Search results
ID | Quantity | Beam | Target | Final state |
Q2min, GeV2 |
Q2max, GeV2 |
Wmin, GeV |
Wmax, GeV |
Spokespersons |
---|---|---|---|---|---|---|---|---|---|
E159M908 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.5 | V. Burkert |
E159M917 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.525 | 1.525 | V. Burkert |
E159M926 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.55 | 1.55 | V. Burkert |
E159M935 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.575 | 1.575 | V. Burkert |
E159M944 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.6 | 1.6 | V. Burkert |
E159M953 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.625 | 1.625 | V. Burkert |
E159M962 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.65 | 1.65 | V. Burkert |
E159M971 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.675 | 1.675 | V. Burkert |
E159M980 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.7 | 1.7 | V. Burkert |
E159M989 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.725 | 1.725 | V. Burkert |
E159M998 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.75 | 1.75 | V. Burkert |
E159M1007 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.775 | 1.775 | V. Burkert |
E159M1016 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.8 | 1.8 | V. Burkert |
E159M1025 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.825 | 1.825 | V. Burkert |
E159M1034 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.85 | V. Burkert |
E159M1043 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.875 | 1.875 | V. Burkert |
E159M1052 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.9 | V. Burkert |
E159M1061 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.925 | 1.925 | V. Burkert |
E159M1070 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 1.95 | V. Burkert |
E159M1079 | dσ/dM(π+,p) | e | p | π+π−p | 4.2 | 5.0 | 1.975 | 1.975 | V. Burkert |