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Experiment: e1-dvcs run CLAS data, 2012
Spokespersons: V. Burket, L. Elouadrhiri, M. Garson, S. Stepanyan
Publication:
Quantity measured: d4σ/dQ2 dxb dt dφ, nb/(rad*GeV^4)
Four folded differential cross section.
Beam: e, polarization: polarized
Target: p (Z=1, A=1), polarization: none
Final state: π0p, polarization: none
Q2 : | 2.583 — 2.593 GeV2 |
---|---|
xb : | 0.2887 — 0.2901 |
Select data slice:
-t = GeV^2 |
Observable quantity measured (Y axis): d4σ/dQ2 dxb dt dφ, nb/(rad*GeV^4)
Parameter (X axis): φ, degrees |
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Measured data:
-t,
GeV^2 |
φ,
degrees |
d4σ/dQ2 dxb dt dφ,
nb/(rad*GeV^4) |
Data errors,
nb/(rad*GeV^4) |
Systematic errors,
nb/(rad*GeV^4) |
---|---|---|---|---|
0.2491 | 45 | 3.5664 | 1.596 | 1.244 |
0.2489 | 63 | 2.1834 | 0.977 | 0.319 |
0.2477 | 81 | 1.4964 | 0.669 | 1.102 |
0.2487 | 171 | 3.8517 | 1.573 | 0.075 |
0.2507 | 261 | 4.1556 | 1.253 | 0.663 |
0.2481 | 279 | 2.9472 | 1.204 | 0.657 |
0.2484 | 297 | 6.604 | 1.832 | 2.446 |
0.3501 | 63 | 5.4406 | 1.405 | 0.827 |
0.3499 | 81 | 4.2102 | 1.168 | 0.841 |
0.3511 | 99 | 2.2048 | 0.78 | 0.177 |
0.3479 | 261 | 3.8348 | 1.213 | 0.367 |
0.3493 | 297 | 2.1172 | 0.864 | 0.064 |
0.4942 | 45 | 2.4428 | 0.815 | 1.479 |
0.4979 | 63 | 1.9773 | 0.528 | 0.158 |
0.4973 | 81 | 2.157 | 0.539 | 0.341 |
0.4974 | 99 | 2.9686 | 0.681 | 0.163 |
0.4999 | 261 | 2.4981 | 0.721 | 0.342 |
0.4963 | 279 | 3.2124 | 0.779 | 0.037 |
0.4961 | 297 | 2.2837 | 0.571 | 0.141 |
0.4945 | 315 | 1.388 | 0.566 | 0.107 |
0.7791 | 45 | 0.6862 | 0.242 | 0.206 |
0.7772 | 63 | 2.1031 | 0.397 | 0.387 |
0.7809 | 81 | 2.0562 | 0.395 | 0.459 |
0.7725 | 99 | 2.4096 | 0.584 | 0.118 |
0.7765 | 261 | 1.7494 | 0.553 | 0.268 |
0.7787 | 279 | 1.8962 | 0.414 | 0.056 |
0.7823 | 297 | 1.1304 | 0.252 | 0.175 |
0.782 | 315 | 1.5119 | 0.315 | 0.258 |
1.216 | 9 | 1.6658 | 0.745 | 0.249 |
1.224 | 27 | 0.89 | 0.246 | 0.074 |
1.205 | 45 | 0.5609 | 0.187 | 0.123 |
1.218 | 63 | 0.605 | 0.213 | 0.229 |
1.219 | 81 | 1.9064 | 0.72 | 0.302 |
1.219 | 297 | 0.5494 | 0.194 | 0.335 |
1.217 | 315 | 0.7237 | 0.18 | 0.123 |
1.211 | 333 | 0.645 | 0.243 | 0.182 |