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Run-11 Transverse Jets: Update to Jet Group (October 30, 2012)
Even though my previous update to the jet group contained a massive amount of information, I was not able to get to everything I had wanted. Here, I post a follow-up addressing some questions raised prior to the meeting as well as questions raised during the meeting.
χ2 Distributions
The first issue involves the χ2 distributions for the sinusoidal fits. Carl has pointed out that if the scattering is purely statistical, the χ2 values should follow the distribution for the specific degrees of freedom. In this case, the Sivers fit has nominally four degrees of freedom, while the Collins(-like) fits have nominally ten.
For the following figures, I separate the data as best I can into independent samples. I fit separately for trigger, xF > 0 or xF < 0, η > 0 or η < 0, ηjet bin (Sivers), pion charge state (Collins), and low or high-z (Collins as a function of jT). I histogram the χ2 values separately for xF > 0 or xF < 0.
Note: Since I am trying to utilize independent samples, I do not include the "all triggers" fits.
Since I needed one, myself, here's a reminder: the average of the χ2 distribution should equal the number of degrees of freedom; the expected distribution is quite asymmetric for low degrees of freedom. I fit the histograms with the distribution as seen in Bevington Appendix C-4 allowing for a floating over-all scale factor. I do not include fits where, due to statistics, there are fewer than the nominal degrees of freedom.
Figure 1
Figure 2
Figure 3
As with the Collins fits as a function of z, the fits as a function of jT are entirely sensible.
Figure 4
The high-z asymmetries have very few statistics, however, rebinning sufficiently removes the flutuations that one gets a decent picture of the χ2. Again, it's completely sane.
Figure 5
The story is much the same for Collins-like.
Figure 6
Figure 7
Finally, the xF < 0 high-z Collins-like looks nuts, but I suspect it's a result of fewer statistics. Perhaps, it's just an outlier in what appears to be an otherwise perfectly sane statistical cross-check.
The bottom line: This study suggests the statistical uncertainties from the fits provide a realistic estimate of the uncertainties, leaving little room for additional systematic contributions.
Sivers for xF < 0
Also raised was the issue about Sivers asymmetries for xF < 0. I have shown these distributions summed over ηjetand trigger but not broken down into ηjet-bins.
Figure 8: Sivers Asymmetry in Bins of ηjet for xF < 0
All Triggers | JP0 | JP1 |
---|---|---|
JP2 | AJP | VPDMB |
Interestingly, there does appear to be a positive asymmetry for |η| > 0.5 driven by JP2. It appears to be small, but the data points are systematically above the horizontal. This is probably worth some investigation.
Sivers Fits for Individual pT Bins
The final issue I will address for this update is to look at Sivers fits for individual pT bins. There appear to be non-zero bins in JP0 and VPDM at high-pT. One sensible check is to look at the fits themselves for those particular bins. One thought is that these bins may be scarcely populated, leading to unreliable fit information. I also turn my attention to individual fits for xF < 0, which seem to be systematically above the horizontal.
Figure 9: Sivers Asymmetry Fits for All Triggers, All η, and xF > 0
6.0 < pT < 7.1 GeV/c |
---|
7.1 < pT < 8.4 GeV/c |
8.4 < pT < 9.9 GeV/c |
9.9 < pT < 11.7 GeV/c |
11.7 < pT < 13.8 GeV/c |
13.8 < pT < 16.3 GeV/c |
16.3 < pT < 19.2 GeV/c |
19.2 < pT < 22.7 GeV/c |
22.7 < pT < 26.8 GeV/c |
26.8 < pT < 31.6 GeV/c |
31.6 < pT < 37.3 GeV/c |
Figure 10: Sivers Asymmetry Fits for JP1, All η, and xF > 0
9.9 < pT < 11.7 GeV/c |
---|
11.7 < pT < 13.8 GeV/c |
13.8 < pT < 16.3 GeV/c |
16.3 < pT < 19.2 GeV/c |
19.2 < pT < 22.7 GeV/c |
22.7 < pT < 26.8 GeV/c |
26.8 < pT < 31.6 GeV/c |
31.6 < pT < 37.3 GeV/c |
Figure 11: Sivers Asymmetry Fits for VPDMB, All η, and xF > 0
6.0 < pT < 7.1 GeV/c |
---|
7.1 < pT < 8.4 GeV/c |
8.4 < pT < 9.9 GeV/c |
9.9 < pT < 11.7 GeV/c |
11.7 < pT < 13.8 GeV/c |
13.8 < pT < 16.3 GeV/c |
16.3 < pT < 19.2 GeV/c |
19.2 < pT < 22.7 GeV/c |
22.7 < pT < 26.8 GeV/c |
26.8 < pT < 31.6 GeV/c |
31.6 < pT < 37.3 GeV/c |
Figure 12: Sivers Asymmetry Fits for All Triggers, η < -0.5, and xF < 0
6.0 < pT < 7.1 GeV/c |
---|
7.1 < pT < 8.4 GeV/c |
8.4 < pT < 9.9 GeV/c |
9.9 < pT < 11.7 GeV/c |
11.7 < pT < 13.8 GeV/c |
13.8 < pT < 16.3 GeV/c |
16.3 < pT < 19.2 GeV/c |
19.2 < pT < 22.7 GeV/c |
22.7 < pT < 26.8 GeV/c |
26.8 < pT < 31.6 GeV/c |
31.6 < pT < 37.3 GeV/c |
Figure 13: Sivers Asymmetry Fits for JP2, η < -0.5, and xF < 0
16.3 < pT < 19.2 GeV/c |
---|
19.2 < pT < 22.7 GeV/c |
22.7 < pT < 26.8 GeV/c |
26.8 < pT < 31.6 GeV/c |
31.6 < pT < 37.3 GeV/c |
Figure 14: Sivers Asymmetry Fits for All Triggers, η > 0.5, and xF < 0
6.0 < pT < 7.1 GeV/c |
---|
7.1 < pT < 8.4 GeV/c |
8.4 < pT < 9.9 GeV/c |
9.9 < pT < 11.7 GeV/c |
11.7 < pT < 13.8 GeV/c |
13.8 < pT < 16.3 GeV/c |
16.3 < pT < 19.2 GeV/c |
19.2 < pT < 22.7 GeV/c |
22.7 < pT < 26.8 GeV/c |
26.8 < pT < 31.6 GeV/c |
31.6 < pT < 37.3 GeV/c |
Figure 15: Sivers Asymmetry Fits for JP2, η > 0.5, and xF < 0
16.3 < pT < 19.2 GeV/c |
---|
19.2 < pT < 22.7 GeV/c |
22.7 < pT < 26.8 GeV/c |
26.8 < pT < 31.6 GeV/c |
31.6 < pT < 37.3 GeV/c |
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