E93-006 CLAS experiment
- Spokespersons
- V. D. Burkert, M. Ripani
- Year
- 2003
- Abstract
- The cross section for the reaction ep -> e' p pi+ pi- was measured in the resonance region for 1.4 < W < 2.1 GeV and 0.5 < Q2 < 1.5 GeV2/c2 using the CLAS detector at Jefferson Laboratory. The data show resonant structures not visible in previous experiments. The comparison of our data to a phenomenological prediction using available information on N* and Delta states shows an evident discrepancy. A better description of the data is obtained either by a sizable change of the properties of the P13(1720) resonance or by introducing a new baryon state, not reported in published analyses.
- Publication
-
- M. Ripani, V. D. Burkert, V. I. Mokeev, M. Battaglieri, R. De Vita, E. Golovach, V. Tauti, and CLAS Collaboration Measurement of ep->e'p pi+pi- and Baryon Resonance Analysis // Phys. Rev. Let. 91, 022002 (2003)
- 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)
Measurements
ID | Quantity | Beam | Target | Final state |
Q2min, GeV2 |
Q2max, GeV2 |
Wmin, GeV |
Wmax, GeV |
---|---|---|---|---|---|---|---|---|
E1M101 | dσ/dφ(π−) | e | p | π+π−p | 1.1 | 1.5 | 1.6 | 1.625 |
E1M102 | dσ/dφ(p) | e | p | π+π−p | 1.1 | 1.5 | 1.6 | 1.625 |
E1M103 | dσ/dφ(π+) | e | p | π+π−p | 1.1 | 1.5 | 1.6 | 1.625 |
E1M104 | dσ/dψ(π−) | e | p | π+π−p | 1.1 | 1.5 | 1.6 | 1.625 |
E1M105 | dσ/dψ(π+) | e | p | π+π−p | 1.1 | 1.5 | 1.6 | 1.625 |
E1M106 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 1.1 | 1.5 | 1.6 | 1.625 |
E1M107 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 1.1 | 1.5 | 1.6 | 1.625 |
E1M108 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 1.1 | 1.5 | 1.625 | 1.65 |
E1M109 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 1.1 | 1.5 | 1.625 | 1.65 |
E1M110 | dσ/dM(π−,p) | e | p | π+π−p | 1.1 | 1.5 | 1.625 | 1.65 |
E1M111 | dσ/dM(π+,p) | e | p | π+π−p | 1.1 | 1.5 | 1.625 | 1.65 |
E1M112 | dσ/dφ(π+) | e | p | π+π−p | 1.1 | 1.5 | 1.625 | 1.65 |
E1M113 | dσ/dφ(p) | e | p | π+π−p | 1.1 | 1.5 | 1.625 | 1.65 |
E1M114 | dσ/dψ(π−) | e | p | π+π−p | 1.1 | 1.5 | 1.625 | 1.65 |
E1M115 | dσ/dψ(π+) | e | p | π+π−p | 1.1 | 1.5 | 1.625 | 1.65 |
E1M116 | dσ/dψ(p) | e | p | π+π−p | 1.1 | 1.5 | 1.625 | 1.65 |
E1M117 | dσ/dφ(π−) | e | p | π+π−p | 1.1 | 1.5 | 1.625 | 1.65 |
E1M118 | dσ/dM(π+,π−) | e | p | π+π−p | 1.1 | 1.5 | 1.625 | 1.65 |
E1M119 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 1.1 | 1.5 | 1.625 | 1.65 |
E1M120 | dσ/dM(π−,p) | e | p | π+π−p | 1.1 | 1.5 | 1.65 | 1.675 |
E1M121 | dσ/dψ(π−) | e | p | π+π−p | 1.1 | 1.5 | 1.65 | 1.675 |
E1M122 | dσ/dM(π+,p) | e | p | π+π−p | 1.1 | 1.5 | 1.65 | 1.675 |
E1M123 | dσ/dφ(π−) | e | p | π+π−p | 1.1 | 1.5 | 1.65 | 1.675 |
E1M124 | dσ/dφ(π+) | e | p | π+π−p | 1.1 | 1.5 | 1.65 | 1.675 |
E1M125 | dσ/dφ(p) | e | p | π+π−p | 1.1 | 1.5 | 1.65 | 1.675 |
E1M126 | dσ/dψ(π+) | e | p | π+π−p | 1.1 | 1.5 | 1.65 | 1.675 |
E1M127 | dσ/dψ(p) | e | p | π+π−p | 1.1 | 1.5 | 1.65 | 1.675 |
E1M128 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 1.1 | 1.5 | 1.65 | 1.675 |
E1M129 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 1.1 | 1.5 | 1.65 | 1.675 |
E1M130 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 1.1 | 1.5 | 1.65 | 1.675 |
E1M131 | dσ/dM(π+,π−) | e | p | π+π−p | 1.1 | 1.5 | 1.65 | 1.675 |
E1M132 | dσ/dM(π−,p) | e | p | π+π−p | 1.1 | 1.5 | 1.675 | 1.7 |
E1M133 | dσ/dψ(π−) | e | p | π+π−p | 1.1 | 1.5 | 1.675 | 1.7 |
E1M134 | dσ/dM(π+,p) | e | p | π+π−p | 1.1 | 1.5 | 1.675 | 1.7 |
E1M135 | dσ/dφ(π−) | e | p | π+π−p | 1.1 | 1.5 | 1.675 | 1.7 |
E1M136 | dσ/dφ(π+) | e | p | π+π−p | 1.1 | 1.5 | 1.675 | 1.7 |
E1M137 | dσ/dφ(p) | e | p | π+π−p | 1.1 | 1.5 | 1.675 | 1.7 |
E1M138 | dσ/dψ(π+) | e | p | π+π−p | 1.1 | 1.5 | 1.675 | 1.7 |
E1M139 | dσ/dψ(p) | e | p | π+π−p | 1.1 | 1.5 | 1.675 | 1.7 |
E1M140 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 1.1 | 1.5 | 1.675 | 1.7 |
E1M141 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 1.1 | 1.5 | 1.675 | 1.7 |
E1M142 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 1.1 | 1.5 | 1.675 | 1.7 |
E1M143 | dσ/dM(π+,π−) | e | p | π+π−p | 1.1 | 1.5 | 1.675 | 1.7 |
E1M144 | dσ/dM(π+,π−) | e | p | π+π−p | 1.1 | 1.5 | 1.7 | 1.725 |
E1M145 | dσ/dψ(p) | e | p | π+π−p | 1.1 | 1.5 | 1.7 | 1.725 |
E1M146 | dσ/dφ(π+) | e | p | π+π−p | 1.1 | 1.5 | 1.7 | 1.725 |
E1M147 | dσ/dM(π−,p) | e | p | π+π−p | 1.1 | 1.5 | 1.7 | 1.725 |
E1M148 | dσ/dM(π+,p) | e | p | π+π−p | 1.1 | 1.5 | 1.7 | 1.725 |
E1M149 | dσ/dφ(π−) | e | p | π+π−p | 1.1 | 1.5 | 1.7 | 1.725 |
E1M150 | dσ/dφ(p) | e | p | π+π−p | 1.1 | 1.5 | 1.7 | 1.725 |
E1M151 | dσ/dψ(π−) | e | p | π+π−p | 1.1 | 1.5 | 1.7 | 1.725 |
E1M152 | dσ/dψ(π+) | e | p | π+π−p | 1.1 | 1.5 | 1.7 | 1.725 |
E1M153 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 1.1 | 1.5 | 1.7 | 1.725 |
E1M154 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 1.1 | 1.5 | 1.7 | 1.725 |
E1M155 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 1.1 | 1.5 | 1.7 | 1.725 |
E1M156 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 1.1 | 1.5 | 1.725 | 1.75 |
E1M157 | dσ/dM(π−,p) | e | p | π+π−p | 1.1 | 1.5 | 1.725 | 1.75 |
E1M158 | dσ/dφ(π+) | e | p | π+π−p | 1.1 | 1.5 | 1.725 | 1.75 |
E1M159 | dσ/dM(π+,π−) | e | p | π+π−p | 1.1 | 1.5 | 1.725 | 1.75 |
E1M160 | dσ/dM(π+,p) | e | p | π+π−p | 1.1 | 1.5 | 1.725 | 1.75 |
E1M161 | dσ/dφ(π−) | e | p | π+π−p | 1.1 | 1.5 | 1.725 | 1.75 |
E1M162 | dσ/dψ(π−) | e | p | π+π−p | 1.1 | 1.5 | 1.725 | 1.75 |
E1M163 | dσ/dψ(p) | e | p | π+π−p | 1.1 | 1.5 | 1.725 | 1.75 |
E1M164 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 1.1 | 1.5 | 1.725 | 1.75 |
E1M165 | dσ/dφ(p) | e | p | π+π−p | 1.1 | 1.5 | 1.725 | 1.75 |
E1M166 | dσ/dψ(π+) | e | p | π+π−p | 1.1 | 1.5 | 1.725 | 1.75 |
E1M167 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 1.1 | 1.5 | 1.725 | 1.75 |
E1M168 | dσ/dM(π+,π−) | e | p | π+π−p | 1.1 | 1.5 | 1.75 | 1.775 |
E1M169 | dσ/dψ(p) | e | p | π+π−p | 1.1 | 1.5 | 1.75 | 1.775 |
E1M170 | dσ/dφ(π+) | e | p | π+π−p | 1.1 | 1.5 | 1.75 | 1.775 |
E1M171 | dσ/dM(π−,p) | e | p | π+π−p | 1.1 | 1.5 | 1.75 | 1.775 |
E1M172 | dσ/dM(π+,p) | e | p | π+π−p | 1.1 | 1.5 | 1.75 | 1.775 |
E1M173 | dσ/dφ(π−) | e | p | π+π−p | 1.1 | 1.5 | 1.75 | 1.775 |
E1M174 | dσ/dφ(p) | e | p | π+π−p | 1.1 | 1.5 | 1.75 | 1.775 |
E1M175 | dσ/dψ(π−) | e | p | π+π−p | 1.1 | 1.5 | 1.75 | 1.775 |
E1M176 | dσ/dψ(π+) | e | p | π+π−p | 1.1 | 1.5 | 1.75 | 1.775 |
E1M177 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 1.1 | 1.5 | 1.75 | 1.775 |
E1M178 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 1.1 | 1.5 | 1.75 | 1.775 |
E1M179 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 1.1 | 1.5 | 1.75 | 1.775 |
E1M180 | dσ/dM(π+,π−) | e | p | π+π−p | 1.1 | 1.5 | 1.775 | 1.8 |
E1M181 | dσ/dψ(p) | e | p | π+π−p | 1.1 | 1.5 | 1.775 | 1.8 |
E1M182 | dσ/dφ(π+) | e | p | π+π−p | 1.1 | 1.5 | 1.775 | 1.8 |
E1M183 | dσ/dM(π−,p) | e | p | π+π−p | 1.1 | 1.5 | 1.775 | 1.8 |
E1M184 | dσ/dM(π+,p) | e | p | π+π−p | 1.1 | 1.5 | 1.775 | 1.8 |
E1M185 | dσ/dφ(π−) | e | p | π+π−p | 1.1 | 1.5 | 1.775 | 1.8 |
E1M186 | dσ/dφ(p) | e | p | π+π−p | 1.1 | 1.5 | 1.775 | 1.8 |
E1M187 | dσ/dψ(π−) | e | p | π+π−p | 1.1 | 1.5 | 1.775 | 1.8 |
E1M188 | dσ/dψ(π+) | e | p | π+π−p | 1.1 | 1.5 | 1.775 | 1.8 |
E1M189 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 1.1 | 1.5 | 1.775 | 1.8 |
E1M190 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 1.1 | 1.5 | 1.775 | 1.8 |
E1M191 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 1.1 | 1.5 | 1.775 | 1.8 |
E1M192 | dσ/dψ(p) | e | p | π+π−p | 1.1 | 1.5 | 1.8 | 1.825 |
E1M193 | dσ/dφ(π+) | e | p | π+π−p | 1.1 | 1.5 | 1.8 | 1.825 |
E1M194 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 1.1 | 1.5 | 1.8 | 1.825 |
E1M195 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 1.1 | 1.5 | 1.8 | 1.825 |
E1M196 | dσ/dM(π+,π−) | e | p | π+π−p | 1.1 | 1.5 | 1.8 | 1.825 |
E1M197 | dσ/dM(π−,p) | e | p | π+π−p | 1.1 | 1.5 | 1.8 | 1.825 |
E1M198 | dσ/dM(π+,p) | e | p | π+π−p | 1.1 | 1.5 | 1.8 | 1.825 |
E1M199 | dσ/dφ(p) | e | p | π+π−p | 1.1 | 1.5 | 1.8 | 1.825 |
E1M200 | dσ/dφ(π−) | e | p | π+π−p | 1.1 | 1.5 | 1.8 | 1.825 |