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Natural and laboratory OSL growth curve–Verification of the basic assumption of luminescence dating
Institution:1. Département des sciences de la Terre et de l''atmosphère, Université du Québec à Montréal, CP 8888 Succ. Centre-Ville, Montréal, Qc H3C 3P8, Canada;2. IRAMAT-CRP2A, UMR 5060 CNRS – Université de Bordeaux3 – Maison de l’Archéologie, 33607 Pessac, France;1. GADAM Centre, Institute of Physics – Centre for Science and Education, Silesian University of Technology, ul. Konarskiego 22B, 44-100 Gliwice, Poland;2. Institute of Geography, University of Bern, Hallerstrasse 12, 3012 Bern, Switzerland;1. Instituto de Física Arroyo Seco – CIFICEN (CONICET – UNCPBA), Pinto 399, 7000 Tandil, Argentina;2. Facultad de Ingeniería – CIFICEN (CONICET – UNCPBA), Av. del Valle 5737, 7400 Olavarría, Argentina;3. Autoridad Regulatoria Nuclear (ARN), Av. Del Libertador 8250, 1429 Buenos Aires, Argentina;4. Comisión de Investigaciones Científicas de la Provincia de Buenos Aires, 1900 La Plata, Argentina;1. Health and Safety Group, Bhabha Atomic Research Center, Mumbai 400085, India;2. Physics Department, McDaniel College, Westminster, MD 21157, USA;3. Physics Group, Bhabha Atomic Research Center, Mumbai 400085, India
Abstract:The basic assumption of luminescence dating is the equality between the growth curve of OSL generated by the natural radiation and the OSL growth curve reconstructed in laboratory conditions. The dose rates that generate the OSL in nature and in laboratory experiments differ by about ten orders of magnitude. Recently some discrepancies between the natural and laboratory growth curves have been observed. It is important to establish their reasons in order to introduce appropriate correction into the OSL dating protocol or to find a test that allows to eliminate the samples which should not be used for dating. For this purpose, both growth curves, natural and laboratory, were reconstructed by means of computer simulations of the processes occurring in the sample during its deposition time in environment as well as those which occur in a laboratory during dating procedure. The simulations were carried out for three models including one shallow trap, two OSL traps, one disconnected deep and one luminescence center. The OSL model for quartz can be more complex than the one used in the presented simulations, but in spite of that the results show effects of growth curves discrepancies similar to those observed in experiments. It is clear that the consistency of growth curves is not a general feature of the OSL processes, but rather a result of an advantageous configuration of trap parameters. The deep disconnected traps play the key role and their complete filling before the zeroing of OSL signal is a necessary condition of the growth curves' consistency.
Keywords:Luminescence dating  OSL growth curve  Computer simulations
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