OPTICAL SPECTROSCOPY AND SCINTILLATION MECHANISMS OF CE(X)LA(1-X)F3

Citation
Aj. Wojtowicz et al., OPTICAL SPECTROSCOPY AND SCINTILLATION MECHANISMS OF CE(X)LA(1-X)F3, Physical review. B, Condensed matter, 49(21), 1994, pp. 14880-14895
Citations number
60
Categorie Soggetti
Physics, Condensed Matter
ISSN journal
01631829
Volume
49
Issue
21
Year of publication
1994
Pages
14880 - 14895
Database
ISI
SICI code
0163-1829(1994)49:21<14880:OSASMO>2.0.ZU;2-B
Abstract
In this paper we present spectroscopic and scintillation studies of mi xed cerium lanthanum trifluoride crystals CexLa1-xF3. A scintillation mechanism is proposed in which the light output of the CexLa1-xF3 scin tillator is determined by three processes: a direct excitation of Ce3 ions by secondary electrons and x rays, an ionization of Ce3+ ions fo llowed by the capture of electrons and formation of Ce bound excitons and, eventually, a transfer of the energy from the electronic-lattice excitations to Ce3+ ions. These three processes occur in various degre es in all inorganic Ce scintillators, and the mixed (Ce,La) trifluorid es provide, therefore, an excellent example of their relative importan ce. The peculiarity of fluorides is that Ce3+ ions occur in regular an d ''perturbed'' sites. The lack of a fast energy migration between the Ce ions and, at the same time, an efficient energy transfer to ''pert urbed'' Ce ions lead to nonexponential decays of the Ce emission. Ther mal quenching is moderate and radiation trapping can be minimized, and there is no evidence of luminescence concentration quenching. The lig ht output under gamma excitation has a maximum value of about 4500 pho tons per MeV, which is significantly lower than the estimated conversi on-limited value of about 25 000 photons per MeV. It is suggested that the stable Ce2+ provides electron traps, competing for electrons with holes localized on F2- and Ce4+ ions. Therefore, mostly one process, namely the direct excitation of Ce3+ ions by secondary electrons and p hotons, contributes to the light output of CeF3. The deomonstrated fea sibility of reducing perturbed Ce makes it a strong contender in those applications where high speed, not high light output, is of prime con cern.