Unmatched Fractions
One relevant question before adding in the 5-6 GeV/c bin is what fraction of reconstructed jets do not match to parton jets? In Run-9 ~20% of jets in the 6-7.1 GeV/c bin did not match to a parton jet. Here, in principle, the fraction should be lower. However, for VPDMB, I take all jets below 16.3 GeV/c. Thus, there is no trigger-filtering in my calculation. This fact coupled with the growing soft cross section seems to conspire to raise the unmatched fraction in 2011. It seems that the trigger-bias from Run-9 actually helps in this arena over Run-11 min-bias! Reducing the cone radius to 0.5 does appear to help to some degree. I have not run over the data trees with R = 0.5 so I cannot yet say how much is the cost in statistics.
Table 1
Bin [GeV/c] |
R = 0.6 |
R = 0.5 |
|
Unmatched (to parton jet) Fraction |
Unmatched (to particle jet) Fraction |
Unmatched (to parton jet) Fraction |
5-6 |
0.445149 |
0.105468 |
0.369943 |
6-7.1 |
0.343303 |
0.102521 |
0.288886 |
7.1-8.4 |
0.300243 |
0.102494 |
0.256054 |
8.4-9.9 |
0.224948 |
0.10803 |
0.137968 |
9.9-11.7 |
0.178408 |
0.0882758 |
0.152845 |
11.7-13.8 |
0.159218 |
0.103019 |
0.158194 |
13.8-16.3 |
0.000924567 |
2.02448e-05 |
0.000333341 |
Jet Histograms
The following histograms represent jets from anti-kT with R = 0.6.
Figure 1
Figure 2
Figure 3
Figure 4
Parton Jets |
Particle Jets |
|
|
Table 2: Parton Jets
Bin |
mean (calc) |
mean err (calc) |
sigma (calc) |
mean (fit) |
mean err (fit) |
sigma (fit) |
0 |
4.376700 |
0.050112 |
1.782332 |
4.298699 |
0.099149 |
1.995898 |
1 |
5.255551 |
0.070918 |
2.032022 |
5.048214 |
0.167162 |
2.171887 |
2 |
6.119759 |
0.114194 |
2.387166 |
5.832943 |
0.186998 |
2.531867 |
3 |
7.114054 |
0.177052 |
2.742883 |
6.901127 |
0.464553 |
2.823919 |
4 |
8.850526 |
0.242213 |
3.054184 |
8.986211 |
0.331816 |
2.786197 |
5 |
11.426827 |
0.275702 |
2.838530 |
11.541767 |
0.500606 |
2.639954 |
6 |
14.243042 |
0.174677 |
3.040576 |
14.394541 |
1.286680 |
2.772319 |
Table 3: Particle Jets
Bin |
mean (calc) |
mean err (calc) |
sigma (calc) |
mean (fit) |
mean err (fit) |
sigma (fit) |
0 |
4.841764 |
0.036212 |
1.567174 |
4.870950 |
0.058215 |
1.754405 |
1 |
5.916643 |
0.053980 |
1.722295 |
5.891218 |
0.164114 |
1.726686 |
2 |
7.008965 |
0.096950 |
2.126271 |
6.959531 |
0.155951 |
2.333823 |
3 |
8.161178 |
0.153885 |
2.437989 |
8.686677 |
0.207796 |
1.989351 |
4 |
10.104818 |
0.188913 |
2.194968 |
9.990243 |
0.248133 |
2.203013 |
5 |
11.791698 |
0.368663 |
2.554170 |
12.303599 |
0.276353 |
1.898854 |
6 |
14.837272 |
0.146978 |
2.562654 |
15.116610 |
0.152352 |
2.163757 |
By rights I should calculate the pT-shifts for the two η windows as well. However, in checking the values, they are consistent with those of the combined window within statistical uncertainties.
Figure 5
Parton Jets |
Particle Jets |
|
|
Figure 6
Parton Jets |
Particle Jets |
|
|
Track Histograms
Figure 7
The issue from last week involving stray tracks above the pion band appears to be resolved by enforcing a cut on the number of hits used in the dE/dx calculation. Here, I require more than 5. The cut appears to resolve the issue entirely.
Figure 8
Figure 9
Figure 10
Figure 11
Figure 12
Figure 13
The current cut is ΔR > 0.1. This means the resolution is ~0.36 or lower. A resolution of 0.4 corresponds to a damping of ~7.7%, while a resolution of 0.36 corresponds to a damping of ~6.3%.