CLAS Physics Database
| ID | Final state | Q2min, GeV2 | Q2max, GeV2 | Wmin, GeV | Wmax, GeV | Quantity | Spokespersons | Title | Year |
|---|
| E216M227 | π+π−p | 2.4 | 3 | 1.95 | 2 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M228 | π+π−p | 2.4 | 3 | 1.95 | 2 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M229 | π+π−p | 2.4 | 3 | 1.95 | 2 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M230 | π+π−p | 2.4 | 3 | 1.95 | 2 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M231 | π+π−p | 2.4 | 3 | 1.95 | 2 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M232 | π+π−p | 2.4 | 3 | 1.95 | 2 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M233 | π+π−p | 2.4 | 3 | 1.95 | 2 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M234 | π+π−p | 2.4 | 3 | 1.95 | 2 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M235 | π+π−p | 2.4 | 3 | 2 | 2.05 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M236 | π+π−p | 2.4 | 3 | 2 | 2.05 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M237 | π+π−p | 2.4 | 3 | 2 | 2.05 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M238 | π+π−p | 2.4 | 3 | 2 | 2.05 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M239 | π+π−p | 2.4 | 3 | 2 | 2.05 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M240 | π+π−p | 2.4 | 3 | 2 | 2.05 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M241 | π+π−p | 2.4 | 3 | 2 | 2.05 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M242 | π+π−p | 2.4 | 3 | 2 | 2.05 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M243 | π+π−p | 2.4 | 3 | 2 | 2.05 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M244 | π+π−p | 2.4 | 3 | 2.05 | 2.1 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M245 | π+π−p | 2.4 | 3 | 2.05 | 2.1 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M246 | π+π−p | 2.4 | 3 | 2.05 | 2.1 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M247 | π+π−p | 2.4 | 3 | 2.05 | 2.1 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M248 | π+π−p | 2.4 | 3 | 2.05 | 2.1 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M249 | π+π−p | 2.4 | 3 | 2.05 | 2.1 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M250 | π+π−p | 2.4 | 3 | 2.05 | 2.1 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M251 | π+π−p | 2.4 | 3 | 2.05 | 2.1 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M252 | π+π−p | 2.4 | 3 | 2.05 | 2.1 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M253 | π+π−p | 3 | 3.5 | 1.4 | 1.45 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M254 | π+π−p | 3 | 3.5 | 1.4 | 1.45 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M255 | π+π−p | 3 | 3.5 | 1.4 | 1.45 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M256 | π+π−p | 3 | 3.5 | 1.4 | 1.45 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M257 | π+π−p | 3 | 3.5 | 1.4 | 1.45 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M258 | π+π−p | 3 | 3.5 | 1.4 | 1.45 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M259 | π+π−p | 3 | 3.5 | 1.4 | 1.45 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M260 | π+π−p | 3 | 3.5 | 1.4 | 1.45 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M261 | π+π−p | 3 | 3.5 | 1.4 | 1.45 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M262 | π+π−p | 3 | 3.5 | 1.45 | 1.5 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M263 | π+π−p | 3 | 3.5 | 1.45 | 1.5 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M264 | π+π−p | 3 | 3.5 | 1.45 | 1.5 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M265 | π+π−p | 3 | 3.5 | 1.45 | 1.5 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M266 | π+π−p | 3 | 3.5 | 1.45 | 1.5 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M267 | π+π−p | 3 | 3.5 | 1.45 | 1.5 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M268 | π+π−p | 3 | 3.5 | 1.45 | 1.5 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M269 | π+π−p | 3 | 3.5 | 1.45 | 1.5 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M270 | π+π−p | 3 | 3.5 | 1.45 | 1.5 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M271 | π+π−p | 3 | 3.5 | 1.5 | 1.55 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M272 | π+π−p | 3 | 3.5 | 1.5 | 1.55 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M273 | π+π−p | 3 | 3.5 | 1.5 | 1.55 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M274 | π+π−p | 3 | 3.5 | 1.5 | 1.55 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M275 | π+π−p | 3 | 3.5 | 1.5 | 1.55 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M276 | π+π−p | 3 | 3.5 | 1.5 | 1.55 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M277 | π+π−p | 3 | 3.5 | 1.5 | 1.55 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M278 | π+π−p | 3 | 3.5 | 1.5 | 1.55 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M279 | π+π−p | 3 | 3.5 | 1.5 | 1.55 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M280 | π+π−p | 3 | 3.5 | 1.55 | 1.6 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M281 | π+π−p | 3 | 3.5 | 1.55 | 1.6 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M282 | π+π−p | 3 | 3.5 | 1.55 | 1.6 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M283 | π+π−p | 3 | 3.5 | 1.55 | 1.6 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M284 | π+π−p | 3 | 3.5 | 1.55 | 1.6 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M285 | π+π−p | 3 | 3.5 | 1.55 | 1.6 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M286 | π+π−p | 3 | 3.5 | 1.55 | 1.6 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M287 | π+π−p | 3 | 3.5 | 1.55 | 1.6 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M288 | π+π−p | 3 | 3.5 | 1.55 | 1.6 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M289 | π+π−p | 3 | 3.5 | 1.6 | 1.65 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M290 | π+π−p | 3 | 3.5 | 1.6 | 1.65 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M291 | π+π−p | 3 | 3.5 | 1.6 | 1.65 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M292 | π+π−p | 3 | 3.5 | 1.6 | 1.65 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M293 | π+π−p | 3 | 3.5 | 1.6 | 1.65 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M294 | π+π−p | 3 | 3.5 | 1.6 | 1.65 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M295 | π+π−p | 3 | 3.5 | 1.6 | 1.65 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M296 | π+π−p | 3 | 3.5 | 1.6 | 1.65 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M297 | π+π−p | 3 | 3.5 | 1.6 | 1.65 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M298 | π+π−p | 3 | 3.5 | 1.65 | 1.7 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M299 | π+π−p | 3 | 3.5 | 1.65 | 1.7 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M300 | π+π−p | 3 | 3.5 | 1.65 | 1.7 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M301 | π+π−p | 3 | 3.5 | 1.65 | 1.7 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M302 | π+π−p | 3 | 3.5 | 1.65 | 1.7 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M303 | π+π−p | 3 | 3.5 | 1.65 | 1.7 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M304 | π+π−p | 3 | 3.5 | 1.65 | 1.7 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M305 | π+π−p | 3 | 3.5 | 1.65 | 1.7 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M306 | π+π−p | 3 | 3.5 | 1.65 | 1.7 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M307 | π+π−p | 3 | 3.5 | 1.7 | 1.75 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M308 | π+π−p | 3 | 3.5 | 1.7 | 1.75 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M309 | π+π−p | 3 | 3.5 | 1.7 | 1.75 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M310 | π+π−p | 3 | 3.5 | 1.7 | 1.75 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M311 | π+π−p | 3 | 3.5 | 1.7 | 1.75 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M312 | π+π−p | 3 | 3.5 | 1.7 | 1.75 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M313 | π+π−p | 3 | 3.5 | 1.7 | 1.75 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M314 | π+π−p | 3 | 3.5 | 1.7 | 1.75 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M315 | π+π−p | 3 | 3.5 | 1.7 | 1.75 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M316 | π+π−p | 3 | 3.5 | 1.75 | 1.8 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M317 | π+π−p | 3 | 3.5 | 1.75 | 1.8 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M318 | π+π−p | 3 | 3.5 | 1.75 | 1.8 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M319 | π+π−p | 3 | 3.5 | 1.75 | 1.8 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M320 | π+π−p | 3 | 3.5 | 1.75 | 1.8 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M321 | π+π−p | 3 | 3.5 | 1.75 | 1.8 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M322 | π+π−p | 3 | 3.5 | 1.75 | 1.8 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M323 | π+π−p | 3 | 3.5 | 1.75 | 1.8 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M324 | π+π−p | 3 | 3.5 | 1.75 | 1.8 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M325 | π+π−p | 3 | 3.5 | 1.8 | 1.85 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M326 | π+π−p | 3 | 3.5 | 1.8 | 1.85 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |