{"title":"pts -聚二乙炔非共振非线性折射率的基本机理","authors":"R. Quintero-Torres, M. Thakur","doi":"10.1364/otfa.1997.wc.3","DOIUrl":null,"url":null,"abstract":"Polydiacetylene single crystal, PTS, is known to have the largest off-resonant nonlinear refractive index (n2). Recently we have demonstrated picosecond all-optical switching using PTS-polydiacetylene in a Fabry-Perot cavity1. This measurement was performed using a pump-probe technique with 90ps pulses at 1.06μm wavelength. In that measurement, besides demonstrating a large modulation depth, we showed that the sign of n2 was negative. In another work, however, a positive sign for n2 was reported from a z-scan measurement2 and two photon resonances were used to explain the positive sign and the off-resonant nonlinear optical processes in PTS. In this work we have made detailed measurements of the sign using Michelson interferometry and z-scan. These and previous measurements using pump-probe technique at different off-resonant wavelengths show that the sign of n2 of PTS is negative over the wavelength of 650 - 1064nm.","PeriodicalId":378320,"journal":{"name":"Organic Thin Films for Photonics Applications","volume":"8 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Basic Mechanisms involved in the Off-resonant Nonlinear Refractive Index of PTS-Polydiacetylene\",\"authors\":\"R. Quintero-Torres, M. Thakur\",\"doi\":\"10.1364/otfa.1997.wc.3\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Polydiacetylene single crystal, PTS, is known to have the largest off-resonant nonlinear refractive index (n2). Recently we have demonstrated picosecond all-optical switching using PTS-polydiacetylene in a Fabry-Perot cavity1. This measurement was performed using a pump-probe technique with 90ps pulses at 1.06μm wavelength. In that measurement, besides demonstrating a large modulation depth, we showed that the sign of n2 was negative. In another work, however, a positive sign for n2 was reported from a z-scan measurement2 and two photon resonances were used to explain the positive sign and the off-resonant nonlinear optical processes in PTS. In this work we have made detailed measurements of the sign using Michelson interferometry and z-scan. These and previous measurements using pump-probe technique at different off-resonant wavelengths show that the sign of n2 of PTS is negative over the wavelength of 650 - 1064nm.\",\"PeriodicalId\":378320,\"journal\":{\"name\":\"Organic Thin Films for Photonics Applications\",\"volume\":\"8 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\":\"Organic Thin Films for Photonics Applications\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/otfa.1997.wc.3\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Organic Thin Films for Photonics Applications","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/otfa.1997.wc.3","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Basic Mechanisms involved in the Off-resonant Nonlinear Refractive Index of PTS-Polydiacetylene
Polydiacetylene single crystal, PTS, is known to have the largest off-resonant nonlinear refractive index (n2). Recently we have demonstrated picosecond all-optical switching using PTS-polydiacetylene in a Fabry-Perot cavity1. This measurement was performed using a pump-probe technique with 90ps pulses at 1.06μm wavelength. In that measurement, besides demonstrating a large modulation depth, we showed that the sign of n2 was negative. In another work, however, a positive sign for n2 was reported from a z-scan measurement2 and two photon resonances were used to explain the positive sign and the off-resonant nonlinear optical processes in PTS. In this work we have made detailed measurements of the sign using Michelson interferometry and z-scan. These and previous measurements using pump-probe technique at different off-resonant wavelengths show that the sign of n2 of PTS is negative over the wavelength of 650 - 1064nm.