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 |
---|---|---|---|---|---|---|---|---|
E62M201 | dσ/dψ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.325 | 1.35 |
E62M202 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.3 | 0.35 | 1.325 | 1.35 |
E62M203 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.3 | 0.35 | 1.325 | 1.35 |
E62M204 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.3 | 0.35 | 1.325 | 1.35 |
E62M205 | dσ/dM(π−,p) | e | p | π+π−p | 0.3 | 0.35 | 1.35 | 1.375 |
E62M206 | dσ/dM(π+,π−) | e | p | π+π−p | 0.3 | 0.35 | 1.35 | 1.375 |
E62M207 | dσ/dM(π+,p) | e | p | π+π−p | 0.3 | 0.35 | 1.35 | 1.375 |
E62M208 | dσ/dφ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.35 | 1.375 |
E62M209 | dσ/dφ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.35 | 1.375 |
E62M210 | dσ/dφ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.35 | 1.375 |
E62M211 | dσ/dψ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.35 | 1.375 |
E62M212 | dσ/dψ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.35 | 1.375 |
E62M213 | dσ/dψ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.35 | 1.375 |
E62M214 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.3 | 0.35 | 1.35 | 1.375 |
E62M215 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.3 | 0.35 | 1.35 | 1.375 |
E62M216 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.3 | 0.35 | 1.35 | 1.375 |
E62M217 | dσ/dM(π−,p) | e | p | π+π−p | 0.3 | 0.35 | 1.375 | 1.4 |
E62M218 | dσ/dM(π+,π−) | e | p | π+π−p | 0.3 | 0.35 | 1.375 | 1.4 |
E62M219 | dσ/dM(π+,p) | e | p | π+π−p | 0.3 | 0.35 | 1.375 | 1.4 |
E62M220 | dσ/dφ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.375 | 1.4 |
E62M221 | dσ/dφ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.375 | 1.4 |
E62M222 | dσ/dφ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.375 | 1.4 |
E62M223 | dσ/dψ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.375 | 1.4 |
E62M224 | dσ/dψ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.375 | 1.4 |
E62M225 | dσ/dψ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.375 | 1.4 |
E62M226 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.3 | 0.35 | 1.375 | 1.4 |
E62M227 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.3 | 0.35 | 1.375 | 1.4 |
E62M228 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.3 | 0.35 | 1.375 | 1.4 |
E62M229 | dσ/dM(π−,p) | e | p | π+π−p | 0.3 | 0.35 | 1.4 | 1.425 |
E62M230 | dσ/dM(π+,π−) | e | p | π+π−p | 0.3 | 0.35 | 1.4 | 1.425 |
E62M231 | dσ/dM(π+,p) | e | p | π+π−p | 0.3 | 0.35 | 1.4 | 1.425 |
E62M232 | dσ/dφ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.4 | 1.425 |
E62M233 | dσ/dφ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.4 | 1.425 |
E62M234 | dσ/dφ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.4 | 1.425 |
E62M235 | dσ/dψ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.4 | 1.425 |
E62M236 | dσ/dψ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.4 | 1.425 |
E62M237 | dσ/dψ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.4 | 1.425 |
E62M238 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.3 | 0.35 | 1.4 | 1.425 |
E62M239 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.3 | 0.35 | 1.4 | 1.425 |
E62M240 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.3 | 0.35 | 1.4 | 1.425 |
E62M241 | dσ/dM(π−,p) | e | p | π+π−p | 0.3 | 0.35 | 1.425 | 1.45 |
E62M242 | dσ/dM(π+,π−) | e | p | π+π−p | 0.3 | 0.35 | 1.425 | 1.45 |
E62M243 | dσ/dM(π+,p) | e | p | π+π−p | 0.3 | 0.35 | 1.425 | 1.45 |
E62M244 | dσ/dφ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.425 | 1.45 |
E62M245 | dσ/dφ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.425 | 1.45 |
E62M246 | dσ/dφ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.425 | 1.45 |
E62M247 | dσ/dψ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.425 | 1.45 |
E62M248 | dσ/dψ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.425 | 1.45 |
E62M249 | dσ/dψ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.425 | 1.45 |
E62M250 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.3 | 0.35 | 1.425 | 1.45 |
E62M251 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.3 | 0.35 | 1.425 | 1.45 |
E62M252 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.3 | 0.35 | 1.425 | 1.45 |
E62M253 | dσ/dM(π−,p) | e | p | π+π−p | 0.3 | 0.35 | 1.45 | 1.475 |
E62M254 | dσ/dM(π+,π−) | e | p | π+π−p | 0.3 | 0.35 | 1.45 | 1.475 |
E62M255 | dσ/dM(π+,p) | e | p | π+π−p | 0.3 | 0.35 | 1.45 | 1.475 |
E62M256 | dσ/dφ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.45 | 1.475 |
E62M257 | dσ/dφ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.45 | 1.475 |
E62M258 | dσ/dφ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.45 | 1.475 |
E62M259 | dσ/dψ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.45 | 1.475 |
E62M260 | dσ/dψ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.45 | 1.475 |
E62M261 | dσ/dψ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.45 | 1.475 |
E62M262 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.3 | 0.35 | 1.45 | 1.475 |
E62M263 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.3 | 0.35 | 1.45 | 1.475 |
E62M264 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.3 | 0.35 | 1.45 | 1.475 |
E62M265 | dσ/dM(π−,p) | e | p | π+π−p | 0.3 | 0.35 | 1.475 | 1.5 |
E62M266 | dσ/dM(π+,π−) | e | p | π+π−p | 0.3 | 0.35 | 1.475 | 1.5 |
E62M267 | dσ/dM(π+,p) | e | p | π+π−p | 0.3 | 0.35 | 1.475 | 1.5 |
E62M268 | dσ/dφ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.475 | 1.5 |
E62M269 | dσ/dφ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.475 | 1.5 |
E62M270 | dσ/dφ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.475 | 1.5 |
E62M271 | dσ/dψ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.475 | 1.5 |
E62M272 | dσ/dψ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.475 | 1.5 |
E62M273 | dσ/dψ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.475 | 1.5 |
E62M274 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.3 | 0.35 | 1.475 | 1.5 |
E62M275 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.3 | 0.35 | 1.475 | 1.5 |
E62M276 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.3 | 0.35 | 1.475 | 1.5 |
E62M277 | dσ/dM(π−,p) | e | p | π+π−p | 0.3 | 0.35 | 1.5 | 1.525 |
E62M278 | dσ/dM(π+,π−) | e | p | π+π−p | 0.3 | 0.35 | 1.5 | 1.525 |
E62M279 | dσ/dM(π+,p) | e | p | π+π−p | 0.3 | 0.35 | 1.5 | 1.525 |
E62M280 | dσ/dφ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.5 | 1.525 |
E62M281 | dσ/dφ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.5 | 1.525 |
E62M282 | dσ/dφ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.5 | 1.525 |
E62M283 | dσ/dψ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.5 | 1.525 |
E62M284 | dσ/dψ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.5 | 1.525 |
E62M285 | dσ/dψ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.5 | 1.525 |
E62M286 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.3 | 0.35 | 1.5 | 1.525 |
E62M287 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.3 | 0.35 | 1.5 | 1.525 |
E62M288 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.3 | 0.35 | 1.5 | 1.525 |
E62M289 | dσ/dM(π−,p) | e | p | π+π−p | 0.3 | 0.35 | 1.525 | 1.55 |
E62M290 | dσ/dM(π+,π−) | e | p | π+π−p | 0.3 | 0.35 | 1.525 | 1.55 |
E62M291 | dσ/dM(π+,p) | e | p | π+π−p | 0.3 | 0.35 | 1.525 | 1.55 |
E62M292 | dσ/dφ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.525 | 1.55 |
E62M293 | dσ/dφ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.525 | 1.55 |
E62M294 | dσ/dφ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.525 | 1.55 |
E62M295 | dσ/dψ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.525 | 1.55 |
E62M296 | dσ/dψ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.525 | 1.55 |
E62M297 | dσ/dψ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.525 | 1.55 |
E62M298 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.3 | 0.35 | 1.525 | 1.55 |
E62M299 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.3 | 0.35 | 1.525 | 1.55 |
E62M300 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.3 | 0.35 | 1.525 | 1.55 |