Draft:Minimum detectable activity

{{Short description|Measurement concept in nuclear physics}}

{{Draft topics|mathematics}}

{{AfC topic|stem}}

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Minimum detectable activity (MDA) is the lowest activity of a radioactive nuclide that can be detected with a detector system, given a particular confidence level{{cite book |last1=Gilmore |first1=Gordon |title=Practical gamma-ray spectrometry |date=2011 |publisher=Wiley |location=Chichester |isbn=978-0-470-86196-7 |edition=2., repr. with corr}}. It is a concept that can be used in several circumstances, such as in whole-body counting or monitoring atmospheric radionuclides{{cite journal |last1=Britton |first1=R. |last2=Davies |first2=A. V. |last3=Burnett |first3=J. L. |last4=Jackson |first4=M. J. |title=A high-efficiency HPGe coincidence system for environmental analysis |journal=Journal of Environmental Radioactivity |date=1 August 2015 |volume=146 |pages=1–5 |doi=10.1016/j.jenvrad.2015.03.033 |url=http://dx.doi.org/10.1016/j.jenvrad.2015.03.033 |issn=0265-931X}}, to determine the presence or absence of a radioactive substance or compare the performance of detector systems.

When it comes to gamma spectroscopy, the minimum detectable activity can be written as

MDA = \frac{L_D}{\epsilon_\gamma \cdot P_\gamma \cdot t_M},

where L_D ins the detection limit in units of counts, \epsilon_\gamma is the detection efficiency of the gamma spectrometer at the particular gamma-ray energy, P_\gamma is the probability of emission for the gamma ray, and t_M is the live time of the measurement. The formula for L_D changes depending on the confidence level. For a confidence level of 95%,

L_D = 2.71 + 3.29 \sigma_0 ,

where \sigma_0 is the uncertainty in background counts in a region-of-interest around the ramma-ray energy. If B is the number of background counts in the region-of-interest, it can be shown that \sigma_0 = \sqrt{2B}.

References

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