{"title":"用于WDM系统的高速可调谐液晶光学滤波器","authors":"A. Sneh, K. Johnson","doi":"10.1109/LEOSST.1994.700513","DOIUrl":null,"url":null,"abstract":"One of the key components in future wavelength-division-multiplexed (WDM) networks is a tunable optical filter. Desirable characteristics for a commercially successful filter include: fast tuning speed, wide tuning range (30-40 nm for systems combining doped fiber amplifiers), low power consumption, and low cost. As an inherently inexpensive technology with low power consumption, liquid crystals (LCs) have the potential to fulfill all of the above req.uirements. Tunable LC Fabry-Perot (FP) filters have been demonstrated using nematic LCs as the active cavity material[l,2]. These filters have a tuning range of -100 nm, however their tuning speed ranges from a few milliseconds to hundreds of milliseconds [:3], which is too slow for packet-switched systems. Another class of LCs, chiral smectic A* LCs, have microsecond and submicrosecond switching speeds, allowing for three orders of magnitude faster tuning over nematic LC filters.","PeriodicalId":379594,"journal":{"name":"Proceedings of IEE/LEOS Summer Topical Meetings: Integrated Optoelectronics","volume":"13 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1994-07-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"17","resultStr":"{\"title\":\"High-speed Tunable Liquid Crystal Optical Filter For WDM Systems\",\"authors\":\"A. Sneh, K. Johnson\",\"doi\":\"10.1109/LEOSST.1994.700513\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"One of the key components in future wavelength-division-multiplexed (WDM) networks is a tunable optical filter. Desirable characteristics for a commercially successful filter include: fast tuning speed, wide tuning range (30-40 nm for systems combining doped fiber amplifiers), low power consumption, and low cost. As an inherently inexpensive technology with low power consumption, liquid crystals (LCs) have the potential to fulfill all of the above req.uirements. Tunable LC Fabry-Perot (FP) filters have been demonstrated using nematic LCs as the active cavity material[l,2]. These filters have a tuning range of -100 nm, however their tuning speed ranges from a few milliseconds to hundreds of milliseconds [:3], which is too slow for packet-switched systems. Another class of LCs, chiral smectic A* LCs, have microsecond and submicrosecond switching speeds, allowing for three orders of magnitude faster tuning over nematic LC filters.\",\"PeriodicalId\":379594,\"journal\":{\"name\":\"Proceedings of IEE/LEOS Summer Topical Meetings: Integrated Optoelectronics\",\"volume\":\"13 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1994-07-06\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"17\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Proceedings of IEE/LEOS Summer Topical Meetings: Integrated Optoelectronics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/LEOSST.1994.700513\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of IEE/LEOS Summer Topical Meetings: Integrated Optoelectronics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/LEOSST.1994.700513","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
High-speed Tunable Liquid Crystal Optical Filter For WDM Systems
One of the key components in future wavelength-division-multiplexed (WDM) networks is a tunable optical filter. Desirable characteristics for a commercially successful filter include: fast tuning speed, wide tuning range (30-40 nm for systems combining doped fiber amplifiers), low power consumption, and low cost. As an inherently inexpensive technology with low power consumption, liquid crystals (LCs) have the potential to fulfill all of the above req.uirements. Tunable LC Fabry-Perot (FP) filters have been demonstrated using nematic LCs as the active cavity material[l,2]. These filters have a tuning range of -100 nm, however their tuning speed ranges from a few milliseconds to hundreds of milliseconds [:3], which is too slow for packet-switched systems. Another class of LCs, chiral smectic A* LCs, have microsecond and submicrosecond switching speeds, allowing for three orders of magnitude faster tuning over nematic LC filters.