Search results
| ID | Quantity | Beam | Target | Final state |
Q2min, GeV2 |
Q2max, GeV2 |
Wmin, GeV |
Wmax, GeV |
Spokespersons |
|---|---|---|---|---|---|---|---|---|---|
| E159M914 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.5 | V. Burkert |
| E159M923 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.525 | 1.525 | V. Burkert |
| E159M932 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.55 | 1.55 | V. Burkert |
| E159M941 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.575 | 1.575 | V. Burkert |
| E159M950 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.6 | 1.6 | V. Burkert |
| E159M959 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.625 | 1.625 | V. Burkert |
| E159M968 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.65 | 1.65 | V. Burkert |
| E159M977 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.675 | 1.675 | V. Burkert |
| E159M986 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.7 | 1.7 | V. Burkert |
| E159M995 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.725 | 1.725 | V. Burkert |
| E159M1004 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.75 | 1.75 | V. Burkert |
| E159M1013 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.775 | 1.775 | V. Burkert |
| E159M1022 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.8 | 1.8 | V. Burkert |
| E159M1031 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.825 | 1.825 | V. Burkert |
| E159M1040 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.85 | V. Burkert |
| E159M1049 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.875 | 1.875 | V. Burkert |
| E159M1058 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.9 | V. Burkert |
| E159M1067 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.925 | 1.925 | V. Burkert |
| E159M1076 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 1.95 | V. Burkert |
| E159M1085 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 4.2 | 5.0 | 1.975 | 1.975 | V. Burkert |