Difference between revisions of "LB Se-79 Soil Analysis"
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<math> A_{Beam Off} = A_{Measure} e^{\lambda t} = 431.10 Hz \pm 54.19 </math> Hz | <math> A_{Beam Off} = A_{Measure} e^{\lambda t} = 431.10 Hz \pm 54.19 </math> Hz | ||
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+ | The efficiency was measured by placing a Ba-133 source at the same position as the pure Se sample and taking the ratio of the measured counts of the 81 keV line to the theoretical number of counts that the sample should have given off, which is computed by | ||
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+ | <math> (Branching Ratio) \times (A_{Source}) \times (3.7 \times 10^{10} \frac{Hz}{Ci}) </math> | ||
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+ | More details can be found at https://wiki.iac.isu.edu/index.php/LB_May_2017_Det_A_Efficiency |
Revision as of 20:30, 15 October 2018
Below is a description of how the activity of the Se-79 in the May 2017 soil/Se was determined.
Activity of Se-79m
First, find the activity of the Se-79m state which has a half life of 3.92
0.01 minutes. The line of interest here is 95.73 0.03 keVHistogram analysis
The most active sample was the 10% Se/soil mixture's pure selenium witness pellet, so let's analyze that first. The histogram for the sample from 615<t<1115 s is shown below.
The line in the stats box labeled "integral" represents the total number of counts in the window, which is
I = 7787
88.24 Countsand the background is
B = 5053.2
60.6 CountsNow subtract the background from the total number of counts in the window
N = 2733.8
107.05Now divide by the runtime to get the activity
= Hz
Note this is the measurement some time after the beam was turned off, so we can correct this back using the known half life of Se-79m (
= 0.0029 0.00008 )Hz
The efficiency was measured by placing a Ba-133 source at the same position as the pure Se sample and taking the ratio of the measured counts of the 81 keV line to the theoretical number of counts that the sample should have given off, which is computed by
More details can be found at https://wiki.iac.isu.edu/index.php/LB_May_2017_Det_A_Efficiency