{"title":"Three-dimensional photonic crystals and their applications","authors":"S. Noda","doi":"10.1109/CLEOPR.1999.811366","DOIUrl":null,"url":null,"abstract":"We report our new approach to develop the complete three-dimensional photonic crystal and the future prospects. Our photonic crystal is constructed with GaAs (or InP) stripes stacked by a wafer-fusion technique to form an asymmetric face-centered cubic (A-FCC) structure. The stacked four layers correspond to the one-period of the A-FCC structure. The band structure has a complete photonic band gap for all wave vectors. Moreover, since the crystal is constructed with a III-V semiconductor, which is widely utilized for optoelectronic devices, by the wafer-bonding technique it is possible to introduce arbitrary defect states and light-emitters and to form an electronically active interface. Thus, once the 3D photonic crystal is realized, it will open a door for various applications including an active quantum device such as zero-threshold laser.","PeriodicalId":408728,"journal":{"name":"Technical Digest. CLEO/Pacific Rim '99. Pacific Rim Conference on Lasers and Electro-Optics (Cat. No.99TH8464)","volume":"45 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1999-08-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Technical Digest. CLEO/Pacific Rim '99. Pacific Rim Conference on Lasers and Electro-Optics (Cat. No.99TH8464)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CLEOPR.1999.811366","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
We report our new approach to develop the complete three-dimensional photonic crystal and the future prospects. Our photonic crystal is constructed with GaAs (or InP) stripes stacked by a wafer-fusion technique to form an asymmetric face-centered cubic (A-FCC) structure. The stacked four layers correspond to the one-period of the A-FCC structure. The band structure has a complete photonic band gap for all wave vectors. Moreover, since the crystal is constructed with a III-V semiconductor, which is widely utilized for optoelectronic devices, by the wafer-bonding technique it is possible to introduce arbitrary defect states and light-emitters and to form an electronically active interface. Thus, once the 3D photonic crystal is realized, it will open a door for various applications including an active quantum device such as zero-threshold laser.