Difference between revisions of "Positrons Using The HRRL"
Line 22: | Line 22: | ||
Reference serkan thesis | Reference serkan thesis | ||
+ | |||
+ | |||
+ | ===Electron Momentum Distributions=== | ||
+ | |||
+ | According to GEANT4 | ||
+ | |||
+ | The electrons which penetrate a 1 mm Tungsten foil have the momentum distribution below | ||
+ | |||
+ | For a 6 MeV incident electron | ||
+ | |||
+ | [[File:HRRL_6MeVePdist_71812.png]] | ||
=Measured HRRL emittance= | =Measured HRRL emittance= |
Revision as of 04:37, 19 July 2012
The purpose of this research is to evaluate the veracity of a positron beam line using the quad triplet method to collect positrons produced when a 10 MeV electron beam impinges on a 1.25 mm thick Tungsten target.
Positron Beam Properties
Tungsten thickness
The optimal Tungsten target thickness to produce positrons using a 10 MeV incident electron beam appears to be 1.25 mm.
Reference Serkan Thesis
Positron Momentum and Phase space distribution
Assuming a 10 meV electron beam having a gaussian spot size with a
= 3mm.
We may want the achromat to have a 10% or less energy spread to measure the above distribution but we will also wan to open the slits to maximize positron current. This may mean accepting an energy spread of 30%.
Reference serkan thesis
Electron Momentum Distributions
According to GEANT4
The electrons which penetrate a 1 mm Tungsten foil have the momentum distribution below
For a 6 MeV incident electron
Measured HRRL emittance
HRRL beam line