Difference between revisions of "Simulation"
From PolWiki
Jump to navigationJump to searchLine 29: | Line 29: | ||
!Ne_total | !Ne_total | ||
!Ne_detected | !Ne_detected | ||
− | |||
|- | |- | ||
|no cut | |no cut | ||
+ | |19909 | ||
+ | |16457 | ||
+ | |- | ||
+ | | | ||
|k'/kmax min cut | |k'/kmax min cut | ||
− | | | + | |9612 |
− | | | + | |9612 |
− | |||
− | |||
− | |||
|} | |} |
Revision as of 10:34, 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_total | Ne_detected | ||
---|---|---|---|
no cut | 19909 | 16457 | |
k'/kmax min cut | 9612 | 9612 |