Search results
ID | Quantity | Beam | Target | Final state |
Q2min, GeV2 |
Q2max, GeV2 |
Wmin, GeV |
Wmax, GeV |
Spokespersons |
---|---|---|---|---|---|---|---|---|---|
E159M913 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.5 | V. Burkert |
E159M922 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.525 | 1.525 | V. Burkert |
E159M931 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.55 | 1.55 | V. Burkert |
E159M940 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.575 | 1.575 | V. Burkert |
E159M949 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.6 | 1.6 | V. Burkert |
E159M958 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.625 | 1.625 | V. Burkert |
E159M967 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.65 | 1.65 | V. Burkert |
E159M976 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.675 | 1.675 | V. Burkert |
E159M985 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.7 | 1.7 | V. Burkert |
E159M994 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.725 | 1.725 | V. Burkert |
E159M1003 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.75 | 1.75 | V. Burkert |
E159M1012 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.775 | 1.775 | V. Burkert |
E159M1021 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.8 | 1.8 | V. Burkert |
E159M1030 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.825 | 1.825 | V. Burkert |
E159M1039 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.85 | V. Burkert |
E159M1048 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.875 | 1.875 | V. Burkert |
E159M1057 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.9 | V. Burkert |
E159M1066 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.925 | 1.925 | V. Burkert |
E159M1075 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 1.95 | V. Burkert |
E159M1084 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 4.2 | 5.0 | 1.975 | 1.975 | V. Burkert |