The luminescence and energy transfer properties of Eu 3ϩ in Y 2 GeO 5 have been investigated. The critical concentration at which the concentration quenching occurred under UV excitation were x ϭ 0.4 in (Y 1Ϫx Eu x ) 2 GeO 5 . To investigate the distinction of photoluminescence behavior of two transitions ͑i.e., 5 D 0 → 7 F 1 and 5 D 0 → 7 F 2 transition͒ for the Eu 3ϩ ion, the decay curves for both 5 D 0 → 7 F 1 and 5 D 0 → 7 F 2 transition have been analyzed. Furthermore the energy migration process of this sample was investigated using Yokota and Tanimoto's formula based on diffusion limited quenching.The (Y 2 O 3 -GeO 2 ) phosphor has recently found an oxide phosphor as a phosphor material for the emitting layer of thin-film electroluminescent ͑TFEL͒ devices. 1,2 Because of high luminous efficiency, (Y 2 O 3 -GeO 2 ):Mn phosphor has been studied as a promising material for TFEL displays as well as plasma display panels and field emission displays. 3 In this view, it seems interesting to study the luminescence of some rare earths in the (Y 2 O 3 -GeO 2 ). Among them, the Eu 3ϩ ion has attracted great attraction due to the application as red phosphors. [4][5][6][7] In this work, we prepared Eu 3ϩ -activated Y 2 GeO 5 phosphor by conventional solid-state reaction and found that this phosphor has a very high critical concentration. Dexter and Schulman, 8 have described that the concentration quenching of the activator is related to cross relaxation and/or energy migration to quenching sites. These phenomena can be due to electromagnetic multipolar interaction or exchange interaction. To obtain insight into the mechanism responsible for the concentration quenching of the Eu 3ϩ emission in this case, we have investigated Y 2 GeO 5 :Eu phosphor over a wide concentration range.
ExperimentalThe powder samples with the general formula (Y 1Ϫx Eu x ) 2 GeO 5 were prepared by the solid-state reaction method. The starting materials used in the preparation of this phosphor were powders of greater purity than 99.99% of Y 2 O 3 , GeO 2 , and Eu 2 O 3 . Preweighed powders were mixed thoroughly in acetone in an agate mortar and dried at 130°C for about 24 h to drive off the solvent and successively heat-treated at several conditions of temperature and duration time, followed by an additional grinding and firing in nitrogen atmosphere. The resulting powders were identified using an X-ray diffraction ͑XRD͒ system with Cu K␣ radiation ͑Ni filter͒. Here, only samples heat-treated at 1500°C for 3 h have been considered.The excitation and emission spectra of the fired samples were measured using a Perkin-Elmer LS-50 luminescence spectrometer with a xenon flash lamp (⌬v 1/2 ϭ 10 s). The decay measurement was performed at 594 nm emission for 5 D 0 → 7 F 1 transition and 611 nm emission for 5 D 0 → 7 F 2 transition, respectively. The pumping source was 254 nm and the pulse duration was 6 ns.
Results and DiscussionIn the XRD patterns of the Y 2 GeO 5 powders heat-treated with different amounts of Eu 3ϩ , most peaks correspond to the Y 2 ...