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 |
---|---|---|---|---|---|---|---|---|
E62M401 | dσ/dφ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.5 | 1.525 |
E62M402 | dσ/dφ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.5 | 1.525 |
E62M403 | dσ/dψ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.5 | 1.525 |
E62M404 | dσ/dψ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.5 | 1.525 |
E62M405 | dσ/dψ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.5 | 1.525 |
E62M406 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.35 | 0.4 | 1.5 | 1.525 |
E62M407 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.35 | 0.4 | 1.5 | 1.525 |
E62M408 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.35 | 0.4 | 1.5 | 1.525 |
E62M409 | dσ/dM(π−,p) | e | p | π+π−p | 0.35 | 0.4 | 1.525 | 1.55 |
E62M410 | dσ/dM(π+,π−) | e | p | π+π−p | 0.35 | 0.4 | 1.525 | 1.55 |
E62M411 | dσ/dM(π+,p) | e | p | π+π−p | 0.35 | 0.4 | 1.525 | 1.55 |
E62M412 | dσ/dφ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.525 | 1.55 |
E62M413 | dσ/dφ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.525 | 1.55 |
E62M414 | dσ/dφ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.525 | 1.55 |
E62M415 | dσ/dψ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.525 | 1.55 |
E62M416 | dσ/dψ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.525 | 1.55 |
E62M417 | dσ/dψ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.525 | 1.55 |
E62M418 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.35 | 0.4 | 1.525 | 1.55 |
E62M419 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.35 | 0.4 | 1.525 | 1.55 |
E62M420 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.35 | 0.4 | 1.525 | 1.55 |
E62M421 | dσ/dM(π−,p) | e | p | π+π−p | 0.4 | 0.45 | 1.3 | 1.325 |
E62M422 | dσ/dM(π+,π−) | e | p | π+π−p | 0.4 | 0.45 | 1.3 | 1.325 |
E62M423 | dσ/dM(π+,p) | e | p | π+π−p | 0.4 | 0.45 | 1.3 | 1.325 |
E62M424 | dσ/dφ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.3 | 1.325 |
E62M425 | dσ/dφ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.3 | 1.325 |
E62M426 | dσ/dφ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.3 | 1.325 |
E62M427 | dσ/dψ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.3 | 1.325 |
E62M428 | dσ/dψ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.3 | 1.325 |
E62M429 | dσ/dψ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.3 | 1.325 |
E62M430 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.4 | 0.45 | 1.3 | 1.325 |
E62M431 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.4 | 0.45 | 1.3 | 1.325 |
E62M432 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.4 | 0.45 | 1.3 | 1.325 |
E62M433 | dσ/dM(π−,p) | e | p | π+π−p | 0.4 | 0.45 | 1.325 | 1.35 |
E62M434 | dσ/dM(π+,π−) | e | p | π+π−p | 0.4 | 0.45 | 1.325 | 1.35 |
E62M435 | dσ/dM(π+,p) | e | p | π+π−p | 0.4 | 0.45 | 1.325 | 1.35 |
E62M436 | dσ/dφ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.325 | 1.35 |
E62M437 | dσ/dφ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.325 | 1.35 |
E62M438 | dσ/dφ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.325 | 1.35 |
E62M439 | dσ/dψ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.325 | 1.35 |
E62M440 | dσ/dψ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.325 | 1.35 |
E62M441 | dσ/dψ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.325 | 1.35 |
E62M442 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.4 | 0.45 | 1.325 | 1.35 |
E62M443 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.4 | 0.45 | 1.325 | 1.35 |
E62M444 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.4 | 0.45 | 1.325 | 1.35 |
E62M445 | dσ/dM(π−,p) | e | p | π+π−p | 0.4 | 0.45 | 1.35 | 1.375 |
E62M446 | dσ/dM(π+,π−) | e | p | π+π−p | 0.4 | 0.45 | 1.35 | 1.375 |
E62M447 | dσ/dM(π+,p) | e | p | π+π−p | 0.4 | 0.45 | 1.35 | 1.375 |
E62M448 | dσ/dφ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.35 | 1.375 |
E62M449 | dσ/dφ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.35 | 1.375 |
E62M450 | dσ/dφ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.35 | 1.375 |
E62M451 | dσ/dψ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.35 | 1.375 |
E62M452 | dσ/dψ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.35 | 1.375 |
E62M453 | dσ/dψ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.35 | 1.375 |
E62M454 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.4 | 0.45 | 1.35 | 1.375 |
E62M455 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.4 | 0.45 | 1.35 | 1.375 |
E62M456 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.4 | 0.45 | 1.35 | 1.375 |
E62M457 | dσ/dM(π−,p) | e | p | π+π−p | 0.4 | 0.45 | 1.375 | 1.4 |
E62M458 | dσ/dM(π+,π−) | e | p | π+π−p | 0.4 | 0.45 | 1.375 | 1.4 |
E62M459 | dσ/dM(π+,p) | e | p | π+π−p | 0.4 | 0.45 | 1.375 | 1.4 |
E62M460 | dσ/dφ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.375 | 1.4 |
E62M461 | dσ/dφ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.375 | 1.4 |
E62M462 | dσ/dφ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.375 | 1.4 |
E62M463 | dσ/dψ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.375 | 1.4 |
E62M464 | dσ/dψ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.375 | 1.4 |
E62M465 | dσ/dψ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.375 | 1.4 |
E62M466 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.4 | 0.45 | 1.375 | 1.4 |
E62M467 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.4 | 0.45 | 1.375 | 1.4 |
E62M468 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.4 | 0.45 | 1.375 | 1.4 |
E62M469 | dσ/dM(π−,p) | e | p | π+π−p | 0.4 | 0.45 | 1.4 | 1.425 |
E62M470 | dσ/dM(π+,π−) | e | p | π+π−p | 0.4 | 0.45 | 1.4 | 1.425 |
E62M471 | dσ/dM(π+,p) | e | p | π+π−p | 0.4 | 0.45 | 1.4 | 1.425 |
E62M472 | dσ/dφ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.4 | 1.425 |
E62M473 | dσ/dφ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.4 | 1.425 |
E62M474 | dσ/dφ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.4 | 1.425 |
E62M475 | dσ/dψ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.4 | 1.425 |
E62M476 | dσ/dψ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.4 | 1.425 |
E62M477 | dσ/dψ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.4 | 1.425 |
E62M478 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.4 | 0.45 | 1.4 | 1.425 |
E62M479 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.4 | 0.45 | 1.4 | 1.425 |
E62M480 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.4 | 0.45 | 1.4 | 1.425 |
E62M481 | dσ/dM(π−,p) | e | p | π+π−p | 0.4 | 0.45 | 1.425 | 1.45 |
E62M482 | dσ/dM(π+,π−) | e | p | π+π−p | 0.4 | 0.45 | 1.425 | 1.45 |
E62M483 | dσ/dM(π+,p) | e | p | π+π−p | 0.4 | 0.45 | 1.425 | 1.45 |
E62M484 | dσ/dφ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.425 | 1.45 |
E62M485 | dσ/dφ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.425 | 1.45 |
E62M486 | dσ/dφ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.425 | 1.45 |
E62M487 | dσ/dψ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.425 | 1.45 |
E62M488 | dσ/dψ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.425 | 1.45 |
E62M489 | dσ/dψ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.425 | 1.45 |
E62M490 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.4 | 0.45 | 1.425 | 1.45 |
E62M491 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.4 | 0.45 | 1.425 | 1.45 |
E62M492 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.4 | 0.45 | 1.425 | 1.45 |
E62M493 | dσ/dM(π−,p) | e | p | π+π−p | 0.4 | 0.45 | 1.45 | 1.475 |
E62M494 | dσ/dM(π+,π−) | e | p | π+π−p | 0.4 | 0.45 | 1.45 | 1.475 |
E62M495 | dσ/dM(π+,p) | e | p | π+π−p | 0.4 | 0.45 | 1.45 | 1.475 |
E62M496 | dσ/dφ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.45 | 1.475 |
E62M497 | dσ/dφ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.45 | 1.475 |
E62M498 | dσ/dφ(p) | e | p | π+π−p | 0.4 | 0.45 | 1.45 | 1.475 |
E62M499 | dσ/dψ(π−) | e | p | π+π−p | 0.4 | 0.45 | 1.45 | 1.475 |
E62M500 | dσ/dψ(π+) | e | p | π+π−p | 0.4 | 0.45 | 1.45 | 1.475 |