摘要
在 98 0nm半导体激光激发下 ,在Er3+ Yb3+ Tm3+ 共掺玻璃样品中得到了如下的 5条较强的上转换荧光带 ,分别是近红外 (80 0nm) ,红 (6 4 5nm) ,绿 (5 4 5和 5 2 5nm) ,蓝 (4 80nm)及紫 (4 0 7nm)。与Er3+ Yb3+ 共掺样品相比 ,Tm3+ 的加入使得 4 80nm的蓝光显著增强 ,这应与Tm3+ 特殊的能级结构有关 ;荧光强度随激发功率变化的双对数曲线表明 4 80nm蓝光发射是双光子激发过程 ,为两个Yb3+ 的合作上转换敏化发光 ,随着激发功率的增加 ,4 80nm荧光的logI logP曲线的斜率将变小 ,逐渐向下“弯曲”。作者详细的分析了各条荧光带的上转换机制 ;并用速率方程讨论了稳态情况下 4 80nm蓝色上转换荧光强度随激发功率变化的关系 ,其结果与实验一致。
Under 980 nm excitation, we obtained five intense up-conversion luminescence bands in Er 3+-Yb 3+-Tm 3+co-doped CdF 2:PbF 2-based glass as follows: infrared(800 nm), red(645 nm), green (545 nm and 525 nm), blue(480 nm ) and violet(407 nm) up-conversion luminescence. With the addition of Tm 3+, the intensity of 480 nm blue luminescence increased notably compared with that of co-doped Yb 3+-Er 3+ sample, which attributed to Tm 3+ special energy level structure; logI-logP plot of the luminescence intensity versus pump power shows that 480 nm luminescence emission is a two-photon excitation process induced by the cooperative up-conversion between two Yb 3+ ions and the slope of logI-logP plot decreases gradually with increasing pump power and shows a tendency to bend down. The up-conversion mechanism is analyzed in detail under 980 nm semiconductor laser excitation; the dependence of 480 nm up-conversion luminescence intensity on the pump power under the steady states is discussed by using rate equation and the results agree well with the experiments.
出处
《光谱学与光谱分析》
SCIE
EI
CAS
CSCD
北大核心
2004年第7期779-783,共5页
Spectroscopy and Spectral Analysis
基金
国家"8 63"课题 (2 0 0 2 32 4 0 30 )资助