{"title":"BSO 晶体中的二阶电能效应","authors":"María Alejandra Guerrero-V, Jorge-Enrique Rueda-P","doi":"10.1007/s00340-024-08327-5","DOIUrl":null,"url":null,"abstract":"<div><p>Using a non-holographic optical setup, we employed a Mueller–Stokes polarimeter to measure both the linear electro-optic and second-order electrogyration effects. The second-order electrogyration effect was observed in a <span>\\(Bi_{12}SiO_{20}\\)</span> (BSO) crystal with a (110) cut. This response was found for the electric field applied both parallel and perpendicular to the [001] direction, where the values for the second-order electrogyration are <span>\\(4.86\\times 10^{7} \\, \\text {pm}^{2}/\\text {V}^{2}\\)</span> and <span>\\(1.87\\times 10^{7} \\, \\text {pm}^{2}/\\text {V}^{2}\\)</span>, respectively. Additionally, the linear electro-optic coefficient <span>\\(\\gamma _{41}\\)</span> was measured to be <span>\\(1.17 \\, \\text {pm/V}\\)</span> for <span>\\(660.5 \\, \\text {nm}\\)</span>.</p></div>","PeriodicalId":474,"journal":{"name":"Applied Physics B","volume":"130 11","pages":""},"PeriodicalIF":2.0000,"publicationDate":"2024-10-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s00340-024-08327-5.pdf","citationCount":"0","resultStr":"{\"title\":\"Second-order electrogyration effect in BSO crystal\",\"authors\":\"María Alejandra Guerrero-V, Jorge-Enrique Rueda-P\",\"doi\":\"10.1007/s00340-024-08327-5\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>Using a non-holographic optical setup, we employed a Mueller–Stokes polarimeter to measure both the linear electro-optic and second-order electrogyration effects. The second-order electrogyration effect was observed in a <span>\\\\(Bi_{12}SiO_{20}\\\\)</span> (BSO) crystal with a (110) cut. This response was found for the electric field applied both parallel and perpendicular to the [001] direction, where the values for the second-order electrogyration are <span>\\\\(4.86\\\\times 10^{7} \\\\, \\\\text {pm}^{2}/\\\\text {V}^{2}\\\\)</span> and <span>\\\\(1.87\\\\times 10^{7} \\\\, \\\\text {pm}^{2}/\\\\text {V}^{2}\\\\)</span>, respectively. Additionally, the linear electro-optic coefficient <span>\\\\(\\\\gamma _{41}\\\\)</span> was measured to be <span>\\\\(1.17 \\\\, \\\\text {pm/V}\\\\)</span> for <span>\\\\(660.5 \\\\, \\\\text {nm}\\\\)</span>.</p></div>\",\"PeriodicalId\":474,\"journal\":{\"name\":\"Applied Physics B\",\"volume\":\"130 11\",\"pages\":\"\"},\"PeriodicalIF\":2.0000,\"publicationDate\":\"2024-10-20\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://link.springer.com/content/pdf/10.1007/s00340-024-08327-5.pdf\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Applied Physics B\",\"FirstCategoryId\":\"4\",\"ListUrlMain\":\"https://link.springer.com/article/10.1007/s00340-024-08327-5\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"OPTICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Applied Physics B","FirstCategoryId":"4","ListUrlMain":"https://link.springer.com/article/10.1007/s00340-024-08327-5","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"OPTICS","Score":null,"Total":0}
Second-order electrogyration effect in BSO crystal
Using a non-holographic optical setup, we employed a Mueller–Stokes polarimeter to measure both the linear electro-optic and second-order electrogyration effects. The second-order electrogyration effect was observed in a \(Bi_{12}SiO_{20}\) (BSO) crystal with a (110) cut. This response was found for the electric field applied both parallel and perpendicular to the [001] direction, where the values for the second-order electrogyration are \(4.86\times 10^{7} \, \text {pm}^{2}/\text {V}^{2}\) and \(1.87\times 10^{7} \, \text {pm}^{2}/\text {V}^{2}\), respectively. Additionally, the linear electro-optic coefficient \(\gamma _{41}\) was measured to be \(1.17 \, \text {pm/V}\) for \(660.5 \, \text {nm}\).
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