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Material | Density | Radiation length | Interaction length | |
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<ac:structured-macro ac:name="unmigrated-wiki-markup" ac:schema-version="1" ac:macro-id="51bfe798-04ca-4bb9-854b-d873498c4262"><ac:plain-text-body><![CDATA[ |
| [g/cm3] | [cm] | [cm] |
BGO | 7.13 | 1.12 | 21.88 | |
PbWO4 | 8.3 | 0.9 | 18. | |
SCG1-C | 3.36 | 4.25 | 45.6 |
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| BGO |
| PbWO4 |
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Detector | Layers | Thickness/layer | Segmentation | X0 | Lambda | X0 | Lambda |
|
| [cm] | [cmxcm] |
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ECAL Barrel | 8 | 3 | 3x3 | 21.4 | 1.1 | 27 | 1.3 |
HCAL Barrel | 17 | 6 | 6x6 |
| 4.7 |
| 5.7 |
Total Barrel | 25 |
|
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| 5.8 |
| 7 |
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ECAL EndCAP | 8 | 3 | 3x3 | 21.4 | 1.1 | 27 | 1.3 |
HCAL EndCAP | 17 | 6 | 6x6 |
| 4.7 |
| 5.7 |
Total EndCAP | 25 |
|
|
| 5.8 |
| 7 |
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The shell script below demonstrates how to run slic using the ccal02 geometry. Note for a dual readout calorimeter it is important that the
/physics/enableOptical flag is set otherwise no Cherenkov photons will be created!
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The Table below list all the data samples currently available at Fermilab. The files can be found on the following directory (on the bluearc system)
/ilc/ild/wenzel/ccal02/slcio_combined
File Name | Type of Events | Nr of Events |
---|---|---|
pi_Theta90_1GeV.slcio | single 1 GeV pions at theta 90 degrees | 20000 |
pi_Theta90_2GeV.slcio | single 2 GeV pions at theta 90 degrees | 20000 |
pi_Theta90_5GeV.slcio | single 5 GeV pions at theta 90 degrees | 20000 |
pi_Theta90_10GeV.slcio | single 10 GeV pions at theta 90 degrees | 20000 |
pi_Theta90_20GeV.slcio | single 20 GeV pions at theta 90 degrees | 20000 |
pi_Theta90_50GeV.slcio | single 50 GeV pions at theta 90 degrees | 20000 |
pi_Theta90_100GeV.slcio | single 100 GeV pions at theta 90 degrees | 20000 |
electron_Theta90_1GeV.slcio | single 1 GeV electrons at theta 90 degrees | 5000 |
electron_Theta90_2GeV.slcio | single 2 GeV electrons at theta 90 degrees | 5000 |
electron_Theta90_5GeV.slcio | single 5 GeV electrons at theta 90 degrees | 5000 |
electron_Theta90_10GeV.slcio | single 10 GeV electrons at theta 90 degrees | 5000 |
electron_Theta90_20GeV.slcio | single 20 GeV electrons at theta 90 degrees | 5000 |
electron_Theta90_50GeV.slcio | single 50 GeV electrons at theta 90 degrees | 2432 |
electron_Theta90_100GeV.slcio | single 100 GeV electrons at theta 90 degrees | 1215 |
neutrons_20GeV.slcio | single 20 GeV neutrons | 200 |
n_Theta90_1GeV.slcio | single 1 GeV neutrons at theta 90 degrees | 10000 |
n_Theta90_2GeV.slcio | single 2 GeV neutrons at theta 90 degrees | 10000 |
n_Theta90_5GeV.slcio | single 5 GeV neutrons at theta 90 degrees | 10000 |
n_Theta90_10GeV.slcio | single 10 GeV neutrons at theta 90 degrees | 10000 |
n_Theta90_20GeV.slcio | single 20 GeV neutrons at theta 90 degrees | 10000 |
nbar_Theta90_1GeV.slcio | single 1 GeV anti-neutrons at theta 90 degrees | 9750 |
nbar_Theta90_2GeV.slcio | single 2 GeV anti-neutrons at theta 90 degrees | 10000 |
nbar_Theta90_5GeV.slcio | single 5 GeV anti-neutrons at theta 90 degrees | 10000 |
nbar_Theta90_10GeV.slcio | single 10 GeV anti-neutrons at theta 90 degrees | 9700 |
nbar_Theta90_20GeV.slcio | single 20 GeV anti-neutrons at theta 90 degrees | 9950 |
muon_Theta90_50GeV.slcio | single 50 GeV muons | 5000 |
K0L_Theta90_1GeV.slcio | single 1 GeV K longs at theta 90 degrees | 20000 |
K0L_Theta90_2GeV.slcio | single 2 GeV K longs at theta 90 degrees | 20000 |
K0L_Theta90_5GeV.slcio | single 5 GeV K longs at theta 90 degrees | 20000 |
K0L_Theta90_10GeV.slcio | single 10 GeV K longs at theta 90 degrees | 20000 |
K0L_Theta90_20GeV.slcio | single 20 GeV K longs at theta 90 degrees | 20000 |
K0L_Theta90_50GeV.slcio | single 50 GeV K longs at theta 90 degrees | 20000 |
|
|
|
panpyZZnunubaruds-0-1000.slcio | ZZ -> neutrino neutrino jet jet | 1000 |
Z0_Theta90_50GeV.slcio | single 50 GeV Z 's at theta 90 degrees | 100000 |
W_0_100.slcio | single 0-100 GeV W 's | 20000 |
W_100_200.slcio | single 100-200 GeV W 's | 20000 |
pythiaZhiggs120_uds_4jets.slcio | associated Z Higgs production Z and Higgs decay into light quarks (jets) | 4823 |