OPTICALLY STIMULATED LUMINESCENCE OF AL2O3

Citation
Ms. Akselrod et al., OPTICALLY STIMULATED LUMINESCENCE OF AL2O3, Radiation measurements, 29(3-4), 1998, pp. 391-399
Citations number
25
Categorie Soggetti
Nuclear Sciences & Tecnology
Journal title
ISSN journal
13504487
Volume
29
Issue
3-4
Year of publication
1998
Pages
391 - 399
Database
ISI
SICI code
1350-4487(1998)29:3-4<391:OSLOA>2.0.ZU;2-V
Abstract
Anion-deficient aluminum oxide doped with carbon (Al2O3:C) is not only an extremely sensitive thermoluminescence (TL) material, but is well suited to optically stimulated luminescence OSL applications due to a high cross-section for interaction of light with radiation-induced tra pped charge. Several different OSL readout protocols have been suggest ed, including pulsed OSL (POSL), and ''delayed'' OSL (DOSL). This pape r examines the properties of Al2O3:C for application using these two r eadout protocols. The POSL technique utilizes the prompt luminescence that results from the direct recombination of released charge carriers at luminescence sites (F-centers in Al2O3:C). Following a pulse of st imulation light using a laser, the POSL signal is observed to decay wi th a temperature-independent lifetime of similar to 35-36 ms. The DOSL signal, on the other hand, utilizes the temperature-dependent signal resulting from the capture of released charge carriers by shallow trap s. The decay Of the luminescence component after the stimulating pulse has a lifetime of several hundred ms, depending upon temperature. The dependence of the DOSL signal on readout temperature can be explained in terms of the involvement of the shallow traps in the process. Howe ver, the intensity (not the lifetime) of the POSL signal is also sligh tly temperature dependent. It is conjectured that this may be caused b y a thermally assisted optical detrapping process involving localized excited states. Different forms of Al2O3:C are examined. By modifying both the concentration and energy distribution of the shallow traps ma terial optimized for DOSL applications can be engineered. In contrast, the best material for POSL is grown with no shallow traps. The integr ated light output in a typical POSL measurement is approximately a fac tor of 7-8 greater than that of DOSL, even for a DOSL-quality sample. (C) 1998 Elsevier Science Ltd. All rights reserved.