Difference between revisions of "June, 7, 2007 Cf rate measurements using Photonics PMT"
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6: No source backround | 6: No source backround | ||
| + | =Measurements = | ||
| + | == Using Photonics PMT and BC | ||
{| border="5" | {| border="5" | ||
! Configuration || Rate (counts/min) || Statistical Error in Rate (Counts/min) | ! Configuration || Rate (counts/min) || Statistical Error in Rate (Counts/min) | ||
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|} | |} | ||
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| + | == Analysis === | ||
Revision as of 17:59, 8 June 2007
Cf source was placed 16.5 cm away from face of PHotonics PMT. The PMT output signal was descriminated by a Lecroy Model 821 descriminator set to pass any voltage below -0.5 mV. The descriminated output was then sent to a counter Model TC 531.
Configuration Definitions
1: Placed the Cf source 16.5 cm from face of Scintillator. neutrons passing through scintillator would also pass through PMT
2: Inserted a 2.5 cm thick steel shielding wall between Scintillator and Cf source. Right up against Scintillator
3: Replaced steel wall with 5 cm thick lead shielding brick
4: Replaced lead brick with 6.7 cm thick paraffin block ( Paraffin N.F. , Household wax made by Parowax. 4 cackes, total net weight 16 oz (454 g))
5: Increased thickness of paraffin block to 13.4 cm
6: No source backround
Measurements
== Using Photonics PMT and BC
| Configuration | Rate (counts/min) | Statistical Error in Rate (Counts/min) |
|---|---|---|
| 1 | 2.7e3 | 0.09e3 |
| 2 | 2.2e3 | 0.01e3 |
| 3 | 0.8e3 | 0.02e3 |
| 4 | 2.2e3 | 0.08e3 |
| 5 | 1.8e3 | 0.02e3 |
| 6 |