Glass Division, Glass Science and Technology Section, CSIR-Central Glass and Ceramic Research Institute, 196, Raja S.C. Mullick Road, Kolkata 700 032, India.
Spectrochim Acta A Mol Biomol Spectrosc. 2013 Aug;112:301-8. doi: 10.1016/j.saa.2013.04.062. Epub 2013 Apr 22.
In this work, a new and non-conventional oxide glass composition based on Bi2O3-GeO2-ZnO system has been formulated with an aim to realize low phonon oxide glass and elucidate its performance when co-doped with Ho(3+)/Yb(3+) for the energy transfer based NIR emission at 2 μm from Ho(3+) ions under Yb(3+) excitation. The glass with 1.0 mol% Ho2O3 and 0.5 mol% Yb2O3 has exhibited maximum energy transfer rate (3602 s(-1)) and energy transfer efficiency (65.92%). Important radiative properties have been predicted for emission transitions of Ho(3+) ions using intensity parameters derived from measured absorption spectra using standard Judd-Ofelt theory. At lower acceptor ion concentration (0.1 mol%), an efficient NIR to visible up-conversion emission has been observed based on two photon absorption process which has found to be reduced significantly at higher Ho(3+) concentrations with simultaneous enhancement in 2 μm emission. Hence, this newly developed glass codoped with Yb(3+)/Ho(3+) is promising glass for sensitized 2 μm emission applications as broad band tunable lasers because of the combination of low phonon energy (707 cm(-1)), high energy transfer efficiency, moderately high emission cross-section (5.33×10(-21) cm(2)) and larger effective half-width of the emission band value of 169 nm.
在这项工作中,我们提出了一种新的非传统的基于 Bi2O3-GeO2-ZnO 系统的氧化物玻璃组成,旨在实现低声子氧化物玻璃,并阐明其在共掺 Ho(3+)/Yb(3+)时的性能,以便在 Yb(3+)激发下实现来自 Ho(3+)离子的基于能量转移的 2μm 近红外发射。在含有 1.0 mol% Ho2O3 和 0.5 mol% Yb2O3 的玻璃中,表现出最大的能量转移速率(3602 s(-1)) 和能量转移效率(65.92%)。使用标准的 Judd-Ofelt 理论,从测量的吸收光谱中导出强度参数,预测了 Ho(3+)离子发射跃迁的重要辐射特性。在较低的受体离子浓度(0.1 mol%)下,观察到基于双光子吸收过程的有效近红外到可见光上转换发射,随着 Ho(3+)浓度的增加,这种上转换发射显著降低,同时 2μm 发射增强。因此,这种新开发的共掺 Yb(3+)/Ho(3+)玻璃有望用于敏化 2μm 发射应用,因为它具有低声子能量(707 cm(-1))、高能量转移效率、中等发射截面(5.33×10(-21) cm(2)))和较大的发射带宽有效半宽值 169nm。