D. Strickland, P. Maine, M. Bouvier, S. Williamson, G. Mourou
{"title":"使用脉冲压缩技术的皮秒脉冲放大","authors":"D. Strickland, P. Maine, M. Bouvier, S. Williamson, G. Mourou","doi":"10.1364/CLEO.1986.THL1","DOIUrl":null,"url":null,"abstract":"Nd:Glass amplifiers have very good energy storage capabilities, but, the energy extraction is extremely inefficient for short pulse amplification. Scientists working in the radar field overcame similar peak power limitations by first chirping and stretching the pulse prior to amplification.1-2 By amplifying the longer pulses, much higher energies could be achieved. The echo was then compressed to a pulsewidth approximately equal to 1/Δf, where Δf is the total frequency chirp.","PeriodicalId":371790,"journal":{"name":"Topical Meeting on Ultrafast Phenomena","volume":"55 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1986-06-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"4","resultStr":"{\"title\":\"Picosecond Pulse Amplification Using Pulse Compression Techniques\",\"authors\":\"D. Strickland, P. Maine, M. Bouvier, S. Williamson, G. Mourou\",\"doi\":\"10.1364/CLEO.1986.THL1\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Nd:Glass amplifiers have very good energy storage capabilities, but, the energy extraction is extremely inefficient for short pulse amplification. Scientists working in the radar field overcame similar peak power limitations by first chirping and stretching the pulse prior to amplification.1-2 By amplifying the longer pulses, much higher energies could be achieved. The echo was then compressed to a pulsewidth approximately equal to 1/Δf, where Δf is the total frequency chirp.\",\"PeriodicalId\":371790,\"journal\":{\"name\":\"Topical Meeting on Ultrafast Phenomena\",\"volume\":\"55 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1986-06-09\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"4\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Topical Meeting on Ultrafast Phenomena\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/CLEO.1986.THL1\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Topical Meeting on Ultrafast Phenomena","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/CLEO.1986.THL1","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Picosecond Pulse Amplification Using Pulse Compression Techniques
Nd:Glass amplifiers have very good energy storage capabilities, but, the energy extraction is extremely inefficient for short pulse amplification. Scientists working in the radar field overcame similar peak power limitations by first chirping and stretching the pulse prior to amplification.1-2 By amplifying the longer pulses, much higher energies could be achieved. The echo was then compressed to a pulsewidth approximately equal to 1/Δf, where Δf is the total frequency chirp.