CLAS Physics Database
| ID | Final state | Q2min, GeV2 | Q2max, GeV2 | Wmin, GeV | Wmax, GeV | Quantity | Spokespersons | Title | Year |
|---|
| E216M927 | π+π−p | 7 | 8 | 1.6 | 1.65 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M928 | π+π−p | 7 | 8 | 1.65 | 1.7 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M929 | π+π−p | 7 | 8 | 1.65 | 1.7 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M930 | π+π−p | 7 | 8 | 1.65 | 1.7 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M931 | π+π−p | 7 | 8 | 1.65 | 1.7 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M932 | π+π−p | 7 | 8 | 1.65 | 1.7 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M933 | π+π−p | 7 | 8 | 1.65 | 1.7 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M934 | π+π−p | 7 | 8 | 1.65 | 1.7 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M935 | π+π−p | 7 | 8 | 1.65 | 1.7 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M936 | π+π−p | 7 | 8 | 1.65 | 1.7 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M937 | π+π−p | 7 | 8 | 1.7 | 1.75 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M938 | π+π−p | 7 | 8 | 1.7 | 1.75 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M939 | π+π−p | 7 | 8 | 1.7 | 1.75 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M940 | π+π−p | 7 | 8 | 1.7 | 1.75 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M941 | π+π−p | 7 | 8 | 1.7 | 1.75 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M942 | π+π−p | 7 | 8 | 1.7 | 1.75 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M943 | π+π−p | 7 | 8 | 1.7 | 1.75 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M944 | π+π−p | 7 | 8 | 1.7 | 1.75 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M945 | π+π−p | 7 | 8 | 1.7 | 1.75 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M946 | π+π−p | 7 | 8 | 1.75 | 1.8 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M947 | π+π−p | 7 | 8 | 1.75 | 1.8 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M948 | π+π−p | 7 | 8 | 1.75 | 1.8 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M949 | π+π−p | 7 | 8 | 1.75 | 1.8 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M950 | π+π−p | 7 | 8 | 1.75 | 1.8 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M951 | π+π−p | 7 | 8 | 1.75 | 1.8 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M952 | π+π−p | 7 | 8 | 1.75 | 1.8 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M953 | π+π−p | 7 | 8 | 1.75 | 1.8 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M954 | π+π−p | 7 | 8 | 1.75 | 1.8 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M955 | π+π−p | 7 | 8 | 1.8 | 1.85 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M956 | π+π−p | 7 | 8 | 1.8 | 1.85 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M957 | π+π−p | 7 | 8 | 1.8 | 1.85 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M958 | π+π−p | 7 | 8 | 1.8 | 1.85 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M959 | π+π−p | 7 | 8 | 1.8 | 1.85 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M960 | π+π−p | 7 | 8 | 1.8 | 1.85 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M961 | π+π−p | 7 | 8 | 1.8 | 1.85 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M962 | π+π−p | 7 | 8 | 1.8 | 1.85 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M963 | π+π−p | 7 | 8 | 1.8 | 1.85 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M964 | π+π−p | 7 | 8 | 1.85 | 1.9 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M965 | π+π−p | 7 | 8 | 1.85 | 1.9 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M966 | π+π−p | 7 | 8 | 1.85 | 1.9 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M967 | π+π−p | 7 | 8 | 1.85 | 1.9 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M968 | π+π−p | 7 | 8 | 1.85 | 1.9 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M969 | π+π−p | 7 | 8 | 1.85 | 1.9 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M970 | π+π−p | 7 | 8 | 1.85 | 1.9 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M971 | π+π−p | 7 | 8 | 1.85 | 1.9 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M972 | π+π−p | 7 | 8 | 1.85 | 1.9 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M973 | π+π−p | 7 | 8 | 1.9 | 1.95 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M974 | π+π−p | 7 | 8 | 1.9 | 1.95 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M975 | π+π−p | 7 | 8 | 1.9 | 1.95 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M976 | π+π−p | 7 | 8 | 1.9 | 1.95 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M977 | π+π−p | 7 | 8 | 1.9 | 1.95 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M978 | π+π−p | 7 | 8 | 1.9 | 1.95 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M979 | π+π−p | 7 | 8 | 1.9 | 1.95 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M980 | π+π−p | 7 | 8 | 1.9 | 1.95 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M981 | π+π−p | 7 | 8 | 1.9 | 1.95 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M982 | π+π−p | 7 | 8 | 1.95 | 2 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M983 | π+π−p | 7 | 8 | 1.95 | 2 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M984 | π+π−p | 7 | 8 | 1.95 | 2 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M985 | π+π−p | 7 | 8 | 1.95 | 2 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M986 | π+π−p | 7 | 8 | 1.95 | 2 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M987 | π+π−p | 7 | 8 | 1.95 | 2 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M988 | π+π−p | 7 | 8 | 1.95 | 2 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M989 | π+π−p | 7 | 8 | 1.95 | 2 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M990 | π+π−p | 7 | 8 | 1.95 | 2 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M991 | π+π−p | 7 | 8 | 2 | 2.05 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M992 | π+π−p | 7 | 8 | 2 | 2.05 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M993 | π+π−p | 7 | 8 | 2 | 2.05 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M994 | π+π−p | 7 | 8 | 2 | 2.05 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M995 | π+π−p | 7 | 8 | 2 | 2.05 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M996 | π+π−p | 7 | 8 | 2 | 2.05 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M997 | π+π−p | 7 | 8 | 2 | 2.05 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M998 | π+π−p | 7 | 8 | 2 | 2.05 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M999 | π+π−p | 7 | 8 | 2 | 2.05 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M1000 | π+π−p | 7 | 8 | 2.05 | 2.1 | dσ/dM(π−,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M1001 | π+π−p | 7 | 8 | 2.05 | 2.1 | dσ/dM(π+,π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M1002 | π+π−p | 7 | 8 | 2.05 | 2.1 | dσ/dM(π+,p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M1003 | π+π−p | 7 | 8 | 2.05 | 2.1 | dσ/dψ(π−) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M1004 | π+π−p | 7 | 8 | 2.05 | 2.1 | dσ/dψ(π+) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M1005 | π+π−p | 7 | 8 | 2.05 | 2.1 | dσ/dψ(p) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M1006 | π+π−p | 7 | 8 | 2.05 | 2.1 | dσ/d(−cos(θ(π−))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M1007 | π+π−p | 7 | 8 | 2.05 | 2.1 | dσ/d(−cos(θ(π+))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M1008 | π+π−p | 7 | 8 | 2.05 | 2.1 | dσ/d(−cos(θ(p))) | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M1010 | π+π−p | 2.4 | 3 | | | σ | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M1011 | π+π−p | 3 | 3.5 | | | σ | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M1012 | π+π−p | 3.5 | 4.2 | | | σ | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M1013 | π+π−p | 4.2 | 5 | | | σ | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M1014 | π+π−p | 5 | 6 | | | σ | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M1015 | π+π−p | 6 | 7 | | | σ | Krishna Chandra | CLAS12 Run Group A | 2018 |
| E216M1016 | π+π−p | 7 | 8 | | | σ | Krishna Chandra | CLAS12 Run Group A | 2018 |