2016
DOI: 10.1016/j.apradiso.2015.10.019
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Validation of energy-weighted algorithm for radiation portal monitor using plastic scintillator

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Cited by 20 publications
(11 citation statements)
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“…In case of 137 Cs having a Compton edge at 0.477 MeV theoretically, it was already observed that the peak of the energyweighted spectrum that originated from the Compton maximum was a feature for nuclide identification in previous studies. Similarly, 60 Co having a clear Compton maximum of the energy spectrum at 1.041 MeV also exhibited a discernable peak in the energy-weighted spectrum [8][9][10][11]. Figs.…”
Section: Spectrum Analysis Of Moving Sourcesmentioning
confidence: 76%
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“…In case of 137 Cs having a Compton edge at 0.477 MeV theoretically, it was already observed that the peak of the energyweighted spectrum that originated from the Compton maximum was a feature for nuclide identification in previous studies. Similarly, 60 Co having a clear Compton maximum of the energy spectrum at 1.041 MeV also exhibited a discernable peak in the energy-weighted spectrum [8][9][10][11]. Figs.…”
Section: Spectrum Analysis Of Moving Sourcesmentioning
confidence: 76%
“…The energy-weighted algorithm proposed in the previous studies multiplies the counts in each energy bin and the energy corresponding to the same channel (in the form of a coefficient) using the following equation: (1) where is the energy-weighted count of the energy spectrum's i th bin, is the original optical photon count in the i th bin, and is the energy coefficient in the i th bin [8][9][10][11]. Applying the equation, it was observed that the increased area, such as the Compton maximum of the gamma energy spectrum measured by the plastic scintillator, was converted into an identifiable peak as shown in Fig.…”
Section: Improvement Of Energy-weighted Algorithmmentioning
confidence: 99%
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“…A simpler method identifies isotopes by finding peaks in the energy/channel weighted spectra, which occur at the point of the Compton edge for isotopes with significant Compton continuums, such as 137 Cs, hence characteristic photopeak energies can be calculated using the Compton scattering equation [76]. In isotopes where the spectra contains multiple low-energy γs and there exists no readily discernable Compton edge, such is the case with 238 U, there still exists a characteristic peak in the energy weighted spectrum which can be determined experimentally.…”
Section: Source Characterisation Based On Energy Considerationsmentioning
confidence: 99%
“…Therefore, various spectral processing techniques have been reported for pseudo gamma spectroscopy of plastic scintillation detectors. Energy windowing [1][2][3][4], F-score analysis [5], energy weighted algorithms [6,7], and inverse matrix [8] are representative methods for pseudo gamma spectroscopy. However, these methods can be categorized as indirect pseudo gamma spectroscopic methods because it is impossible to directly identify the energy of incident gamma rays.…”
Section: Introductionmentioning
confidence: 99%