2015
DOI: 10.1016/j.radmeas.2015.09.006
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Time and dose-rate dependence of TL and OSL due to competition between excitation and fading

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Cited by 10 publications
(2 citation statements)
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“…It is also observed that the signal registered with the highest dose-rate (β source) is more dominant for the first peak of Z and ReS samples than for the 330 °C and sensitized peak. The findings of peak intensities at 330 °C and the sensitized peak summarized in Table 2 are in agreement with Valladas and Ferreira [9]. The authors studied rock crystal (hyaline) samples annealed at 600 °C using two radiation sources with dose-rate of 1.33×10 -4 Gy/s ( 137 Cs) and 0.15 Gy/s ( 60 Co).…”
Section: Kinetic Analysissupporting
confidence: 87%
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“…It is also observed that the signal registered with the highest dose-rate (β source) is more dominant for the first peak of Z and ReS samples than for the 330 °C and sensitized peak. The findings of peak intensities at 330 °C and the sensitized peak summarized in Table 2 are in agreement with Valladas and Ferreira [9]. The authors studied rock crystal (hyaline) samples annealed at 600 °C using two radiation sources with dose-rate of 1.33×10 -4 Gy/s ( 137 Cs) and 0.15 Gy/s ( 60 Co).…”
Section: Kinetic Analysissupporting
confidence: 87%
“…The overall analysis of dose-rate effects in some luminescent materials suggested that the TL response as a function of the dose is not completely independent from the dose-rate. In the case of quartz, it was also noticed that the TL emissions related to high temperature glow peaks change differently with the increase of the dose-rate [7,9]. Another study showed that the variation of the dose-rate from 1.4x10 -3 to 3.3 Gy/s caused a decrease in TL signal in a factor of five in powdered samples of Brazilian quartz irradiated with 60 Co γ rays [5].…”
Section: Introductionmentioning
confidence: 99%