CLAS12 Run Group A
- Spokesperson
- Krishna Chandra
- Year
- 2018
- 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/dψ(π−) dσ/dψ(π+) dσ/dψ(p)
Measurements
| ID | Quantity | Beam | Target | Final state |
Q2min, GeV2 |
Q2max, GeV2 |
Wmin, GeV |
Wmax, GeV |
|---|---|---|---|---|---|---|---|---|
| E216M127 | dσ/dM(π−,p) | e | p | π+π−p | 2.4 | 3.0 | 1.4 | 1.45 |
| E216M128 | dσ/dM(π+,π−) | e | p | π+π−p | 2.4 | 3.0 | 1.4 | 1.45 |
| E216M129 | dσ/dM(π+,p) | e | p | π+π−p | 2.4 | 3.0 | 1.4 | 1.45 |
| E216M130 | dσ/dψ(π−) | e | p | π+π−p | 2.4 | 3.0 | 1.4 | 1.45 |
| E216M131 | dσ/dψ(π+) | e | p | π+π−p | 2.4 | 3.0 | 1.4 | 1.45 |
| E216M132 | dσ/dψ(p) | e | p | π+π−p | 2.4 | 3.0 | 1.4 | 1.45 |
| E216M133 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 2.4 | 3.0 | 1.4 | 1.45 |
| E216M134 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 2.4 | 3.0 | 1.4 | 1.45 |
| E216M135 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 2.4 | 3.0 | 1.4 | 1.45 |
| E216M136 | dσ/dM(π−,p) | e | p | π+π−p | 2.4 | 3.0 | 1.45 | 1.5 |
| E216M137 | dσ/dM(π+,π−) | e | p | π+π−p | 2.4 | 3.0 | 1.45 | 1.5 |
| E216M138 | dσ/dM(π+,p) | e | p | π+π−p | 2.4 | 3.0 | 1.45 | 1.5 |
| E216M139 | dσ/dψ(π−) | e | p | π+π−p | 2.4 | 3.0 | 1.45 | 1.5 |
| E216M140 | dσ/dψ(π+) | e | p | π+π−p | 2.4 | 3.0 | 1.45 | 1.5 |
| E216M141 | dσ/dψ(p) | e | p | π+π−p | 2.4 | 3.0 | 1.45 | 1.5 |
| E216M142 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 2.4 | 3.0 | 1.45 | 1.5 |
| E216M143 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 2.4 | 3.0 | 1.45 | 1.5 |
| E216M144 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 2.4 | 3.0 | 1.45 | 1.5 |
| E216M145 | dσ/dM(π−,p) | e | p | π+π−p | 2.4 | 3.0 | 1.5 | 1.55 |
| E216M146 | dσ/dM(π+,π−) | e | p | π+π−p | 2.4 | 3.0 | 1.5 | 1.55 |
| E216M147 | dσ/dM(π+,p) | e | p | π+π−p | 2.4 | 3.0 | 1.5 | 1.55 |
| E216M148 | dσ/dψ(π−) | e | p | π+π−p | 2.4 | 3.0 | 1.5 | 1.55 |
| E216M149 | dσ/dψ(π+) | e | p | π+π−p | 2.4 | 3.0 | 1.5 | 1.55 |
| E216M150 | dσ/dψ(p) | e | p | π+π−p | 2.4 | 3.0 | 1.5 | 1.55 |
| E216M151 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 2.4 | 3.0 | 1.5 | 1.55 |
| E216M152 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 2.4 | 3.0 | 1.5 | 1.55 |
| E216M153 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 2.4 | 3.0 | 1.5 | 1.55 |
| E216M154 | dσ/dM(π−,p) | e | p | π+π−p | 2.4 | 3.0 | 1.55 | 1.6 |
| E216M155 | dσ/dM(π+,π−) | e | p | π+π−p | 2.4 | 3.0 | 1.55 | 1.6 |
| E216M156 | dσ/dM(π+,p) | e | p | π+π−p | 2.4 | 3.0 | 1.55 | 1.6 |
| E216M157 | dσ/dψ(π−) | e | p | π+π−p | 2.4 | 3.0 | 1.55 | 1.6 |
| E216M158 | dσ/dψ(π+) | e | p | π+π−p | 2.4 | 3.0 | 1.55 | 1.6 |
| E216M159 | dσ/dψ(p) | e | p | π+π−p | 2.4 | 3.0 | 1.55 | 1.6 |
| E216M160 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 2.4 | 3.0 | 1.55 | 1.6 |
| E216M161 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 2.4 | 3.0 | 1.55 | 1.6 |
| E216M162 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 2.4 | 3.0 | 1.55 | 1.6 |
| E216M163 | dσ/dM(π−,p) | e | p | π+π−p | 2.4 | 3.0 | 1.6 | 1.65 |
| E216M164 | dσ/dM(π+,π−) | e | p | π+π−p | 2.4 | 3.0 | 1.6 | 1.65 |
| E216M165 | dσ/dM(π+,p) | e | p | π+π−p | 2.4 | 3.0 | 1.6 | 1.65 |
| E216M166 | dσ/dψ(π−) | e | p | π+π−p | 2.4 | 3.0 | 1.6 | 1.65 |
| E216M167 | dσ/dψ(π+) | e | p | π+π−p | 2.4 | 3.0 | 1.6 | 1.65 |
| E216M168 | dσ/dψ(p) | e | p | π+π−p | 2.4 | 3.0 | 1.6 | 1.65 |
| E216M169 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 2.4 | 3.0 | 1.6 | 1.65 |
| E216M170 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 2.4 | 3.0 | 1.6 | 1.65 |
| E216M171 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 2.4 | 3.0 | 1.6 | 1.65 |
| E216M172 | dσ/dM(π−,p) | e | p | π+π−p | 2.4 | 3.0 | 1.65 | 1.7 |
| E216M173 | dσ/dM(π+,π−) | e | p | π+π−p | 2.4 | 3.0 | 1.65 | 1.7 |
| E216M174 | dσ/dM(π+,p) | e | p | π+π−p | 2.4 | 3.0 | 1.65 | 1.7 |
| E216M175 | dσ/dψ(π−) | e | p | π+π−p | 2.4 | 3.0 | 1.65 | 1.7 |
| E216M176 | dσ/dψ(π+) | e | p | π+π−p | 2.4 | 3.0 | 1.65 | 1.7 |
| E216M177 | dσ/dψ(p) | e | p | π+π−p | 2.4 | 3.0 | 1.65 | 1.7 |
| E216M178 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 2.4 | 3.0 | 1.65 | 1.7 |
| E216M179 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 2.4 | 3.0 | 1.65 | 1.7 |
| E216M180 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 2.4 | 3.0 | 1.65 | 1.7 |
| E216M181 | dσ/dM(π−,p) | e | p | π+π−p | 2.4 | 3.0 | 1.7 | 1.75 |
| E216M182 | dσ/dM(π+,π−) | e | p | π+π−p | 2.4 | 3.0 | 1.7 | 1.75 |
| E216M183 | dσ/dM(π+,p) | e | p | π+π−p | 2.4 | 3.0 | 1.7 | 1.75 |
| E216M184 | dσ/dψ(π−) | e | p | π+π−p | 2.4 | 3.0 | 1.7 | 1.75 |
| E216M185 | dσ/dψ(π+) | e | p | π+π−p | 2.4 | 3.0 | 1.7 | 1.75 |
| E216M186 | dσ/dψ(p) | e | p | π+π−p | 2.4 | 3.0 | 1.7 | 1.75 |
| E216M187 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 2.4 | 3.0 | 1.7 | 1.75 |
| E216M188 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 2.4 | 3.0 | 1.7 | 1.75 |
| E216M189 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 2.4 | 3.0 | 1.7 | 1.75 |
| E216M190 | dσ/dM(π−,p) | e | p | π+π−p | 2.4 | 3.0 | 1.75 | 1.8 |
| E216M191 | dσ/dM(π+,π−) | e | p | π+π−p | 2.4 | 3.0 | 1.75 | 1.8 |
| E216M192 | dσ/dM(π+,p) | e | p | π+π−p | 2.4 | 3.0 | 1.75 | 1.8 |
| E216M193 | dσ/dψ(π−) | e | p | π+π−p | 2.4 | 3.0 | 1.75 | 1.8 |
| E216M194 | dσ/dψ(π+) | e | p | π+π−p | 2.4 | 3.0 | 1.75 | 1.8 |
| E216M195 | dσ/dψ(p) | e | p | π+π−p | 2.4 | 3.0 | 1.75 | 1.8 |
| E216M196 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 2.4 | 3.0 | 1.75 | 1.8 |
| E216M197 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 2.4 | 3.0 | 1.75 | 1.8 |
| E216M198 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 2.4 | 3.0 | 1.75 | 1.8 |
| E216M199 | dσ/dM(π−,p) | e | p | π+π−p | 2.4 | 3.0 | 1.8 | 1.85 |
| E216M200 | dσ/dM(π+,π−) | e | p | π+π−p | 2.4 | 3.0 | 1.8 | 1.85 |
| E216M201 | dσ/dM(π+,p) | e | p | π+π−p | 2.4 | 3.0 | 1.8 | 1.85 |
| E216M202 | dσ/dψ(π−) | e | p | π+π−p | 2.4 | 3.0 | 1.8 | 1.85 |
| E216M203 | dσ/dψ(π+) | e | p | π+π−p | 2.4 | 3.0 | 1.8 | 1.85 |
| E216M204 | dσ/dψ(p) | e | p | π+π−p | 2.4 | 3.0 | 1.8 | 1.85 |
| E216M205 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 2.4 | 3.0 | 1.8 | 1.85 |
| E216M206 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 2.4 | 3.0 | 1.8 | 1.85 |
| E216M207 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 2.4 | 3.0 | 1.8 | 1.85 |
| E216M208 | dσ/dM(π−,p) | e | p | π+π−p | 2.4 | 3.0 | 1.85 | 1.9 |
| E216M209 | dσ/dM(π+,π−) | e | p | π+π−p | 2.4 | 3.0 | 1.85 | 1.9 |
| E216M210 | dσ/dM(π+,p) | e | p | π+π−p | 2.4 | 3.0 | 1.85 | 1.9 |
| E216M211 | dσ/dψ(π−) | e | p | π+π−p | 2.4 | 3.0 | 1.85 | 1.9 |
| E216M212 | dσ/dψ(π+) | e | p | π+π−p | 2.4 | 3.0 | 1.85 | 1.9 |
| E216M213 | dσ/dψ(p) | e | p | π+π−p | 2.4 | 3.0 | 1.85 | 1.9 |
| E216M214 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 2.4 | 3.0 | 1.85 | 1.9 |
| E216M215 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 2.4 | 3.0 | 1.85 | 1.9 |
| E216M216 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 2.4 | 3.0 | 1.85 | 1.9 |
| E216M217 | dσ/dM(π−,p) | e | p | π+π−p | 2.4 | 3.0 | 1.9 | 1.95 |
| E216M218 | dσ/dM(π+,π−) | e | p | π+π−p | 2.4 | 3.0 | 1.9 | 1.95 |
| E216M219 | dσ/dM(π+,p) | e | p | π+π−p | 2.4 | 3.0 | 1.9 | 1.95 |
| E216M220 | dσ/dψ(π−) | e | p | π+π−p | 2.4 | 3.0 | 1.9 | 1.95 |
| E216M221 | dσ/dψ(π+) | e | p | π+π−p | 2.4 | 3.0 | 1.9 | 1.95 |
| E216M222 | dσ/dψ(p) | e | p | π+π−p | 2.4 | 3.0 | 1.9 | 1.95 |
| E216M223 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 2.4 | 3.0 | 1.9 | 1.95 |
| E216M224 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 2.4 | 3.0 | 1.9 | 1.95 |
| E216M225 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 2.4 | 3.0 | 1.9 | 1.95 |
| E216M226 | dσ/dM(π−,p) | e | p | π+π−p | 2.4 | 3.0 | 1.95 | 2.0 |