2021
DOI: 10.1007/978-3-030-73488-6_11
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Radioactive Noble Gas Detection and Measurement with Plastic Scintillators

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Cited by 5 publications
(2 citation statements)
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“…where A is the area of the distribution, µ is its centroid and σ 2 is the variance of the Gaussian distribution. For fitting the α-spectra of 222 Rn and its short-lived progenies, a composite model of the sum of three Gaussian distributions is applied: However, certain factors could lead to an additional asymmetric broadening of the αpeaks [12]. In the current case of spectroscopy of 222 Rn absorbed in plastic scintillators, we anticipate that the major contribution to the peak asymmetry is the observed in previous studies [6,7] non-uniformity of the photocathode response of the used PMTs.…”
Section: Alpha Spectra Analysismentioning
confidence: 94%
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“…where A is the area of the distribution, µ is its centroid and σ 2 is the variance of the Gaussian distribution. For fitting the α-spectra of 222 Rn and its short-lived progenies, a composite model of the sum of three Gaussian distributions is applied: However, certain factors could lead to an additional asymmetric broadening of the αpeaks [12]. In the current case of spectroscopy of 222 Rn absorbed in plastic scintillators, we anticipate that the major contribution to the peak asymmetry is the observed in previous studies [6,7] non-uniformity of the photocathode response of the used PMTs.…”
Section: Alpha Spectra Analysismentioning
confidence: 94%
“…The problem of finding suitable analytical function to fit the asymmetric α-peaks has been the subject of many studies [13][14][15][16]. An overview and a historical account in the development of analytical function to fit α-spectra from plastic scintillators are given in Chapter 11 in [12]. Here, we propose an improved model for approximating alpha-spectra obtained with plastic scintillators which is based on the Exponentially Modified Gaussian (EMG) distribution.…”
Section: Alpha Spectra Analysismentioning
confidence: 99%