Difference between revisions of "G4Beamline PbBi"

From New IAC Wiki
Jump to navigation Jump to search
Line 20: Line 20:
  
 
The Random number seed is set by Time in G4beamline to use a different set of pseudo random numbers each time it is run
 
The Random number seed is set by Time in G4beamline to use a different set of pseudo random numbers each time it is run
 +
 +
 +
  
 
{| border="1"
 
{| border="1"
Line 32: Line 35:
 
| 2.5    || 1997 ||  
 
| 2.5    || 1997 ||  
 
|-
 
|-
| 3|| 2233 || 1986
+
| 3|| 2233,2250 || 1986
 
|-
 
|-
 
| 3.5|| 2193 ||  
 
| 3.5|| 2193 ||  

Revision as of 21:41, 28 April 2015

Development of a Positron source using a PbBi converter and a Solenoid

Converter target properties

Definition of Lead Bismuth


1cm diameter target 2 mm thick PbBi

0.5 Tesla solenoid

G4BeamLine and MCNPX

Target thickness optimization

First simple test is to send 1 million, 10 MeV electrons towards a PbBi target and count how many positrons leave the downstream side

The Random number seed is set by Time in G4beamline to use a different set of pseudo random numbers each time it is run



PbBi Thickness (mm) #positrons/million electrons (G4Beamline) #positrons/million electrons (MCNPX)
1 960 1091
1.5 1508
2 1963,1919,1880,1877,1970 1984
2.5 1997
3 2233,2250 1986
3.5 2193
4 2184 1858
5 2042 1646
6 1851 1541
10 1480 1216

TF PosE 04-28-15.png Positrons2.png

Solenoid

Positrons#Simulations