Now that the xF < 0 issue appears to be resolved, it is useful to make one more apples-to-apples comparison with Kevin. For this comparison, I have removed the geometric trigger and edited the Nhits cut to require a miminum of 21 hits rather than the minimum of 6 applied to Nhits, dE/dx. Also, I have added additional z-bins to correspond to Kevin's definitions. Our polarization corrections are still a bit different, but he will implement the fill-by-fill corrections, soon. Also, I still implement my high-pT cut at 9.9 GeV/c to correspond with my jet-pT binning.
pT > 9.9 GeV/c
Figure 1: Total Range of Pseudorapidity
Figure 2: |η| < 0.5
Figure 3: 0.5 < |η| < 1
Table 1: π+
xF > 0 |
xF < 0 |
η Range |
Linear Fit |
Uncertainty |
χ2/ν |
Constant Fit |
Uncertainty |
χ2/ν |
Linear Fit |
Uncertainty |
χ2/ν |
Constant Fit |
Uncertainty |
χ2/ν |
|η| < 1 |
0.0320 |
0.00396 |
6.078/5 |
0.00350 |
0.000487 |
19.42/6 |
0.0129 |
0.00397 |
13.95/5 |
0.00126 |
0.000488 |
17.75/6 |
|η| < 0.5 |
0.0254 |
0.00493 |
5.508/5 |
0.00281 |
0.000606 |
10.37/6 |
0.0125 |
0.00489 |
11.32/5 |
0.00133 |
0.000601 |
12.94/6 |
0.5 < |η| < 1 |
0.0439 |
0.00663 |
3.520/5 |
0.00476 |
0.000817 |
13.37/6 |
0.0136 |
0.00680 |
7.822/5 |
0.00113 |
0.000834 |
9.991/6 |
Table 2: π-
xF > 0 |
xF < 0 |
η Range |
Linear Fit |
Uncertainty |
χ2/ν |
Constant Fit |
Uncertainty |
χ2/ν |
Linear Fit |
Uncertainty |
χ2/ν |
Constant Fit |
Uncertainty |
χ2/ν |
|η| < 1 |
-0.0338 |
0.00411 |
15.45/5 |
-0.00397 |
0.000494 |
18.57/6 |
-0.0106 |
0.00412 |
2.707/5 |
-0.00117 |
0.000495 |
3.739/6 |
|η| < 0.5 |
-0.0252 |
0.00511 |
12.74/5 |
-0.00317 |
0.000615 |
10.52/6 |
-0.0155 |
0.00507 |
2.966/5 |
-0.00145 |
0.000610 |
6.700/6 |
0.5 < |η| < 1 |
-0.0493 |
0.00690 |
6.741/4 |
-0.00543 |
0.000832 |
15.20/5 |
-0.00102 |
0.00705 |
12.06/5 |
-0.000636 |
0.000848 |
11.52/6 |
So, by in large, the values are quite similar to my previous update. The trends are a bit cleaner. This could perhaps be the effect of more statistics, but also could be the result of the Nhits > 20 cut. Perhaps, the present cut is more selective of good pion events. For xF > 0 and the full range of psuedorapidity, Kevin sees averages of 0.00356±0.000511 and ‐0.00415±0.000519 for π+ and π-, respectively. For xF < 0 and the full range of pseudorapidity, Kevin sees averages of 0.00141±0.000504 and -0.00115±0.000509 for π+ and π-, respectively.
pT < 9.9 GeV/c
Figure 4: Total Range of Pseudorapidity
Figure 5: |η| < 0.5
Figure 6: 0.5 < |η| < 1
Table 3: π+
xF > 0 |
xF < 0 |
η Range |
Linear Fit |
Uncertainty |
χ2/ν |
Constant Fit |
Uncertainty |
χ2/ν |
Linear Fit |
Uncertainty |
χ2/ν |
Constant Fit |
Uncertainty |
χ2/ν |
|η| < 1 |
0.00910 |
0.00221 |
11.66/6 |
0.00122 |
0.000337 |
15.42/7 |
0.000771 |
0.00222 |
2.569/6 |
4.95e-05 |
0.000337 |
2.668/7 |
|η| < 0.5 |
0.00451 |
0.00278 |
9.490/6 |
0.000636 |
0.000424 |
9.862/7 |
0.000427 |
0.00276 |
2.303/6 |
-0.000272 |
0.000420 |
1.907/7 |
0.5 < |η| < 1 |
0.0170 |
0.00364 |
9.805/6 |
0.00223 |
0.000555 |
15.39/7 |
0.00295 |
0.00372 |
7.632/6 |
0.000631 |
0.000565 |
7.011/7 |
Table 4: π-
xF > 0 |
xF < 0 |
η Range |
Linear Fit |
Uncertainty |
χ2/ν |
Constant Fit |
Uncertainty |
χ2/ν |
Linear Fit |
Uncertainty |
χ2/ν |
Constant Fit |
Uncertainty |
χ2/ν |
|η| < 1 |
-0.00989 |
0.00226 |
4.359/6 |
-0.00114 |
0.000342 |
12.35/7 |
-0.00321 |
0.00227 |
9.227/6 |
-0.000421 |
0.000342 |
9.719/7 |
|η| < 0.5 |
-0.00809 |
0.00283 |
2.690/6 |
-0.00115 |
0.000430 |
3.707/7 |
-0.00186 |
0.00281 |
8.042/6 |
-8.89e-05 |
0.000426 |
8.436/7 |
0.5 < |η| < 1 |
-0.0131 |
0.00375 |
6.742/6 |
-0.00113 |
0.000565 |
14.85/7 |
-0.00569 |
0.00382 |
7.283/6 |
-0.00102 |
0.000574 |
6.320/7 |
Again, the values are similar to my previous update. The trends, again, appear to be a bit cleaner. For xF > 0 and the full range of pseudorapidity, Kevin sees averages of 0.00122±0.000348 and -0.00119±0.000353 for π+ and π-, resectively. For xF < 0, he sees averages of 2.29e-05±0.000345 and -0.000556±0.000351.
Summary
Figure 7
pT > 9.9 GeV/c |
pT < 9.9 GeV/c |
|
|
In Fig. 7 I post the slopes as a function of η. The behavior is quite similar to my previous results. The differences may be statistically significant given the high degree of correlation between the events.