Y. Quiquempois, G. Martinelli, P. Bernage, M. Douay, P. Niay, E. Delevaque, H. Poignant, B. Loisel, J. Bayon
{"title":"锗硅酸盐纤维的紫外和热极化","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":"{\"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}","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}
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.
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