Difference between revisions of "Elong-13-06-03"
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− | For the spectrometer setting bins plots, where <math>A_{zz}</math> and <math>b_1 | + | For the spectrometer setting bins plots, where <math>A_{zz}</math> and <math>b_1</math> are in blue and red, these are included as an additional systematic uncertainty. For the rebinned plots, where <math>A_{zz}</math> and <math>b_1</math> are in pink, each of the drift uncertainties are added as a weighted average. The weights are the number of events that each spectrometer contributes to the rebinned statistics. |
==Conservative Estimates== | ==Conservative Estimates== |
Revision as of 16:00, 3 June 2013
Including Drift by Bin
Dustin's work on the drift has given a different value depending on the spectrometer setting, which are shown in the table below.
<math>x_{\mathrm{Spectrometer}}</math> <math>dA_{zz}^{drift}</math> 0.15 0.0046 0.30 0.0037 0.45 0.0028 0.55 0.0021
For the spectrometer setting bins plots, where <math>A_{zz}</math> and <math>b_1</math> are in blue and red, these are included as an additional systematic uncertainty. For the rebinned plots, where <math>A_{zz}</math> and <math>b_1</math> are in pink, each of the drift uncertainties are added as a weighted average. The weights are the number of events that each spectrometer contributes to the rebinned statistics.
Conservative Estimates
If we apply these with a conservative estimate, with <math>P_{zz}=20\%</math> and <math>dA_{zz}^{(Rel. Sys)} = 12\%</math>, we can estimate both the full spectrometer bins:
We can then use a weighted average for <math>dA_{zz}^{drift}</math>, where the weights are number of events that each spectrometer setting contributes to a particular <math>x</math> bin. The rebinned estimate is then:
Same as above, but if we split the systematic uncertainty into bars, we get:
Optimistic Estimates
If we apply these with an optimistic estimate, with <math>P_{zz}=40\%</math> and <math>dA_{zz}^{(Rel. Sys)} = 9\%</math>, we can estimate both the full spectrometer bins:
We can then use a weighted average for <math>dA_{zz}^{drift}</math>, where the weights are number of events that each spectrometer setting contributes to a particular <math>x</math> bin. The rebinned estimate is then:
Same as above, but if we split the systematic uncertainty into bars, we get:
--E. Long 20:58, 3 June 2013 (UTC)