首页 | 本学科首页   官方微博 | 高级检索  
     检索      

用不同强度皮秒脉冲相关技术测量甲酚紫吸收恢复时间
引用本文:刘俊业,李多录.用不同强度皮秒脉冲相关技术测量甲酚紫吸收恢复时间[J].发光学报,1992,13(1):21-25.
作者姓名:刘俊业  李多录
作者单位:中国科学院长春物理研究所激发态物理开放实验室, 长春 130021
基金项目:国家自然科学基金;激发态物理开放实验室基金
摘    要:以Ar+离子锁模激光器同步泵浦R6G染料激光器作光源,用不同强度皮秒脉冲相关的泵涌—探测技术测得甲酚紫甲醇溶液的吸收恢复时间为162±3.5ps.并且用三能级模型对这一动力学过程进行了理论分析.

关 键 词:皮秒脉冲  泵浦  染料  吸收恢复  测量

MEASUREMENT OF ABSORPTION RECOVERY TIME OF CRESYL VIOLET BY CORRELATION TECHNIQUE OF PICOSECOND PULSES WITH DIFFERENT INTENSITIES
Liu Junye,Li Duolu,Jin Zhouzhe,Jin Chunming,Huang Shihua,Yu Jiaqi.MEASUREMENT OF ABSORPTION RECOVERY TIME OF CRESYL VIOLET BY CORRELATION TECHNIQUE OF PICOSECOND PULSES WITH DIFFERENT INTENSITIES[J].Chinese Journal of Luminescence,1992,13(1):21-25.
Authors:Liu Junye  Li Duolu  Jin Zhouzhe  Jin Chunming  Huang Shihua  Yu Jiaqi
Institution:Laboratory of Excited State Processes, Changchun Institute of Physics, Academia Sinica, Changchun 130021
Abstract:As a transform-limited light source, we used a pulsed Rh6G dye laser synchronously pumped by a mode locked Ar+ lasar with, a repetition rate of 82 MHz. The operation wavelength was 514.5nm. The dye laser was tuned to 590 nm which was nearly the peak of the absorption spectrum of cresyl violet in methanol solution. The single mode-locked pulse duration, tp was 3 ps. The output beam of dye laser was split into two beams or the pump beam and the probe beam. The ratio of intensity between them was about 100:1. The light-spot-rodius ratio of the pump beam to the probu was 3:1. It means that the probe beam fell inside the pump beam on the sample. The energy change in the probe boam induced by the pump beam was selectively picked up by a lock-in amplifier.The dynamic equation to describe the absorption racovoiy process can be written as follows dN3(t)/dt=B&(t)N0-N3(t)/τ3 (1) dN2(t)/dt=N3(t)/τ32-N2(t)/τ21 (2) where N0 is the population in the ground state at t= 0. N3(t) and N2(t) arc the transient population in |3 >and|2 >state, respectively. B is a constant relating to the absorption cross suction σ13. Wo resolved eqs. (1) and (2) using N3(0)=N2(0)=0 , then N2(t)∝expτ21) can bo derived. Fitting the experimental data (curve a sea Fig. 4) with those calculated by eq. (3) (curve b), we got the absorption recovery time τ21=162 ps.
Keywords:
本文献已被 CNKI 维普 等数据库收录!
点击此处可从《发光学报》浏览原始摘要信息
点击此处可从《发光学报》下载免费的PDF全文
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号