G. Wisner, A. Angelbeck, B. A. Woody, A. Greiner, R. Freeman, H. C. Reynolds
{"title":"利用自适应光学技术进行闪光跟踪","authors":"G. Wisner, A. Angelbeck, B. A. Woody, A. Greiner, R. Freeman, H. C. Reynolds","doi":"10.1364/cleos.1976.thf6","DOIUrl":null,"url":null,"abstract":"Adaptive optical techniques have been employed to track target glint returns using two-axis steering and focus correction. Measurements were made on laboratory apparatus, operating at 10.6 µm. The apparatus consists of a low power CO2 laser, a 300-Hz bandwidth wavefront manipulator, focusing optics to form a far-field beam pattern, a moving glint (a small polished sphere), and an on-axis receiver that views target return. Adaptive control is implemented by tagging each correction mode with a high-frequency low-amplitude dither which is a small fraction of the available mode range. Classical hill-climbing servos are used to maximize glint return by nulling the dither component of each correction at a zero slope point corresponding to maximum target power.","PeriodicalId":301658,"journal":{"name":"Conference on Laser and Electrooptical Systems","volume":"70 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1976-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Glint tracking using adaptive optical techniques\",\"authors\":\"G. Wisner, A. Angelbeck, B. A. Woody, A. Greiner, R. Freeman, H. C. Reynolds\",\"doi\":\"10.1364/cleos.1976.thf6\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Adaptive optical techniques have been employed to track target glint returns using two-axis steering and focus correction. Measurements were made on laboratory apparatus, operating at 10.6 µm. The apparatus consists of a low power CO2 laser, a 300-Hz bandwidth wavefront manipulator, focusing optics to form a far-field beam pattern, a moving glint (a small polished sphere), and an on-axis receiver that views target return. Adaptive control is implemented by tagging each correction mode with a high-frequency low-amplitude dither which is a small fraction of the available mode range. Classical hill-climbing servos are used to maximize glint return by nulling the dither component of each correction at a zero slope point corresponding to maximum target power.\",\"PeriodicalId\":301658,\"journal\":{\"name\":\"Conference on Laser and Electrooptical Systems\",\"volume\":\"70 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1976-04-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Conference on Laser and Electrooptical Systems\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/cleos.1976.thf6\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Conference on Laser and Electrooptical Systems","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/cleos.1976.thf6","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Adaptive optical techniques have been employed to track target glint returns using two-axis steering and focus correction. Measurements were made on laboratory apparatus, operating at 10.6 µm. The apparatus consists of a low power CO2 laser, a 300-Hz bandwidth wavefront manipulator, focusing optics to form a far-field beam pattern, a moving glint (a small polished sphere), and an on-axis receiver that views target return. Adaptive control is implemented by tagging each correction mode with a high-frequency low-amplitude dither which is a small fraction of the available mode range. Classical hill-climbing servos are used to maximize glint return by nulling the dither component of each correction at a zero slope point corresponding to maximum target power.