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 |
---|---|---|---|---|---|---|---|---|
E62M101 | dσ/dφ(π+) | e | p | π+π−p | 0.25 | 0.3 | 1.4 | 1.425 |
E62M102 | dσ/dφ(p) | e | p | π+π−p | 0.25 | 0.3 | 1.4 | 1.425 |
E62M103 | dσ/dψ(π−) | e | p | π+π−p | 0.25 | 0.3 | 1.4 | 1.425 |
E62M104 | dσ/dψ(π+) | e | p | π+π−p | 0.25 | 0.3 | 1.4 | 1.425 |
E62M105 | dσ/dψ(p) | e | p | π+π−p | 0.25 | 0.3 | 1.4 | 1.425 |
E62M106 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.25 | 0.3 | 1.4 | 1.425 |
E62M107 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.25 | 0.3 | 1.4 | 1.425 |
E62M108 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.25 | 0.3 | 1.4 | 1.425 |
E62M109 | dσ/dM(π−,p) | e | p | π+π−p | 0.25 | 0.3 | 1.425 | 1.45 |
E62M110 | dσ/dM(π+,π−) | e | p | π+π−p | 0.25 | 0.3 | 1.425 | 1.45 |
E62M111 | dσ/dM(π+,p) | e | p | π+π−p | 0.25 | 0.3 | 1.425 | 1.45 |
E62M112 | dσ/dφ(π−) | e | p | π+π−p | 0.25 | 0.3 | 1.425 | 1.45 |
E62M113 | dσ/dφ(π+) | e | p | π+π−p | 0.25 | 0.3 | 1.425 | 1.45 |
E62M114 | dσ/dφ(p) | e | p | π+π−p | 0.25 | 0.3 | 1.425 | 1.45 |
E62M115 | dσ/dψ(π−) | e | p | π+π−p | 0.25 | 0.3 | 1.425 | 1.45 |
E62M116 | dσ/dψ(π+) | e | p | π+π−p | 0.25 | 0.3 | 1.425 | 1.45 |
E62M117 | dσ/dψ(p) | e | p | π+π−p | 0.25 | 0.3 | 1.425 | 1.45 |
E62M118 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.25 | 0.3 | 1.425 | 1.45 |
E62M119 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.25 | 0.3 | 1.425 | 1.45 |
E62M120 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.25 | 0.3 | 1.425 | 1.45 |
E62M121 | dσ/dM(π−,p) | e | p | π+π−p | 0.25 | 0.3 | 1.45 | 1.475 |
E62M122 | dσ/dM(π+,π−) | e | p | π+π−p | 0.25 | 0.3 | 1.45 | 1.475 |
E62M123 | dσ/dM(π+,p) | e | p | π+π−p | 0.25 | 0.3 | 1.45 | 1.475 |
E62M124 | dσ/dφ(π−) | e | p | π+π−p | 0.25 | 0.3 | 1.45 | 1.475 |
E62M125 | dσ/dφ(π+) | e | p | π+π−p | 0.25 | 0.3 | 1.45 | 1.475 |
E62M126 | dσ/dφ(p) | e | p | π+π−p | 0.25 | 0.3 | 1.45 | 1.475 |
E62M127 | dσ/dψ(π−) | e | p | π+π−p | 0.25 | 0.3 | 1.45 | 1.475 |
E62M128 | dσ/dψ(π+) | e | p | π+π−p | 0.25 | 0.3 | 1.45 | 1.475 |
E62M129 | dσ/dψ(p) | e | p | π+π−p | 0.25 | 0.3 | 1.45 | 1.475 |
E62M130 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.25 | 0.3 | 1.45 | 1.475 |
E62M131 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.25 | 0.3 | 1.45 | 1.475 |
E62M132 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.25 | 0.3 | 1.45 | 1.475 |
E62M133 | dσ/dM(π−,p) | e | p | π+π−p | 0.25 | 0.3 | 1.475 | 1.5 |
E62M134 | dσ/dM(π+,π−) | e | p | π+π−p | 0.25 | 0.3 | 1.475 | 1.5 |
E62M135 | dσ/dM(π+,p) | e | p | π+π−p | 0.25 | 0.3 | 1.475 | 1.5 |
E62M136 | dσ/dφ(π−) | e | p | π+π−p | 0.25 | 0.3 | 1.475 | 1.5 |
E62M137 | dσ/dφ(π+) | e | p | π+π−p | 0.25 | 0.3 | 1.475 | 1.5 |
E62M138 | dσ/dφ(p) | e | p | π+π−p | 0.25 | 0.3 | 1.475 | 1.5 |
E62M139 | dσ/dψ(π−) | e | p | π+π−p | 0.25 | 0.3 | 1.475 | 1.5 |
E62M140 | dσ/dψ(π+) | e | p | π+π−p | 0.25 | 0.3 | 1.475 | 1.5 |
E62M141 | dσ/dψ(p) | e | p | π+π−p | 0.25 | 0.3 | 1.475 | 1.5 |
E62M142 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.25 | 0.3 | 1.475 | 1.5 |
E62M143 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.25 | 0.3 | 1.475 | 1.5 |
E62M144 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.25 | 0.3 | 1.475 | 1.5 |
E62M145 | dσ/dM(π−,p) | e | p | π+π−p | 0.25 | 0.3 | 1.5 | 1.525 |
E62M146 | dσ/dM(π+,π−) | e | p | π+π−p | 0.25 | 0.3 | 1.5 | 1.525 |
E62M147 | dσ/dM(π+,p) | e | p | π+π−p | 0.25 | 0.3 | 1.5 | 1.525 |
E62M148 | dσ/dφ(π−) | e | p | π+π−p | 0.25 | 0.3 | 1.5 | 1.525 |
E62M149 | dσ/dφ(π+) | e | p | π+π−p | 0.25 | 0.3 | 1.5 | 1.525 |
E62M150 | dσ/dφ(p) | e | p | π+π−p | 0.25 | 0.3 | 1.5 | 1.525 |
E62M151 | dσ/dψ(π−) | e | p | π+π−p | 0.25 | 0.3 | 1.5 | 1.525 |
E62M152 | dσ/dψ(π+) | e | p | π+π−p | 0.25 | 0.3 | 1.5 | 1.525 |
E62M153 | dσ/dψ(p) | e | p | π+π−p | 0.25 | 0.3 | 1.5 | 1.525 |
E62M154 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.25 | 0.3 | 1.5 | 1.525 |
E62M155 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.25 | 0.3 | 1.5 | 1.525 |
E62M156 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.25 | 0.3 | 1.5 | 1.525 |
E62M157 | dσ/dM(π−,p) | e | p | π+π−p | 0.25 | 0.3 | 1.525 | 1.55 |
E62M158 | dσ/dM(π+,π−) | e | p | π+π−p | 0.25 | 0.3 | 1.525 | 1.55 |
E62M159 | dσ/dM(π+,p) | e | p | π+π−p | 0.25 | 0.3 | 1.525 | 1.55 |
E62M160 | dσ/dφ(π−) | e | p | π+π−p | 0.25 | 0.3 | 1.525 | 1.55 |
E62M161 | dσ/dφ(π+) | e | p | π+π−p | 0.25 | 0.3 | 1.525 | 1.55 |
E62M162 | dσ/dφ(p) | e | p | π+π−p | 0.25 | 0.3 | 1.525 | 1.55 |
E62M163 | dσ/dψ(π−) | e | p | π+π−p | 0.25 | 0.3 | 1.525 | 1.55 |
E62M164 | dσ/dψ(π+) | e | p | π+π−p | 0.25 | 0.3 | 1.525 | 1.55 |
E62M165 | dσ/dψ(p) | e | p | π+π−p | 0.25 | 0.3 | 1.525 | 1.55 |
E62M166 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.25 | 0.3 | 1.525 | 1.55 |
E62M167 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.25 | 0.3 | 1.525 | 1.55 |
E62M168 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.25 | 0.3 | 1.525 | 1.55 |
E62M169 | dσ/dM(π−,p) | e | p | π+π−p | 0.25 | 0.3 | 1.55 | 1.575 |
E62M170 | dσ/dM(π+,π−) | e | p | π+π−p | 0.25 | 0.3 | 1.55 | 1.575 |
E62M171 | dσ/dM(π+,p) | e | p | π+π−p | 0.25 | 0.3 | 1.55 | 1.575 |
E62M172 | dσ/dφ(π−) | e | p | π+π−p | 0.25 | 0.3 | 1.55 | 1.575 |
E62M173 | dσ/dφ(π+) | e | p | π+π−p | 0.25 | 0.3 | 1.55 | 1.575 |
E62M174 | dσ/dφ(p) | e | p | π+π−p | 0.25 | 0.3 | 1.55 | 1.575 |
E62M175 | dσ/dψ(π−) | e | p | π+π−p | 0.25 | 0.3 | 1.55 | 1.575 |
E62M176 | dσ/dψ(π+) | e | p | π+π−p | 0.25 | 0.3 | 1.55 | 1.575 |
E62M177 | dσ/dψ(p) | e | p | π+π−p | 0.25 | 0.3 | 1.55 | 1.575 |
E62M178 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.25 | 0.3 | 1.55 | 1.575 |
E62M179 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.25 | 0.3 | 1.55 | 1.575 |
E62M180 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.25 | 0.3 | 1.55 | 1.575 |
E62M181 | dσ/dM(π−,p) | e | p | π+π−p | 0.3 | 0.35 | 1.3 | 1.325 |
E62M182 | dσ/dM(π+,π−) | e | p | π+π−p | 0.3 | 0.35 | 1.3 | 1.325 |
E62M183 | dσ/dM(π+,p) | e | p | π+π−p | 0.3 | 0.35 | 1.3 | 1.325 |
E62M184 | dσ/dφ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.3 | 1.325 |
E62M185 | dσ/dφ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.3 | 1.325 |
E62M186 | dσ/dφ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.3 | 1.325 |
E62M187 | dσ/dψ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.3 | 1.325 |
E62M188 | dσ/dψ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.3 | 1.325 |
E62M189 | dσ/dψ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.3 | 1.325 |
E62M190 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.3 | 0.35 | 1.3 | 1.325 |
E62M191 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.3 | 0.35 | 1.3 | 1.325 |
E62M192 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.3 | 0.35 | 1.3 | 1.325 |
E62M193 | dσ/dM(π−,p) | e | p | π+π−p | 0.3 | 0.35 | 1.325 | 1.35 |
E62M194 | dσ/dM(π+,π−) | e | p | π+π−p | 0.3 | 0.35 | 1.325 | 1.35 |
E62M195 | dσ/dM(π+,p) | e | p | π+π−p | 0.3 | 0.35 | 1.325 | 1.35 |
E62M196 | dσ/dφ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.325 | 1.35 |
E62M197 | dσ/dφ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.325 | 1.35 |
E62M198 | dσ/dφ(p) | e | p | π+π−p | 0.3 | 0.35 | 1.325 | 1.35 |
E62M199 | dσ/dψ(π−) | e | p | π+π−p | 0.3 | 0.35 | 1.325 | 1.35 |
E62M200 | dσ/dψ(π+) | e | p | π+π−p | 0.3 | 0.35 | 1.325 | 1.35 |