Difference between revisions of "PosRun 12 10 2013"

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120 Hz , 39 MeV electrons on 2 mm thick tungsten
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Electron coincidence rate was always 80 Hz
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PICAP coincidence detector is compared of two silicon disks 1cm in radius separated by two cm
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{| border="1"  |cellpadding="20" cellspacing="0
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|-
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|<math> \theta</math> ||  E (MeV) || I beam for e- pVs 50 ohms ||  I beam for e+ || e+ Rate  || mag - det dist ( cm)
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|-
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|  50  ||  9.7 || ||. ||
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|-
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|  57  ||  8.8||. || || ||  65
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|-
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|  68 || 6.8 ||  197|| 5820  || 23 || 77
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|-
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|  78 || 5.5 ||  968  || || || 60
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|-
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|  90 || 4.5 ||  || || 23||
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|-
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|}
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[[Positrons_Using_40Mev_Linac#10.2F14.2F13]]
  
  
 
[[Positrons_Using_40Mev_Linac#10.2F14.2F13]]
 
[[Positrons_Using_40Mev_Linac#10.2F14.2F13]]

Latest revision as of 21:35, 10 December 2013

120 Hz , 39 MeV electrons on 2 mm thick tungsten

Electron coincidence rate was always 80 Hz


PICAP coincidence detector is compared of two silicon disks 1cm in radius separated by two cm

[math] \theta[/math] E (MeV) I beam for e- pVs 50 ohms I beam for e+ e+ Rate mag - det dist ( cm)
50 9.7 .
57 8.8 . 65
68 6.8 197 5820 23 77
78 5.5 968 60
90 4.5 23



Positrons_Using_40Mev_Linac#10.2F14.2F13


Positrons_Using_40Mev_Linac#10.2F14.2F13