UV and thermal poling of germanosilicate fibre

Y. Quiquempois, G. Martinelli, P. Bernage, M. Douay, P. Niay, E. Delevaque, H. Poignant, B. Loisel, J. Bayon
{"title":"UV and thermal poling of germanosilicate fibre","authors":"Y. Quiquempois, G. Martinelli, P. Bernage, M. Douay, P. Niay, E. Delevaque, H. Poignant, B. Loisel, J. Bayon","doi":"10.1364/bgppf.1997.bmg.8","DOIUrl":null,"url":null,"abstract":"The non-zero second order susceptibility obtained by poling a glass is generally explained by the creation of a permanent frozen electric field EDC which breaks the centro-symmetry of the glass. Multiplying the third order susceptibility tensor terms by EDC gives rise to second order non zero terms according to the relation (1) So, after a poling process applied to a fiber, a linear (Pockels) non-zero electrooptic coefficient r333 appears.","PeriodicalId":182420,"journal":{"name":"Bragg Gratings, Photosensitivity, and Poling in Glass Fibers and Waveguides: Applications and Fundamentals","volume":"24 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Bragg Gratings, Photosensitivity, and Poling in Glass Fibers and Waveguides: Applications and Fundamentals","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/bgppf.1997.bmg.8","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

The non-zero second order susceptibility obtained by poling a glass is generally explained by the creation of a permanent frozen electric field EDC which breaks the centro-symmetry of the glass. Multiplying the third order susceptibility tensor terms by EDC gives rise to second order non zero terms according to the relation (1) So, after a poling process applied to a fiber, a linear (Pockels) non-zero electrooptic coefficient r333 appears.
锗硅酸盐纤维的紫外和热极化
通过极化玻璃得到的非零二阶磁化率一般可以用一个永久冻结电场EDC的产生来解释,它破坏了玻璃的中心对称性。将三阶磁化率张量项乘以EDC,根据关系式(1)得到二阶非零项。因此,对光纤进行极化处理后,出现线性(Pockels)非零电光系数r333。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:604180095
Book学术官方微信