{"title":"Observation of intrinsic optical bistability induced by self-focusing in a semiconductor-doped glass filter","authors":"F. Pereira, J. Salcedo, M. Belsley","doi":"10.1364/cleo_europe.1994.cthi79","DOIUrl":null,"url":null,"abstract":"Wherret et al.1 have derived a general condition for the existence of intrinsic optical bistability, stipulating that the absorption length of the sample, αL, must be less than 0.18. Nonetheless several research groups have observed optical bistability in samples with absorption lengths significantly above this limit.2 It has been suggested2 that the observed bistability is the result of an initial self-focusing of the incident beam brought about by thermal refractive index change which then induces a bistable effect in the final portion of the sample. If the focal length of the laser induced thermal lens is comparable with the sample thickness, then the reduction of the laser beam size could then induce bistability at a lower threshold in the final portion of the sample. We have carried a systematic test of this hypothesis, using a modified version of the Z-scan technique, on a commercially available semiconductor-doped glass filter.","PeriodicalId":276336,"journal":{"name":"1994 Conference on Lasers and Electro-Optics Europe","volume":"41 5","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":"1994 Conference on Lasers and Electro-Optics Europe","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/cleo_europe.1994.cthi79","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
Wherret et al.1 have derived a general condition for the existence of intrinsic optical bistability, stipulating that the absorption length of the sample, αL, must be less than 0.18. Nonetheless several research groups have observed optical bistability in samples with absorption lengths significantly above this limit.2 It has been suggested2 that the observed bistability is the result of an initial self-focusing of the incident beam brought about by thermal refractive index change which then induces a bistable effect in the final portion of the sample. If the focal length of the laser induced thermal lens is comparable with the sample thickness, then the reduction of the laser beam size could then induce bistability at a lower threshold in the final portion of the sample. We have carried a systematic test of this hypothesis, using a modified version of the Z-scan technique, on a commercially available semiconductor-doped glass filter.
Wherret et al.1推导了存在本征光学双稳性的一般条件,规定样品的吸收长度αL必须小于0.18。尽管如此,一些研究小组已经观察到吸收长度明显超过这个限制的样品的光学双稳性有人认为,所观察到的双稳性是由热折射率变化引起的入射光束的初始自聚焦的结果,然后在样品的最终部分引起双稳效应。如果激光诱导热透镜的焦距与样品厚度相当,那么激光束尺寸的减小可以在样品的最终部分以较低的阈值诱导双稳。我们已经对这一假设进行了系统的测试,使用改进版的z扫描技术,在市售的半导体掺杂玻璃过滤器上。