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 |
---|---|---|---|---|---|---|---|---|
E62M301 | dσ/dM(π−,p) | e | p | π+π−p | 0.35 | 0.4 | 1.3 | 1.325 |
E62M302 | dσ/dM(π+,π−) | e | p | π+π−p | 0.35 | 0.4 | 1.3 | 1.325 |
E62M303 | dσ/dM(π+,p) | e | p | π+π−p | 0.35 | 0.4 | 1.3 | 1.325 |
E62M304 | dσ/dφ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.3 | 1.325 |
E62M305 | dσ/dφ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.3 | 1.325 |
E62M306 | dσ/dφ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.3 | 1.325 |
E62M307 | dσ/dψ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.3 | 1.325 |
E62M308 | dσ/dψ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.3 | 1.325 |
E62M309 | dσ/dψ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.3 | 1.325 |
E62M310 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.35 | 0.4 | 1.3 | 1.325 |
E62M311 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.35 | 0.4 | 1.3 | 1.325 |
E62M312 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.35 | 0.4 | 1.3 | 1.325 |
E62M313 | dσ/dM(π−,p) | e | p | π+π−p | 0.35 | 0.4 | 1.325 | 1.35 |
E62M314 | dσ/dM(π+,π−) | e | p | π+π−p | 0.35 | 0.4 | 1.325 | 1.35 |
E62M315 | dσ/dM(π+,p) | e | p | π+π−p | 0.35 | 0.4 | 1.325 | 1.35 |
E62M316 | dσ/dφ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.325 | 1.35 |
E62M317 | dσ/dφ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.325 | 1.35 |
E62M318 | dσ/dφ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.325 | 1.35 |
E62M319 | dσ/dψ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.325 | 1.35 |
E62M320 | dσ/dψ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.325 | 1.35 |
E62M321 | dσ/dψ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.325 | 1.35 |
E62M322 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.35 | 0.4 | 1.325 | 1.35 |
E62M323 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.35 | 0.4 | 1.325 | 1.35 |
E62M324 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.35 | 0.4 | 1.325 | 1.35 |
E62M325 | dσ/dM(π−,p) | e | p | π+π−p | 0.35 | 0.4 | 1.35 | 1.375 |
E62M326 | dσ/dM(π+,π−) | e | p | π+π−p | 0.35 | 0.4 | 1.35 | 1.375 |
E62M327 | dσ/dM(π+,p) | e | p | π+π−p | 0.35 | 0.4 | 1.35 | 1.375 |
E62M328 | dσ/dφ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.35 | 1.375 |
E62M329 | dσ/dφ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.35 | 1.375 |
E62M330 | dσ/dφ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.35 | 1.375 |
E62M331 | dσ/dψ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.35 | 1.375 |
E62M332 | dσ/dψ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.35 | 1.375 |
E62M333 | dσ/dψ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.35 | 1.375 |
E62M334 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.35 | 0.4 | 1.35 | 1.375 |
E62M335 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.35 | 0.4 | 1.35 | 1.375 |
E62M336 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.35 | 0.4 | 1.35 | 1.375 |
E62M337 | dσ/dM(π−,p) | e | p | π+π−p | 0.35 | 0.4 | 1.375 | 1.4 |
E62M338 | dσ/dM(π+,π−) | e | p | π+π−p | 0.35 | 0.4 | 1.375 | 1.4 |
E62M339 | dσ/dM(π+,p) | e | p | π+π−p | 0.35 | 0.4 | 1.375 | 1.4 |
E62M340 | dσ/dφ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.375 | 1.4 |
E62M341 | dσ/dφ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.375 | 1.4 |
E62M342 | dσ/dφ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.375 | 1.4 |
E62M343 | dσ/dψ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.375 | 1.4 |
E62M344 | dσ/dψ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.375 | 1.4 |
E62M345 | dσ/dψ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.375 | 1.4 |
E62M346 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.35 | 0.4 | 1.375 | 1.4 |
E62M347 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.35 | 0.4 | 1.375 | 1.4 |
E62M348 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.35 | 0.4 | 1.375 | 1.4 |
E62M349 | dσ/dM(π−,p) | e | p | π+π−p | 0.35 | 0.4 | 1.4 | 1.425 |
E62M350 | dσ/dM(π+,π−) | e | p | π+π−p | 0.35 | 0.4 | 1.4 | 1.425 |
E62M351 | dσ/dM(π+,p) | e | p | π+π−p | 0.35 | 0.4 | 1.4 | 1.425 |
E62M352 | dσ/dφ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.4 | 1.425 |
E62M353 | dσ/dφ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.4 | 1.425 |
E62M354 | dσ/dφ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.4 | 1.425 |
E62M355 | dσ/dψ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.4 | 1.425 |
E62M356 | dσ/dψ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.4 | 1.425 |
E62M357 | dσ/dψ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.4 | 1.425 |
E62M358 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.35 | 0.4 | 1.4 | 1.425 |
E62M359 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.35 | 0.4 | 1.4 | 1.425 |
E62M360 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.35 | 0.4 | 1.4 | 1.425 |
E62M361 | dσ/dM(π−,p) | e | p | π+π−p | 0.35 | 0.4 | 1.425 | 1.45 |
E62M362 | dσ/dM(π+,π−) | e | p | π+π−p | 0.35 | 0.4 | 1.425 | 1.45 |
E62M363 | dσ/dM(π+,p) | e | p | π+π−p | 0.35 | 0.4 | 1.425 | 1.45 |
E62M364 | dσ/dφ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.425 | 1.45 |
E62M365 | dσ/dφ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.425 | 1.45 |
E62M366 | dσ/dφ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.425 | 1.45 |
E62M367 | dσ/dψ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.425 | 1.45 |
E62M368 | dσ/dψ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.425 | 1.45 |
E62M369 | dσ/dψ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.425 | 1.45 |
E62M370 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.35 | 0.4 | 1.425 | 1.45 |
E62M371 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.35 | 0.4 | 1.425 | 1.45 |
E62M372 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.35 | 0.4 | 1.425 | 1.45 |
E62M373 | dσ/dM(π−,p) | e | p | π+π−p | 0.35 | 0.4 | 1.45 | 1.475 |
E62M374 | dσ/dM(π+,π−) | e | p | π+π−p | 0.35 | 0.4 | 1.45 | 1.475 |
E62M375 | dσ/dM(π+,p) | e | p | π+π−p | 0.35 | 0.4 | 1.45 | 1.475 |
E62M376 | dσ/dφ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.45 | 1.475 |
E62M377 | dσ/dφ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.45 | 1.475 |
E62M378 | dσ/dφ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.45 | 1.475 |
E62M379 | dσ/dψ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.45 | 1.475 |
E62M380 | dσ/dψ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.45 | 1.475 |
E62M381 | dσ/dψ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.45 | 1.475 |
E62M382 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.35 | 0.4 | 1.45 | 1.475 |
E62M383 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.35 | 0.4 | 1.45 | 1.475 |
E62M384 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.35 | 0.4 | 1.45 | 1.475 |
E62M385 | dσ/dM(π−,p) | e | p | π+π−p | 0.35 | 0.4 | 1.475 | 1.5 |
E62M386 | dσ/dM(π+,π−) | e | p | π+π−p | 0.35 | 0.4 | 1.475 | 1.5 |
E62M387 | dσ/dM(π+,p) | e | p | π+π−p | 0.35 | 0.4 | 1.475 | 1.5 |
E62M388 | dσ/dφ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.475 | 1.5 |
E62M389 | dσ/dφ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.475 | 1.5 |
E62M390 | dσ/dφ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.475 | 1.5 |
E62M391 | dσ/dψ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.475 | 1.5 |
E62M392 | dσ/dψ(π+) | e | p | π+π−p | 0.35 | 0.4 | 1.475 | 1.5 |
E62M393 | dσ/dψ(p) | e | p | π+π−p | 0.35 | 0.4 | 1.475 | 1.5 |
E62M394 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.35 | 0.4 | 1.475 | 1.5 |
E62M395 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.35 | 0.4 | 1.475 | 1.5 |
E62M396 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.35 | 0.4 | 1.475 | 1.5 |
E62M397 | dσ/dM(π−,p) | e | p | π+π−p | 0.35 | 0.4 | 1.5 | 1.525 |
E62M398 | dσ/dM(π+,π−) | e | p | π+π−p | 0.35 | 0.4 | 1.5 | 1.525 |
E62M399 | dσ/dM(π+,p) | e | p | π+π−p | 0.35 | 0.4 | 1.5 | 1.525 |
E62M400 | dσ/dφ(π−) | e | p | π+π−p | 0.35 | 0.4 | 1.5 | 1.525 |