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M. Jain, A. Murray, L. Bøtter-Jensen (2003)
Characterisation of blue-light stimulated luminescence components in different quartz samples: implications for dose measurementRadiation Measurements, 37
A. Wintle, A. Murray (2006)
A review of quartz optically stimulated luminescence characteristics and their relevance in single-aliquot regeneration dating protocolsRadiation Measurements, 41
A. Murray, A. Wintle (1999)
Isothermal decay of optically stimulated luminescence in quartzRadiation Measurements, 30
Jeong-Heon Choi, G. Duller, A. Wintle (2006)
Analysis of quartz LM-OSL curves
(2006)
Thoughts arising from “Choi
N. Kıyak, T. Canel (2006)
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Single aliquot dating of ceramics by green light stimulation of luminescence from quartzNuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms, 132
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Partial bleaching and the decay form characteristics of quartz OSLRadiation Measurements, 27
J. Wallinga, A. Bos, G. Duller (2008)
On the separation of quartz OSL signal components using different stimulation modesRadiation Measurements, 43
C. Kuhns, N. Larsen, S. McKeever (2000)
Characteristics of LM-OSL from several different types of quartzRadiation Measurements, 32
G. Polymeris, D. Afouxenidis, N. Tsirliganis, G. Kitis (2009)
The TL and room temperature OSL properties of the glow peak at 110°C in natural milky quartz:a case studyRadiation Measurements, 44
G. Kitisa, V. Pagonisb (2008)
Computerized curve deconvolution analysis for LM-OSL
(2007)
Component resolved OSL
N. Kıyak, G. Polymeris, G. Kitis (2008)
LM-OSL thermal activation curves of quartz: Relevance to the thermal activation of the 110 °C TL glow-peakRadiation Measurements, 43
M. Chithambo, R. Galloway (2001)
On the slow component of luminescence stimulated from quartz by pulsed blue light-emitting diodesNuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms, 183
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(2006)
Thoughts arising from “ Choi , Duller and Wintle : Analysis of quartz LM-OSL curves . Ancient TL 24 , 9-20 ( 2006 ) ”
N. Poolton, L. Bøtter-Jensen, C. Andersen, M. Jain, A. Murray, A. Malins, F. Quinn (2003)
Measuring modulated luminescence using non-modulated stimulation: ramping the sample periodRadiation Measurements, 37
G. Polymeris, N. Kıyak, G. Kitis (2008)
Component Resolved IR Bleaching Study of the Blue LM-OSL Signal of Various Quartz Samples, 32
N. Kıyak, G. Polymeris, G. Kitis (2007)
Component resolved OSL dose response and sensitization of various sedimentary quartz samplesRadiation Measurements, 42
G. Kitis, C. Furetta, V. Pagonis (2009)
MIXED-ORDER KINETICS MODEL FOR OPTICALLY STIMULATED LUMINESCENCEModern Physics Letters B, 23
G. Polymeris, N. Tsirliganis, Z. Loukou, G. Kitis (2006)
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J. Singarayer, R. Bailey (2003)
Further investigations of the quartz optically stimulated luminescence components using linear modulationRadiation Measurements, 37
N. Kiyaka, T. Canelb (2006)
Equivalent dose in quartz from young samples using the SAR protocol and the effect of preheat temperature
E. Bulur (1996)
An alternative technique for optically stimulated luminescence (OSL) experimentRadiation Measurements, 26
J. Singarayer, R. Bailey (2004)
Component-resolved bleaching spectra of quartz optically stimulated luminescence: preliminary results and implications for datingRadiation Measurements, 38
E. Bulur, L. Bøtter-Jensen, A. Murray (2000)
Optically stimulated luminescence from quartz measured using the linear modulation techniqueRadiation Measurements, 32
A. Wintle, A. Murray (1999)
Luminescence sensitivity changes in quartzRadiation Measurements, 30
M. Jain, L. Lindvold (2007)
Blue light stimulation and Linearly Modulated Optically Stimulated Luminescence
The present paper presents a comparative experimental study of two commonly measured Optically Stimulated Luminescence (OSL) signals in quartz. The experimental study measures both the continuous wave OSL (CW-OSL) and the linearly modulated (LM-OSL) signals from the same quartz sample for a range of stimulation temperatures between 180 and 280°C, while the former is transformed to pseudo LM-OSL (ps LM-OSL). A computerized deconvolution curve analysis of the LM-OSL and ps LM-OSL signals was carried out, and the contributions of several OSL components to the initial OSL signal (0.1 s) were shown to be independent of the stimulation temperature used during the measurement. It was also found that the composite OSL (0.1 s) signal consists mainly of the first two OSL components present in the OSL curves. The equivalence of the ps LM-OSL (transformed CW-OSL) and of LM-OSL measurements was also examined by an appropriate choice of the experimental stimulation times, and of the stimulation power of the blue LEDs used during the measurement.
Geochronometria – Springer Journals
Published: May 25, 2011
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