Niowave 6-2016: Difference between revisions

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|0.0  ||6 || 18
|0.0  ||6 || 18
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|0.0  || 8 ||50,43,42,39,43
|0.0  || 8 ||50,43,42,39,43= 43<math> \pm</math> 4
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|-
|0.0  || 10 || 122,112,119,95,117 = 113<math> \pm</math> 11
|0.0  || 10 || 122,112,119,95,117 = 113<math> \pm</math> 11
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|  0.3  || 6  || 89
|  0.3  || 6  || 89
-
|  0.3  || 8 || running now
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|  0.3  || 10  || 664,652,618,591,603=626<math> \pm</math> 31
|  0.3  || 10  || 664,652,618,591,603=626<math> \pm</math> 31

Revision as of 13:31, 15 June 2016

Previously observed in Niowave_1-2016


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/

Solenoid Field (Tesla) Incident Electron Energy (MeV) Positrons/Million electrons
0.0 6 18
0.0 8 50,43,42,39,43= 43[math]\displaystyle{ \pm }[/math] 4
0.0 10 122,112,119,95,117 = 113[math]\displaystyle{ \pm }[/math] 11
0.2 6 65,62,71,62,58=64[math]\displaystyle{ \pm }[/math] 5
0.2 8 233,210,218,213,215 =218[math]\displaystyle{ \pm }[/math] 9
0.2 10 404,418,420,420,416=416[math]\displaystyle{ \pm }[/math] 7
0.3 6 89

-

0.3 8 running now
0.3 10 664,652,618,591,603=626[math]\displaystyle{ \pm }[/math] 31


G4Beamline_PbBi#Reports