| The Dy3+ doping Y2O3/Gd2O3 phosphors were obtained through precursor synthesis via carbonate homogeneous precipitation using rare earth nitrates as mother salt and urea as precipitating agent, followed by calcination at 600-1300 ℃. The synthesis, particle size control, crystal structure stabilization, fluorescence properties and energy transfer studied systematically in a wide range(Dy/Ln=0-10 at%, Ln=Y+Gd+Dy). The following main conclusions have been reached:(1) The monodisperse spherical (Y1-xDyx)2O3 precursor particles were synthesized by homogeneous precipitation technique. From which it can be seen that all the precursors were amorphous with approximate composition of(Y1-xDyx)(OH)(CO3)·1.4H2O whose size can be controlled by adjusting the urea content. The phase pure(Y1-xDyx)2O3 can be obtained by annealing at 600 ℃, and the monodisperse spherical morphology can be kept even at higher temperature of 1000 ℃, while the spherical morphology was destroyed when the calcination temperature increases up to 1200 ℃. The(Y1-xDyx)2O3 phosphor particles exhibit strong yellow emission and weak blue emission(corresponding to 4F9/2→6H13/2 and 4F9/2→6H15/2 transition of Dy3+ respectively) upon UV excitation at 352 nm(6H15/2→6P7/2 transition of Dy3+). The luminescent property of the phosphors can be improved with the temperature increasing and the quenching concentration of Dy3+ is found to be 2 at%.(2) The monodisperse spherical(Gd1-xDyx)2O3 precursor particles were synthesized by homogeneous precipitation technique. All the precursors were amorphous with approximate composition of(Gd1-xDyx)(OH)(CO3)·1.3H2O. The precursor particle size can be controlled by adjusting the urea content and partially replacing deionized water with organic solvent as the reaction solution. The(Gd1-xDyx)2O3 phosphor particles exhibit strong yellow emission and weak blue emission(corresponding to 4F9/2→6H13/2 and 4F9/2→6H15/2 transition of Dy3+ respectively) upon UV excitation at 275 nm(8S7/2→6IJ transition of Gd3+) and the quenching concentration of Dy3+ is found to be 2 at%. Owing to the energy transfer of Gd3+→Dy3+ the fluorescence intensity of the phosphor was significantly improved, and increased with the calcination temperature increasing. Fluorescence decay for the 575 nm emission of(Gd1-xDyx)2O3 reduced gradually with the Dy3+ content and calcination temperature increasing. The former is mainly due to the energy transfer between Dy3+, while the latter is attributed to the improved crystallinity of phosphor particles. A cubic phase to monoclinic phase transition of Gd2O3 was found when the calcination temperature was fixed at 1300 ℃. Based on this, doping with smaller ionic radius Y3+ was proposed to stabilize the lattice structure of Gd2O3 and the minimum doping amount was determined to be 5 at%.(3) The monodisperse spherical [(YyGd1-y)1-xDyx]2O3 precursor particles were synthesized by homogeneous precipitation technique. All precursors were amorphous with approximate composition of [(YyGd1-y)1-xDyx](OH)(CO3)·1.5H2O. All precursors have good monodisperse spherical morphology and the morphology can be kept even at higher temperature of 1000 ℃. The differential precipitation of Y3+ and Gd3+ was found by TG analysis. The [(YyGd1-y)1-xDyx]2O3 phosphor particles exhibit strong yellow emission(4F9/2→6H13/2 transition of Dy3+) upon UV excitation at 275 nm(8S7/2→6IJ transition of Gd3+), and the yellow emission intensity is stronger than that of blue emission. The high efficient energy transfer between Gd3+→Dy3+ can improve the fluorescence properties of phosphors, which can be defined by the comparison of [(Yy Gd1-y)0.98Dy0.02]2O3 and(Y0.98Dy0.02)2O3. |