980nm脉冲激发下Er^(3+)掺杂材料中~4I_(13/2)→~4I_(15/2)跃迁的瞬态行为(英文)  

Transient Behavior of the Emission ~4I_(13/2)→~4I_(15/2) in Er^(3+) Doped Material under 980 nm-pulsed Excitation

作　　者：张国有[1] 

机构地区：[1]内蒙古民族大学,内蒙古通辽028043

出　　处：《发光学报》2005年第1期47-50,共4页Chinese Journal of Luminescence

基　　金：国家自然科学基金资助项目(50172046,50102006)~~

摘　　要：在过去的几十年人们对Er3+掺杂的玻璃材料进行了广泛的研究,因为Er3+的 4I13 /2→ 4I15 /2跃迁能够给出适合红外光通讯窗口的 1. 5μm的发射。据我们所知,目前关于脉冲激光激发下Er3+掺杂材料 1. 5μm发射的动力学行为研究报道仍很少。我们引入了转移函数理论,研究了 980nm脉冲激发下Er3+的 4I13 /2能级荧光的动力学行为。发现在 980nm脉冲激发后,其荧光衰减遵循双指数规律,4I13 /2能级布居分为指数上升和指数下降两个过程。In the last decades, much attention has been paid to the Er^(3+) doped glass materials since it is widely known that the transition ()~4I_(13/2)→()~4I_(15/2) of Er^(3+) can give an emission peaking around 1.5 μm, which matches the IR optical communication window. To our knowledge there are very few of investigations on the dynamics of 1.5 μm (emission) of Er^(3+). The transfer function theory is introduced to investigate transient fluorescent behavior of the transition ()~4I_(13/2)→()~4I_(15/2) in the Er^(3+) doped materials under 980 nm-pulsed excitation. A mathematical expression for the temporal emission evolution is given. It is found that after having been excited by 980 nm δ-pulse the luminescence decay of level ()~4I_(13/2) obeys double exponential function law, and the variation of population of the level ()~4I_(13/2) has two stages: rise-stage and set-stage.

关 键 词：Er^3+掺杂材料 转移函数 瞬态荧光特性 

分 类 号：O482.31[理学—固体物理]