Difference between revisions of "Simulation"
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− | ! | + | !Ne |
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|no cut | |no cut | ||
|19909 | |19909 | ||
+ | |- | ||
+ | |require trigger the e detector | ||
|16457 | |16457 | ||
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− | |k'/kmax min | + | |+ cut on k'/kmax min |
|9612 | |9612 | ||
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+ | |+ cut on 4 hits in the e detector | ||
|9612 | |9612 | ||
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Revision as of 10:38, 14 April 2010
The electron detector
- The electron detector is placed 5 mm above the primary electron beam. To check that, I forced the energy of the scattered electrons to be the one of the primary beam (E=1.165 GeV). The figure below demonstrates that the electron detector is effectively located above the primary beam (ignore the photon detector and scattered photons).
- Then after restoring the scattered electron energy formula, 100 events are generated in the following figures:
- A close-up on the electron detector
- Now looking at some distributions and numbers. The simulation was run with the following inputs:
Beam energy = 1.165 GeV Beam polarization = 80% Dipole length and height: 125cm x 4.125" Laser: 532nm, 1kW and alpha_c=35.28 mrad
Ne | |
---|---|
no cut | 19909 |
require trigger the e detector | 16457 |
9612 | |
9612 |