2005
DOI: 10.1080/10420150500331438
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Simulation of competing irradiation and fading effects in thermoluminescence dosimetry

Abstract: The aim of this article is to give some useful expressions for fading correction in practical situations as they can be encountered in radiation protection dosimetry monitoring, i.e. personal, environmental and clinical dosimetry. They are obtained considering the general case in which, for both first and second-order kinetics, during the experimental period of time two effects are in competition between them: one is the trapping rate due to the irradiation, the second is the detrapping rate which takes place … Show more

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Cited by 5 publications
(3 citation statements)
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“…Considering initial irradiation of samples followed by fading at room temperature and assuming first-order kinetics, for a storage time ts>>ti (irradiation time), following expression simulated this case is (Kitis et al, 2005;Gomez-Ros et al, 1996): Φ = Φ0exp(-pt) and then p = (-1/t)ln(Φ/Φ0), where Φ can be considered integrated glow curve or peak area. So by taking into account at final 42 days of fading; p = 0.149 d -1 or 14.9 % lost per day of TL signal for ZnO, and 15.9 % for ZnO:Tb.…”
Section: Fading Of the Tl Signalsmentioning
confidence: 99%
“…Considering initial irradiation of samples followed by fading at room temperature and assuming first-order kinetics, for a storage time ts>>ti (irradiation time), following expression simulated this case is (Kitis et al, 2005;Gomez-Ros et al, 1996): Φ = Φ0exp(-pt) and then p = (-1/t)ln(Φ/Φ0), where Φ can be considered integrated glow curve or peak area. So by taking into account at final 42 days of fading; p = 0.149 d -1 or 14.9 % lost per day of TL signal for ZnO, and 15.9 % for ZnO:Tb.…”
Section: Fading Of the Tl Signalsmentioning
confidence: 99%
“…Levels N (cm -3 ) E (eV) s (s -1 ) A (cm 3 s -1 ) B (cm 3 s -1 ) 1.75 2.510 14 5.010 -10 0.0  i 5.010 13 2.00 1.010 10 1.010 -10 0.0 8  i 3.010 11 1.43 5.010 13 5.010 -7 5.010 -9 9  i 1.010 13 1.75 5.010 14 1.010 -9 5.010 -10 10  i 1.010 14 5.00 1.010 13 1.010 -9 1.010 -10 11  i 5.010 12 5.00 1.010 13 1.010 -10 1.010 -10…”
Section: Fig 2(a)unclassified
“…Another approach towards understanding the complex nature of quartz is by way of simulation/modelling. This has proved very viable in explaining many luminescent phenomena for various materials generally [4,5,6,12,14,25,26]. This process is something identical to virtually synthetizing, say, a TL material with some predetermined properties and subsequently subjecting it to traditional experimental procedures numerically.…”
Section: Introductionmentioning
confidence: 99%