π−p | 0.45 | 0.5 | 1.35 | 1.375 |
E62M556 | dσ/dφ(π−) | e | p | π+π−p | 0.45 | 0.5 | 1.35 | 1.375 |
E62M557 | dσ/dφ(π+) | e | p | π+π−p | 0.45 | 0.5 | 1.35 | 1.375 |
E62M558 | dσ/dφ(p) | e | p | π+π−p | 0.45 | 0.5 | 1.35 | 1.375 |
E62M559 | dσ/dψ(π−) | e | p | π+π−p | 0.45 | 0.5 | 1.35 | 1.375 |
E62M560 | dσ/dψ(π+) | e | p | π+π−p | 0.45 | 0.5 | 1.35 | 1.375 |
E62M561 | dσ/dψ(p) | e | p | π+π−p | 0.45 | 0.5 | 1.35 | 1.375 |
E62M562 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.45 | 0.5 | 1.35 | 1.375 |
E62M563 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.45 | 0.5 | 1.35 | 1.375 |
E62M564 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.45 | 0.5 | 1.35 | 1.375 |
E62M565 | dσ/dM(π−,p) | e | p | π+π−p | 0.45 | 0.5 | 1.375 | 1.4 |
E62M566 | dσ/dM(π+,π−) | e | p | π+π−p | 0.45 | 0.5 | 1.375 | 1.4 |
E62M567 | dσ/dM(π+,p) | e | p | π+π−p | 0.45 | 0.5 | 1.375 | 1.4 |
E62M568 | dσ/dφ(π−) | e | p | π+π−p | 0.45 | 0.5 | 1.375 | 1.4 |
E62M569 | dσ/dφ(π+) | e | p | π+π−p | 0.45 | 0.5 | 1.375 | 1.4 |
E62M570 | dσ/dφ(p) | e | p | π+π−p | 0.45 | 0.5 | 1.375 | 1.4 |
E62M571 | dσ/dψ(π−) | e | p | π+π−p | 0.45 | 0.5 | 1.375 | 1.4 |
E62M572 | dσ/dψ(π+) | e | p | π+π−p | 0.45 | 0.5 | 1.375 | 1.4 |
E62M573 | dσ/dψ(p) | e | p | π+π−p | 0.45 | 0.5 | 1.375 | 1.4 |
E62M574 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.45 | 0.5 | 1.375 | 1.4 |
E62M575 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.45 | 0.5 | 1.375 | 1.4 |
E62M576 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.45 | 0.5 | 1.375 | 1.4 |
E62M577 | dσ/dM(π−,p) | e | p | π+π−p | 0.45 | 0.5 | 1.4 | 1.425 |
E62M578 | dσ/dM(π+,π−) | e | p | π+π−p | 0.45 | 0.5 | 1.4 | 1.425 |
E62M579 | dσ/dM(π+,p) | e | p | π+π−p | 0.45 | 0.5 | 1.4 | 1.425 |
E62M580 | dσ/dφ(π−) | e | p | π+π−p | 0.45 | 0.5 | 1.4 | 1.425 |
E62M581 | dσ/dφ(π+) | e | p | π+π−p | 0.45 | 0.5 | 1.4 | 1.425 |
E62M582 | dσ/dφ(p) | e | p | π+π−p | 0.45 | 0.5 | 1.4 | 1.425 |
E62M583 | dσ/dψ(π−) | e | p | π+π−p | 0.45 | 0.5 | 1.4 | 1.425 |
E62M584 | dσ/dψ(π+) | e | p | π+π−p | 0.45 | 0.5 | 1.4 | 1.425 |
E62M585 | dσ/dψ(p) | e | p | π+π−p | 0.45 | 0.5 | 1.4 | 1.425 |
E62M586 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.45 | 0.5 | 1.4 | 1.425 |
E62M587 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.45 | 0.5 | 1.4 | 1.425 |
E62M588 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.45 | 0.5 | 1.4 | 1.425 |
E62M589 | dσ/dM(π−,p) | e | p | π+π−p | 0.45 | 0.5 | 1.425 | 1.45 |
E62M590 | dσ/dM(π+,π−) | e | p | π+π−p | 0.45 | 0.5 | 1.425 | 1.45 |
E62M591 | dσ/dM(π+,p) | e | p | π+π−p | 0.45 | 0.5 | 1.425 | 1.45 |
E62M592 | dσ/dφ(π−) | e | p | π+π−p | 0.45 | 0.5 | 1.425 | 1.45 |
E62M593 | dσ/dφ(π+) | e | p | π+π−p | 0.45 | 0.5 | 1.425 | 1.45 |
E62M594 | dσ/dφ(p) | e | p | π+π−p | 0.45 | 0.5 | 1.425 | 1.45 |
E62M595 | dσ/dψ(π−) | e | p | π+π−p | 0.45 | 0.5 | 1.425 | 1.45 |
E62M596 | dσ/dψ(π+) | e | p | π+π−p | 0.45 | 0.5 | 1.425 | 1.45 |
E62M597 | dσ/dψ(p) | e | p | π+π−p | 0.45 | 0.5 | 1.425 | 1.45 |
E62M598 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.45 | 0.5 | 1.425 | 1.45 |
E62M599 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.45 | 0.5 | 1.425 | 1.45 |
E62M600 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.45 | 0.5 | 1.425 | 1.45 |