Difference between revisions of "G4Beamline PbBi"
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Line 39: | Line 39: | ||
| 2 || 1963,1919,1880,1877,1970 = 1902 <math>\pm</math> 43 || 1984 | | 2 || 1963,1919,1880,1877,1970 = 1902 <math>\pm</math> 43 || 1984 | ||
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− | | 2.5 || 1997 || | + | | 2.5 || 1997 || 2062 |
|- | |- | ||
| 3|| 2233,2250, 2251,2226 , 2222=2236 <math>\pm</math> 13|| 1986 | | 3|| 2233,2250, 2251,2226 , 2222=2236 <math>\pm</math> 13|| 1986 | ||
|- | |- | ||
− | | 3.5|| 2193 || | + | | 3.5|| 2193 || 1938 |
|- | |- | ||
| 4|| 2184,2156,2089,2173,2181=2157 <math>\pm</math> 39 || 1858 | | 4|| 2184,2156,2089,2173,2181=2157 <math>\pm</math> 39 || 1858 |
Revision as of 18:28, 29 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
The G4Beamlin incident electron beam has the following properties
beam gaussian particle=e- nEvents=1000000 beamZ=0.0 sigmaX=1.0 sigmaY=1.0 sigmaXp=0.100 sigmaYp=0.100 meanMomentum=10.0 sigmaP=4.0 meanT=0.0 sigmaT=0.0
PbBi Thickness (mm) | #positrons/million electrons (G4Beamline) | #positrons/million electrons (MCNPX) |
1 | 960,874, 916,934,897=916 +/- 33 | 1091 |
1.5 | 1508 | |
2 | 1963,1919,1880,1877,1970 = 1902 | 431984 |
2.5 | 1997 | 2062 |
3 | 2233,2250, 2251,2226 , 2222=2236 | 131986 |
3.5 | 2193 | 1938 |
4 | 2184,2156,2089,2173,2181=2157 | 391858 |
5 | 2042 | 1646 |
6 | 1851, 1932 | 1541 |
10 | 1480 | 1216 |
Energy Distribution
Angular distribution of positrons
2mm thick, 10 MeV, 1 cm cylindrical incident electron distribution, 100k positrons, 1 million electrons, commas eliminated, on surface of target find Pz,Py,Pz, Vx,Vy,Vz for positrons and electrons