CLAS Physics Database
| ID | Final state | Q2min, GeV2 | Q2max, GeV2 | Wmin, GeV | Wmax, GeV | Quantity | Spokespersons | Title | Year |
| E216M127 | π+π−p | 2.4 | 3 | 1.4 | 1.45 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M128 | π+π−p | 2.4 | 3 | 1.4 | 1.45 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M129 | π+π−p | 2.4 | 3 | 1.4 | 1.45 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M130 | π+π−p | 2.4 | 3 | 1.4 | 1.45 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M131 | π+π−p | 2.4 | 3 | 1.4 | 1.45 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M132 | π+π−p | 2.4 | 3 | 1.4 | 1.45 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M133 | π+π−p | 2.4 | 3 | 1.4 | 1.45 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M134 | π+π−p | 2.4 | 3 | 1.4 | 1.45 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M135 | π+π−p | 2.4 | 3 | 1.4 | 1.45 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M136 | π+π−p | 2.4 | 3 | 1.45 | 1.5 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M137 | π+π−p | 2.4 | 3 | 1.45 | 1.5 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M138 | π+π−p | 2.4 | 3 | 1.45 | 1.5 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M139 | π+π−p | 2.4 | 3 | 1.45 | 1.5 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M140 | π+π−p | 2.4 | 3 | 1.45 | 1.5 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M141 | π+π−p | 2.4 | 3 | 1.45 | 1.5 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M142 | π+π−p | 2.4 | 3 | 1.45 | 1.5 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M143 | π+π−p | 2.4 | 3 | 1.45 | 1.5 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M144 | π+π−p | 2.4 | 3 | 1.45 | 1.5 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M145 | π+π−p | 2.4 | 3 | 1.5 | 1.55 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M146 | π+π−p | 2.4 | 3 | 1.5 | 1.55 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M147 | π+π−p | 2.4 | 3 | 1.5 | 1.55 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M148 | π+π−p | 2.4 | 3 | 1.5 | 1.55 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M149 | π+π−p | 2.4 | 3 | 1.5 | 1.55 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M150 | π+π−p | 2.4 | 3 | 1.5 | 1.55 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M151 | π+π−p | 2.4 | 3 | 1.5 | 1.55 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M152 | π+π−p | 2.4 | 3 | 1.5 | 1.55 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M153 | π+π−p | 2.4 | 3 | 1.5 | 1.55 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M154 | π+π−p | 2.4 | 3 | 1.55 | 1.6 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M155 | π+π−p | 2.4 | 3 | 1.55 | 1.6 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M156 | π+π−p | 2.4 | 3 | 1.55 | 1.6 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M157 | π+π−p | 2.4 | 3 | 1.55 | 1.6 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M158 | π+π−p | 2.4 | 3 | 1.55 | 1.6 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M159 | π+π−p | 2.4 | 3 | 1.55 | 1.6 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M160 | π+π−p | 2.4 | 3 | 1.55 | 1.6 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M161 | π+π−p | 2.4 | 3 | 1.55 | 1.6 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M162 | π+π−p | 2.4 | 3 | 1.55 | 1.6 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M163 | π+π−p | 2.4 | 3 | 1.6 | 1.65 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M164 | π+π−p | 2.4 | 3 | 1.6 | 1.65 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M165 | π+π−p | 2.4 | 3 | 1.6 | 1.65 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M166 | π+π−p | 2.4 | 3 | 1.6 | 1.65 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M167 | π+π−p | 2.4 | 3 | 1.6 | 1.65 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M168 | π+π−p | 2.4 | 3 | 1.6 | 1.65 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M169 | π+π−p | 2.4 | 3 | 1.6 | 1.65 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M170 | π+π−p | 2.4 | 3 | 1.6 | 1.65 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M171 | π+π−p | 2.4 | 3 | 1.6 | 1.65 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M172 | π+π−p | 2.4 | 3 | 1.65 | 1.7 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M173 | π+π−p | 2.4 | 3 | 1.65 | 1.7 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M174 | π+π−p | 2.4 | 3 | 1.65 | 1.7 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M175 | π+π−p | 2.4 | 3 | 1.65 | 1.7 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M176 | π+π−p | 2.4 | 3 | 1.65 | 1.7 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M177 | π+π−p | 2.4 | 3 | 1.65 | 1.7 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M178 | π+π−p | 2.4 | 3 | 1.65 | 1.7 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M179 | π+π−p | 2.4 | 3 | 1.65 | 1.7 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M180 | π+π−p | 2.4 | 3 | 1.65 | 1.7 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M181 | π+π−p | 2.4 | 3 | 1.7 | 1.75 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M182 | π+π−p | 2.4 | 3 | 1.7 | 1.75 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M183 | π+π−p | 2.4 | 3 | 1.7 | 1.75 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M184 | π+π−p | 2.4 | 3 | 1.7 | 1.75 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M185 | π+π−p | 2.4 | 3 | 1.7 | 1.75 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M186 | π+π−p | 2.4 | 3 | 1.7 | 1.75 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M187 | π+π−p | 2.4 | 3 | 1.7 | 1.75 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M188 | π+π−p | 2.4 | 3 | 1.7 | 1.75 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M189 | π+π−p | 2.4 | 3 | 1.7 | 1.75 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M190 | π+π−p | 2.4 | 3 | 1.75 | 1.8 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M191 | π+π−p | 2.4 | 3 | 1.75 | 1.8 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M192 | π+π−p | 2.4 | 3 | 1.75 | 1.8 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M193 | π+π−p | 2.4 | 3 | 1.75 | 1.8 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M194 | π+π−p | 2.4 | 3 | 1.75 | 1.8 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M195 | π+π−p | 2.4 | 3 | 1.75 | 1.8 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M196 | π+π−p | 2.4 | 3 | 1.75 | 1.8 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M197 | π+π−p | 2.4 | 3 | 1.75 | 1.8 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M198 | π+π−p | 2.4 | 3 | 1.75 | 1.8 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M199 | π+π−p | 2.4 | 3 | 1.8 | 1.85 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M200 | π+π−p | 2.4 | 3 | 1.8 | 1.85 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M201 | π+π−p | 2.4 | 3 | 1.8 | 1.85 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M202 | π+π−p | 2.4 | 3 | 1.8 | 1.85 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M203 | π+π−p | 2.4 | 3 | 1.8 | 1.85 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M204 | π+π−p | 2.4 | 3 | 1.8 | 1.85 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M205 | π+π−p | 2.4 | 3 | 1.8 | 1.85 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M206 | π+π−p | 2.4 | 3 | 1.8 | 1.85 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M207 | π+π−p | 2.4 | 3 | 1.8 | 1.85 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M208 | π+π−p | 2.4 | 3 | 1.85 | 1.9 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M209 | π+π−p | 2.4 | 3 | 1.85 | 1.9 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M210 | π+π−p | 2.4 | 3 | 1.85 | 1.9 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M211 | π+π−p | 2.4 | 3 | 1.85 | 1.9 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M212 | π+π−p | 2.4 | 3 | 1.85 | 1.9 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M213 | π+π−p | 2.4 | 3 | 1.85 | 1.9 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M214 | π+π−p | 2.4 | 3 | 1.85 | 1.9 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M215 | π+π−p | 2.4 | 3 | 1.85 | 1.9 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M216 | π+π−p | 2.4 | 3 | 1.85 | 1.9 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M217 | π+π−p | 2.4 | 3 | 1.9 | 1.95 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M218 | π+π−p | 2.4 | 3 | 1.9 | 1.95 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M219 | π+π−p | 2.4 | 3 | 1.9 | 1.95 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M220 | π+π−p | 2.4 | 3 | 1.9 | 1.95 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M221 | π+π−p | 2.4 | 3 | 1.9 | 1.95 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M222 | π+π−p | 2.4 | 3 | 1.9 | 1.95 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M223 | π+π−p | 2.4 | 3 | 1.9 | 1.95 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M224 | π+π−p | 2.4 | 3 | 1.9 | 1.95 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M225 | π+π−p | 2.4 | 3 | 1.9 | 1.95 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M226 | π+π−p | 2.4 | 3 | 1.95 | 2 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |