Full simulation and reconstruction of Run2a detector has been used to
generate and reconstruct 100 ttbar events. COT tracking has been performed
with the merged set of tracks, Silicon tracking is done with "Outside-In"
algorithm (RunI style by Weiming Yao) in 2d only.
The denominator is defined using only MonteCarlo quantities:
The efficiency is defined looking at the difference of fitted track
parameters and the OBSP helix.
The cuts are very wide:
CAVEATS
| CUTS |
|
tt + 5 extra min bias | tt + 10 extra min bias |
|
| All generated particles | 34958 | 133421 | 260064 | 337410 |
| Denominator Tracks | 3126 | 5417 | 6560 | 5081 |
| Found Silicon tracks | 2774 (88.7%) | 4646 (85.8%) | 5660 (86.3%) | 4402 (86.6%) |
| Good Silicon tracks | 2724(87.1%) | 4497 (83.0%) | 5286 (80.6%) | 4003(78.8%) |
Study of hit sharing
We looked at the fraction of hits on fiducial (or b-daughter) tracks that are shared as a function of layer ( i.e. radius) and extra minimum bias interactions. A hit is defined shared for this study when the cluster associated to it has a contribution from another particle charge. Note: the geometric charge deposition model underestimates the cluster width, so the amount of sharing. This is particularly true for L0 where the floating strip is not implemented in this model.
| LAYER |
|
|
|
|
| 0 | 0.39 | 0.42 | 0.51 | 0.54 |
| 1 | 0.23 | 0.24 | 0.31 | 0.33 |
| 2 | 0.14 | 0.14 | 0.21 | 0.23 |
| 3 | 0.13 | 0.11 | 0.15 | 0.17 |
| 4 | 0.08 | 0.07 | 0.10 | 0.12 |
| 5 | 0.08 | 0.08 | 0.10 | 0.12 |
| 6 | 0.17 | 0.17 | 0.17 | 0.18 |
| 7 | 0.11 | 0.11 | 0.13 | 0.12 |
| LAYER |
|
|
|
|
| 0 | 0.54 | 0.63 | 0.73 | 0.75 |
| 1 | 0.37 | 0.46 | 0.46 | 0.49 |
| 2 | 0.24 | 0.24 | 0.35 | 0.36 |
| 3 | 0.17 | 0.13 | 0.22 | 0.33 |
| 4 | 0.16 | 0.07 | 0.13 | 0.17 |
| 5 | 0.14 | 0.11 | 0.14 | 0.20 |
| 6 | 0.20 | 0.21 | 0.18 | 0.21 |
| 7 | 0.12 | 0.12 | 0.17 | 0.17 |
TO DO NEXT