FNAL NUSEA results from E.A. Hawker, et al., Phys. Rev. Lett. 80 3715 (1998) ============================================================================ This table gives the average x1 above and below the cut made to eliminate Upsilon events from the data sample, and a weighting factor based on the number of events in each x_2 bin that were above or below this cut. Avg. Above Upsilon Below Upislon Cross Section Bin x_2 avg x1 weight avg x2 weight Ratio Stat Err -- ----- ------ ------ ------ ----- ------------------ 1 0.0364 0 0 0.5732 1.000 1.039 +/- 0.017 2 0.0574 0 0 0.4987 1.000 1.079 +/- 0.013 3 0.0816 0 0 0.4503 1.000 1.113 +/- 0.015 4 0.1063 0.7378 0.019 0.3937 0.981 1.133 +/- 0.020 5 0.1315 0.6340 0.114 0.3420 0.886 1.196 +/- 0.029 6 0.1563 0.5650 0.285 0.3004 0.715 1.124 +/- 0.035 7 0.1815 0.5064 0.446 0.2661 0.554 1.091 +/- 0.043 8 0.2066 0.4672 0.585 0.2383 0.415 1.098 +/- 0.055 9 0.2314 0.4243 0.716 0.2176 0.284 1.055 +/- 0.067 10 0.2643 0.3882 0.852 0.1954 0.148 0.967 +/- 0.067 11 0.3116 0.3573 0.991 0.1750 0.009 0.881 +/- 0.141 In addition to the statistical error on each point, there is also an overall multiplicative systematic error of +/- 1% on each of the cross section ratios. The average mass in each bin above and below the Upsilon cut may be found using m^2 = x1 x2 s, where s = 1503.0 GeV^2