Time-resolved Z-scan and thermal lens measurements in Er+3 and Nd+3 doped fluoroindate glasses

被引:34
作者
Catunda, T
Baesso, ML
Messaddeq, Y
Aegerter, MA
机构
[1] UNIV NACL ESTADUAL SAO PAULO, INST QUIM, BR-14800900 ARARAQUARA, SP, BRAZIL
[2] UNIV SAO PAULO, INST FIS SAO CARLOS, BR-13560970 SAO CARLOS, SP, BRAZIL
[3] UNIV ESTADUAL MARINGA, DEPT FIS, BR-87020900 MARINGA, PARANA, BRAZIL
[4] UNIV SAARLAND, INST NEUE MAT, D-66123 SAARBRUCKEN, GERMANY
基金
巴西圣保罗研究基金会;
关键词
D O I
10.1016/S0022-3093(97)00055-0
中图分类号
TQ174 [陶瓷工业]; TB3 [工程材料学];
学科分类号
0805 ; 080502 ;
摘要
In rare earth ion doped solids, a resonant non-linear refractive index, n(2), appears when the laser pumps one of the ion excited states and the refractive index change is proportional to the excited state population. In these solids there an usually thermal and non-thermal lensing effects, where the non-thermal one is due to the polarizability difference, Delta alpha, between excited and ground states of the ions. We have used the time resolved Z-scan and a mode-mismatched thermal lens technique with Ar+ ion laser in Er+3 (20ZnF(2)-20SrF(2)-2NaF-16BaF(2)-6GaF(3)-(36 - x)InF3-xErF(3), with x = 1, 2, 3 and 4 mol%) and Nd+3 (20SrF(2)-16BaF(2)-20ZnF(2)-2GdF(3)-2NaF-(40 - x)InF3-xNdF(3), with x = 0.1, 0.25, 0.5-1 mol%) doped fluoroindate glasses, In both samples we found that the non-linear refraction is due to the thermal effect, while the non-thermal effect is negligible. This result indicates that in fluoride glasses Delta alpha is very small (less than 10(-26) cm(3)). We also measured the imaginary part of the non-linear refractive index (n(2) '') due to absorption saturation.
引用
收藏
页码:225 / 230
页数:6
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