The study of the luminescence properties of rare earth doped systems historically focuses on systems which exhibit strong luminescence. More recently, extensive studies on materials with high quantum effrciency are in part motivated b y the search for new plosplor and scintillator materials. However, a thorough study of certain systems which show very low quantum yield will certainly lead to a better understanding of phosphor materials and rare earth systems in general. As an example of recent studies which address both the fundamental question of relaxation processes in rare earth doped systems and phosphor applications we present studies on cerium-doped lutetium oxide crystals which are characterized by a compJete quenching of the 5d-4f luminnescence and compare its optical properties to that of very efficient cerium doped phosphor material, lutetium oxyorthosilicate. To find the mechanisms which lead to the different quantum efficiency in these systems, extensive absorption, photoexcitation and photoconductivity studies were performed on singłe crystals. We demonstrate that the radically different emission properties of the investigated systems originate in smaJl but crucial differences in the location of the emitting 5d level of the cerium ion with respect to the conduction band of the host -a general result which can be applied to a broad range of materials.PACS numbers: 72.40.-+, 78.50.Ec, 78.55.Hx
IntroduttionMaterials doped with Ce3 + have attracted the interest of solid state researchers since the early sixties, and most papers focus on the application of these materials as phosphors or scintillators [1]. Despite of more than 30 years of research, one crucial question has not been fully answered: i.e., why do seemingly similar Ce-doped systems show drastically different luminescence properties, ranging from quantum efficiencies of nearly 100% to systems where the luminescence is completely quenched.High quantum efficiencies can be understood easily in terms of the electronic structure of trivalent cerium: the simple electron configuration 4f 1 leads (257)