T. Tanaka, K. Sako, R. Kasegawa, M. Toishi, K. Watanabe, S. Akao
{"title":"用于全息数据存储的可调谐蓝色激光器","authors":"T. Tanaka, K. Sako, R. Kasegawa, M. Toishi, K. Watanabe, S. Akao","doi":"10.1109/ODS.2006.1632769","DOIUrl":null,"url":null,"abstract":"2. Emission section The tunable blue-laser system we report here consists of a micro computer, electric circuits, and the laser shown in Fig. 1. Figure 2 shows the inside of the laser, consisting of the emission section, the wavelength monitor and the mode hop monitor. The emission section consists of a laser diode (LD), a lens, a grating, a mirror and a motor. A Littrow-type laser is used to generate a single-mode ray. The LD’s multi-mode ray is collimated in the lens and diffracted on the grating. One of the first-order rays is selected by adjusting the angle of the grating and diffracted back to the LD, and the LD lases in a single mode of its wavelength. The incident angle and the diffracted angle are the same, and the angles θ are given by g λ θ = sin 2 (1)","PeriodicalId":332569,"journal":{"name":"2006 Optical Data Storage Topical Meeting","volume":"26 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2006-06-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Tunable Blue Laser for Holographic Data Storage\",\"authors\":\"T. Tanaka, K. Sako, R. Kasegawa, M. Toishi, K. Watanabe, S. Akao\",\"doi\":\"10.1109/ODS.2006.1632769\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"2. Emission section The tunable blue-laser system we report here consists of a micro computer, electric circuits, and the laser shown in Fig. 1. Figure 2 shows the inside of the laser, consisting of the emission section, the wavelength monitor and the mode hop monitor. The emission section consists of a laser diode (LD), a lens, a grating, a mirror and a motor. A Littrow-type laser is used to generate a single-mode ray. The LD’s multi-mode ray is collimated in the lens and diffracted on the grating. One of the first-order rays is selected by adjusting the angle of the grating and diffracted back to the LD, and the LD lases in a single mode of its wavelength. The incident angle and the diffracted angle are the same, and the angles θ are given by g λ θ = sin 2 (1)\",\"PeriodicalId\":332569,\"journal\":{\"name\":\"2006 Optical Data Storage Topical Meeting\",\"volume\":\"26 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2006-06-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2006 Optical Data Storage Topical Meeting\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ODS.2006.1632769\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2006 Optical Data Storage Topical Meeting","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ODS.2006.1632769","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
2. Emission section The tunable blue-laser system we report here consists of a micro computer, electric circuits, and the laser shown in Fig. 1. Figure 2 shows the inside of the laser, consisting of the emission section, the wavelength monitor and the mode hop monitor. The emission section consists of a laser diode (LD), a lens, a grating, a mirror and a motor. A Littrow-type laser is used to generate a single-mode ray. The LD’s multi-mode ray is collimated in the lens and diffracted on the grating. One of the first-order rays is selected by adjusting the angle of the grating and diffracted back to the LD, and the LD lases in a single mode of its wavelength. The incident angle and the diffracted angle are the same, and the angles θ are given by g λ θ = sin 2 (1)