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ID | Quantity | Beam | Target | Final state |
Q2min, GeV2 |
Q2max, GeV2 |
Wmin, GeV |
Wmax, GeV |
Spokespersons |
---|---|---|---|---|---|---|---|---|---|
E50M1 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 1.144 | 4.232 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M2 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 1.144 | 1.161 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M3 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 1.373 | 1.385 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M4 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 1.48 | 1.483 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M5 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 1.603 | 1.613 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M6 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 1.74 | 1.753 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M7 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 1.865 | 1.876 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M8 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 1.948 | 1.957 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M9 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 2.094 | 2.106 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M10 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 2.202 | 2.219 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M11 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 2.222 | 2.248 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M12 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 2.329 | 2.346 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M13 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 2.583 | 2.593 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M14 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 2.705 | 2.722 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M15 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 2.726 | 2.754 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M16 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 3.114 | 3.13 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M17 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 3.213 | 3.232 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M18 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 3.282 | 3.296 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M19 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 3.582 | 3.685 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M20 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 3.741 | 3.759 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M21 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 4.179 | 4.188 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
E50M22 | d4σ/dQ2 dxb dt dφ | e | p | π0p | 4.221 | 4.232 | None | None | V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan |
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