{"title":"光纤到户发生了什么?","authors":"P. Shumate","doi":"10.1109/CLEO.1997.603138","DOIUrl":null,"url":null,"abstract":"situations: with nonthreshold interaction of the laser beam with the NLC, and with the threshold interaction (known as optical Freedericks transition). Some characteristic dependencies are presented in Figs. 2 and 3. For nonthreshold case, the sensitivity of the NLCreorientation magnitude to the speed of motion was found to be of the order of ANlAv -0.2 ()*m/s)-’ [for the beam power P = 722 mW. The effect of the transverse motion is stronger for the for critical character of interaction light and NLC, AN/Av 1 (pm/s)-’]. The following simple expression allows us to gain some physical insight into the problem, and to evaluate the characteristic parameters:","PeriodicalId":173652,"journal":{"name":"CLEO '97., Summaries of Papers Presented at the Conference on Lasers and Electro-Optics","volume":"11 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1997-05-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":"{\"title\":\"What's happening in fiber-to-the-home?\",\"authors\":\"P. Shumate\",\"doi\":\"10.1109/CLEO.1997.603138\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"situations: with nonthreshold interaction of the laser beam with the NLC, and with the threshold interaction (known as optical Freedericks transition). Some characteristic dependencies are presented in Figs. 2 and 3. For nonthreshold case, the sensitivity of the NLCreorientation magnitude to the speed of motion was found to be of the order of ANlAv -0.2 ()*m/s)-’ [for the beam power P = 722 mW. The effect of the transverse motion is stronger for the for critical character of interaction light and NLC, AN/Av 1 (pm/s)-’]. The following simple expression allows us to gain some physical insight into the problem, and to evaluate the characteristic parameters:\",\"PeriodicalId\":173652,\"journal\":{\"name\":\"CLEO '97., Summaries of Papers Presented at the Conference on Lasers and Electro-Optics\",\"volume\":\"11 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1997-05-18\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"3\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"CLEO '97., Summaries of Papers Presented at the Conference on Lasers and Electro-Optics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/CLEO.1997.603138\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"CLEO '97., Summaries of Papers Presented at the Conference on Lasers and Electro-Optics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CLEO.1997.603138","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
situations: with nonthreshold interaction of the laser beam with the NLC, and with the threshold interaction (known as optical Freedericks transition). Some characteristic dependencies are presented in Figs. 2 and 3. For nonthreshold case, the sensitivity of the NLCreorientation magnitude to the speed of motion was found to be of the order of ANlAv -0.2 ()*m/s)-’ [for the beam power P = 722 mW. The effect of the transverse motion is stronger for the for critical character of interaction light and NLC, AN/Av 1 (pm/s)-’]. The following simple expression allows us to gain some physical insight into the problem, and to evaluate the characteristic parameters: