Search results
ID | Quantity | Beam | Target | Final state |
Q2min, GeV2 |
Q2max, GeV2 |
Wmin, GeV |
Wmax, GeV |
Spokespersons |
---|---|---|---|---|---|---|---|---|---|
E159M911 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.5 | 1.5 | V. Burkert |
E159M920 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.525 | 1.525 | V. Burkert |
E159M929 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.55 | 1.55 | V. Burkert |
E159M938 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.575 | 1.575 | V. Burkert |
E159M947 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.6 | 1.6 | V. Burkert |
E159M956 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.625 | 1.625 | V. Burkert |
E159M965 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.65 | 1.65 | V. Burkert |
E159M974 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.675 | 1.675 | V. Burkert |
E159M983 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.7 | 1.7 | V. Burkert |
E159M992 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.725 | 1.725 | V. Burkert |
E159M1001 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.75 | 1.75 | V. Burkert |
E159M1010 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.775 | 1.775 | V. Burkert |
E159M1019 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.8 | 1.8 | V. Burkert |
E159M1028 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.825 | 1.825 | V. Burkert |
E159M1037 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.85 | 1.85 | V. Burkert |
E159M1046 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.875 | 1.875 | V. Burkert |
E159M1055 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.9 | 1.9 | V. Burkert |
E159M1064 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.925 | 1.925 | V. Burkert |
E159M1073 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.95 | 1.95 | V. Burkert |
E159M1082 | dσ/dψ(p) | e | p | π+π−p | 4.2 | 5.0 | 1.975 | 1.975 | V. Burkert |