Difference between revisions of "Niowave 6-2016"
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|+ Positron Rates -vs- Solenoid Field for 2mm thick PbBi target and several Beam pipe diameters | |+ Positron Rates -vs- Solenoid Field for 2mm thick PbBi target and several Beam pipe diameters | ||
|} | |} | ||
+ | |||
+ | |||
+ | |||
+ | = 34.8 mm pipe, 0.0 -> 0.5 Tesla, E= 6,8,10 MeV.= | ||
+ | |||
+ | positrons produced per million incident electrons on a 2mm thick PbBi target that exit a 15 cm long Solenoid surrounding a 34.8 mm diameter beam pipe. | ||
+ | |||
+ | running in | ||
+ | |||
+ | /home/foretony/src/GEANT4/geant4.9.6.p02/Simulations/NioWave/SolenoidExit/batch/ | ||
+ | |||
+ | {| border="1" | ||
+ | {| border="1" | ||
+ | | Solenoid Field (Tesla) || Incident Electron Energy (MeV)|| Positrons/Million electrons | ||
+ | |- | ||
+ | |0.0 ||6 || 18, running this now | ||
+ | |- | ||
+ | |0.0 || 8 ||50,43,42,39,43= 43<math> \pm</math> 4 | ||
+ | |- | ||
+ | |0.0 || 10 || 122,112,119,95,117 = 113<math> \pm</math> 11 | ||
+ | |- | ||
+ | | 0.2 || 6 || 65,62,71,62,58=64<math> \pm</math> 5 | ||
+ | |- | ||
+ | | 0.2 || 8 ||233,210,218,213,215 =218<math> \pm</math> 9 | ||
+ | |- | ||
+ | | 0.2 || 10 || 404,418,420,420,416=416<math> \pm</math> 7 | ||
+ | |- | ||
+ | | 0.3 || 6 || 89,96,91,94,102=94<math> \pm</math> 5 | ||
+ | |- | ||
+ | | 0.3 || 8 || 324,308,319,318,310=316<math> \pm</math> 7 | ||
+ | |- | ||
+ | | 0.3 || 10 || 664,652,618,591,603=626<math> \pm</math> 31 | ||
+ | |+ | ||
+ | |} | ||
+ | |||
+ | |||
+ | [[G4Beamline_PbBi#Reports]] |
Latest revision as of 17:48, 16 June 2016
Previously observed in Niowave_1-2016
34.8 mm pipe, 0.0 -> 0.5 Tesla, E= 6,8,10 MeV.
positrons produced per million incident electrons on a 2mm thick PbBi target that exit a 15 cm long Solenoid surrounding a 34.8 mm diameter beam pipe.
running in
/home/foretony/src/GEANT4/geant4.9.6.p02/Simulations/NioWave/SolenoidExit/batch/
Solenoid Field (Tesla) | Incident Electron Energy (MeV) | Positrons/Million electrons |
0.0 | 6 | 18, running this now |
0.0 | 8 | 50,43,42,39,43= 43 | 4
0.0 | 10 | 122,112,119,95,117 = 113 | 11
0.2 | 6 | 65,62,71,62,58=64 | 5
0.2 | 8 | 233,210,218,213,215 =218 | 9
0.2 | 10 | 404,418,420,420,416=416 | 7
0.3 | 6 | 89,96,91,94,102=94 | 5
0.3 | 8 | 324,308,319,318,310=316 | 7
0.3 | 10 | 664,652,618,591,603=626 | 31