Search results
ID | Quantity | Beam | Target | Final state |
Q2min, GeV2 |
Q2max, GeV2 |
Wmin, GeV |
Wmax, GeV |
Spokespersons |
---|---|---|---|---|---|---|---|---|---|
E159M906 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.5 | V. Burkert |
E159M915 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.525 | 1.525 | V. Burkert |
E159M924 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.55 | 1.55 | V. Burkert |
E159M933 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.575 | 1.575 | V. Burkert |
E159M942 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.6 | 1.6 | V. Burkert |
E159M951 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.625 | 1.625 | V. Burkert |
E159M960 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.65 | 1.65 | V. Burkert |
E159M969 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.675 | 1.675 | V. Burkert |
E159M978 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.7 | 1.7 | V. Burkert |
E159M987 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.725 | 1.725 | V. Burkert |
E159M996 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.75 | 1.75 | V. Burkert |
E159M1005 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.775 | 1.775 | V. Burkert |
E159M1014 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.8 | 1.8 | V. Burkert |
E159M1023 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.825 | 1.825 | V. Burkert |
E159M1032 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.85 | V. Burkert |
E159M1041 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.875 | 1.875 | V. Burkert |
E159M1050 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.9 | V. Burkert |
E159M1059 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.925 | 1.925 | V. Burkert |
E159M1068 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 1.95 | V. Burkert |
E159M1077 | dσ/dM(π−,p) | e | p | π+π−p | 4.2 | 5.0 | 1.975 | 1.975 | V. Burkert |