{"title":"二次谐波产生利用轴对称,极化光束与空间变化的椭圆率","authors":"Y. Kozawa, S. Sato","doi":"10.1109/CLEO.2008.4551552","DOIUrl":null,"url":null,"abstract":"Transverse mode conversion by second harmonic generation is demonstrated using focused axially symmetric, polarized beams with spatial variation of ellipticity. Superposition of higher order transverse modes of Hermite-Gaussian or Laguerre-Gaussian beams forms peculiar intensity patterns.","PeriodicalId":6382,"journal":{"name":"2008 Conference on Lasers and Electro-Optics and 2008 Conference on Quantum Electronics and Laser Science","volume":"295 1","pages":"1-2"},"PeriodicalIF":0.0000,"publicationDate":"2008-05-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Second harmonic generation using axially symmetric, polarized beams with spatial variation of ellipticity\",\"authors\":\"Y. Kozawa, S. Sato\",\"doi\":\"10.1109/CLEO.2008.4551552\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Transverse mode conversion by second harmonic generation is demonstrated using focused axially symmetric, polarized beams with spatial variation of ellipticity. Superposition of higher order transverse modes of Hermite-Gaussian or Laguerre-Gaussian beams forms peculiar intensity patterns.\",\"PeriodicalId\":6382,\"journal\":{\"name\":\"2008 Conference on Lasers and Electro-Optics and 2008 Conference on Quantum Electronics and Laser Science\",\"volume\":\"295 1\",\"pages\":\"1-2\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2008-05-04\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2008 Conference on Lasers and Electro-Optics and 2008 Conference on Quantum Electronics and Laser Science\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/CLEO.2008.4551552\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2008 Conference on Lasers and Electro-Optics and 2008 Conference on Quantum Electronics and Laser Science","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CLEO.2008.4551552","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Second harmonic generation using axially symmetric, polarized beams with spatial variation of ellipticity
Transverse mode conversion by second harmonic generation is demonstrated using focused axially symmetric, polarized beams with spatial variation of ellipticity. Superposition of higher order transverse modes of Hermite-Gaussian or Laguerre-Gaussian beams forms peculiar intensity patterns.