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85026398984
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note
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eff, resulting in complicated substructures around the various peaks. Also, the fit errors returned by MINUIT are inflated, since there is strong correlation between the parameters for neighboring peaks. Because of the generally unsatisfactory results obtained by peak fitting, we have opted to sum over what we believe are the appropriate bins corresponding to the various event categories, and to take into account the uncertainties arising from the slightly subjective process of choosing bins.
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25
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85026348294
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note
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34≈0.7, significantly larger than the observed Z's. Using the high-gain channels does not help; the majority (50-85 %) of these events appear as pedestals, which is why we count them as pedestals, but some (10-30%) appear as protons, and the rest still appear between 0.2-0.5 in Z. Nothing unusual is seen in examining the x and y position distributions for these events, ruling out the possibility that they are due to hits at the edges of the detectors. An increasing fraction of events falls into this category as the target mass increases.
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0042938029
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[27] Particle Data Group, D. E. Groom et al., Eur. Phys. J. C 15, 1 (2000).
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Eur. Phys. J. C
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Groom, D.E.1
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85026401086
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note
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8Be - the contamination of the true Be sample can be no worse than 20%. It seems likely that the actual contamination is in fact smaller than this.
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29
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85026353269
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note
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0. The uncertainties shown in Table VII are the quadrature sums of the contributions from acceptance, the factors in Table VI, and the uncertainties on the cross sections in Table V.
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