Ilya Selyuzhenkov October 13, 2008
I have finished production of jet trees for Michael's gamma filtered events
You can find jet and skim file lists in my directory at IUCF disk (RCF):
Number of jet events is 1284581 (1020 files).
Production size, including archived log files, is 4.0G.
The script to run jet finder:
/star/institutions/iucf/IlyaSelyuzhenkov/simu/JetTrees/20081008_gJet/StRoot/macros/RunJetSimuSkimFinder.C
JetFinder and JetMaker code:
/star/institutions/iucf/IlyaSelyuzhenkov/simu/JetTrees/20081008_gJet/StRoot/StJetFinder
/star/institutions/iucf/IlyaSelyuzhenkov/simu/JetTrees/20081008_gJet/StRoot/StJetMaker
For more details see these threads of discussions:
Ilya Selyuzhenkov October 14, 2008
Data sets:
Figure 1: Horizontal distance from 4th order polynomial function to max(D_tail-F_tail)
See this page for definition and more details
Figure 2:
purity[g-jet] vs. efficiency[g-jet] (upper left);
rejection[QCD] vs. efficiency[g-jet] (upper right);
purity[g-jet] vs. rejection[QCD] (lower left);
pp2006 to MC ratio, N[pp2006]/(N[g-jet]+N[QCD]), vs. horizontal distance (lower right)
Ilya Selyuzhenkov October 15, 2008
Data sets:
Some observations:
Figure 1a: partonic pt for gamma-jet [old] events
after analysis cuts and partonic pt bin weighting
(Note:Arbitrary absolute scale)
Figure 1b: partonic pt for gamma-jet [gamma-filtered] events after analysis cuts.
Michael's StBetaWeightCalculator has been used to caclulate partonic pt weights
Figure 1c: partonic pt for QCD jets [old] events
after analysis cuts and partonic pt bin weighting
(Note:Arbitrary absolute scale)
Figure 1d: partonic pt for QCD jets [gamma-filtered] events after analysis cuts.
Michael's StBetaWeightCalculator has been used to caclulate partonic pt weights
Figure 2: reconstructed gamma pt: old MC vs. pp2006 data (scaled to the same luminosity)
Figure 3: reconstructed gamma pt: gamma-filtered MC vs. pp2006 data (scaled to the same luminosity)
Ilya Selyuzhenkov October 15, 2008
Data sets:
Figure 1: Horizontal distance from sided residual plot: R_cluster > 0.9
(see Figs. 1-5 from this post for horizontal distance definition)
Figure 2: Purity/efficiency/rejection, and data to MC[gamma-jet+QCD] ratio plots: R_cluster > 0.9
(see text above Fig. 6 from this post for purity, efficiency, and background rejection definition)
Figure 3: Reconstructed gamma pt: R_cluster > 0.98
Figure 4: Horizontal distance from sided residual plot: R_cluster > 0.98
Figure 5: Purity/efficiency/rejection, and data to MC[gamma-jet+QCD] ratio plots: R_cluster > 0.98
Ilya Selyuzhenkov October 21, 2008
Data sets:
Some comments:
Fig. 1-3, upper left plots (pre1=0 pre2=0) show that
average energy per strip in data-driven gamma-jet MC (i.e. solid red square in Fig. 3)
is systematically higher than that for pp2006 data (black circles in Fig. 3).
Note, that there is an agreement between SMD shower shapes
for pp2006 data and data-driven gamma-jet simulations
if one scales them to the same peak value
(Compare red vs. black in upper left plot from Fig. 1 at this link)
Fig. 4, upper left plot (pre1=0 pre2=0):
Integrated SMD energy from 25 strips
in raw gamma-jet simulations (red line) match pp2006 data (black line)
in the region where signal to background ratio is high, E_smd(25-strips)>0.1GeV.
This indicates that raw MC does a good job in
reproducing total energy deposited by direct photon.
Fig. 5, upper left plot (pre1=0 pre2=0):
There is mismatch between distributions of energy in 25 strips cluster
from data-driven gamma-jet simulations and pp2006 data.
This probably reflects the way we scale our library shower shapes
in data-driven shower shape replacement procedure.
Currently, the scaling factor for the library shape is calculated based on the ratio
of direct photon energy from Geant record to the energy of the library photon.
Our library is build out of photons from eta-meson decay,
which has been reconstructed by running pi0 finder.
The purity of the library is about 70% (see Fig. 1 at this post for more details).
The improvement of scaling procedure could be to
preserve total SMD energy deposited within 25 strips from raw MC,
and use that energy to scale shower shapes from the library.
Fig. 6, upper left plot (pre1=0 pre2=0):
Mismatch between integrated 5-strip energy for raw MC and pp2006 in Fig. 6
corresponds to "known" difference in shower shapes from raw Monte-Carlo and real data.
Figure 1: SMD shower shapes: data, raw, and data-driven MC (40 strips).
Vertical axis shows average energy per strip (no overall shower shapes scaling)
Figure 2: Shower shapes: data, raw, and data-driven MC (12 strips)
Figure 3: Shower shapes: data, raw, and data-driven MC (5 strips)
Figure 4: 25 strips SMD cluster energy for raw Monte-Carlo
(Note: type in x-axis lables, should be "25 strip peak" instead of 5)
Figure 5: 25 strips SMD cluster energy for data-driven Monte-Carlo
Figure 6: 5 strips SMD peak energy for raw Monte-Carlo
Figure 7: 5 strips SMD peak energy for data-driven Monte-Carlo
Figure 8:Energy from the right tail (up to 30 strips) for raw Monte-Carlo
Figure 9:Energy from the right tail (up to 30 strips) for data-driven Monte-Carlo
Ilya Selyuzhenkov October 27, 2008
Data sets:
Shower shapes scaling options in data-driven maker:
In all figures below (exept for pp2006 data and raw Monte-Carlo)
the SMD based shower shape scaling has been used.
Figure 1: SMD shower shapes: data, raw, and data-driven MC (40 strips).
Vertical axis shows average energy per strip (no overall shower shapes scaling)
Figure 2: Shower shapes: data, raw, and data-driven MC (12 strips)
Figure 3: Shower shapes: data, raw, and data-driven MC (5 strips)
Figure 4: 25 strips SMD cluster energy for data-driven Monte-Carlo
(SMD based shower shape scaling)
Figure 5: 25 strips SMD cluster energy for raw Monte-Carlo
Note, the difference between results in Fig. 4 and 5. for MC gamma-jets (shown in red)
at low energy (Esmd < 0.04) for pre1=0 pre2=0 case.
This effect is due to the "Number of strips fired in 5-strips cluster > 3" cut.
In data-driven Monte-Carlo we may have shower shapes
with small number of strips fired (rejected in raw Monte-Carlo)
to be replaced by library shape with different (bigger) number of strips fired.
This mostly affects photons which starts to shower
later in the detector and only fires few strips (pre1=0 pre2=0 case)
Ilya Selyuzhenkov October 30, 2008
Below are links to drupal pages
with various SMD energy distributions and shower shapes
for the following set of cuts/conditions:
Figure 1: Case A
Figure 2:Case B
Figure 3:Case C
Figure 4:Case D
Figure 1: Case A
Figure 2:Case B
Figure 3:Case C
Figure 4:Case D
Figure 1: Case A
Figure 2: Case B
Figure 3: Case C
Figure 4: Case D
Figure 1: Case A
Figure 2:Case B
Figure 3:Case C
Figure 4:Case D
Figure 1: Case A
Figure 2:Case B
Figure 3:Case C
Figure 4:Case D
Figure 1: Case A
Figure 2:Case B
Figure 3:Case C
Figure 4:Case D
Figure 1: Case A
Figure 2:Case B
Figure 3:Case C
Figure 4:Case D
Figure 1: Case A
Figure 2:Case B
Figure 3:Case C
Figure 4:Case D