{"title":"以亚本征腔往返间隔从啁啾锁模激光二极管发出的250 fs脉冲序列","authors":"N. Stelmakh, A. Azouz, J. Lourtioz","doi":"10.1109/ISLC.1996.553773","DOIUrl":null,"url":null,"abstract":"To our knowledge, fine periodical evolutions of the pulse structure with the length of the external cavity have never been reported in short-pulse mode-locked extended-cavity laser diodes. In this communication, we demonstrate a strong inter-dependence between the external and intrinsic cavity lengths in these mode-locked laser systems when an external chirp compensation is used. We found that the length of the external cavity (l/sub e/) must be equal to a multiple of the intrinsic laser diode cavity length (l/sub i/) to produce standard pulse structures with one sub-pulse per intrinsic cavity roundtrip time. Similarly, the external cavity length must be equal to (m+1/n)*l/sub i/, with m being an integer, to obtain n sub-pulses per intrinsic cavity roundtrip time. In our experiments, we observed pronounced pulse structures for n up to 8. This latter value corresponds to the generation of /spl sim/250 fs pulse trains with a pulse repetition rate of /spl sim/300 GHz and a total energy /spl sim/20-30 pJ.","PeriodicalId":346992,"journal":{"name":"Conference Digest. 15th IEEE International Semiconductor Laser Conference","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"1996-10-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Trains of 250 fs pulses at sub-intrinsic-cavity roundtrip intervals from chirped mode-locked laser diodes\",\"authors\":\"N. Stelmakh, A. Azouz, J. Lourtioz\",\"doi\":\"10.1109/ISLC.1996.553773\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"To our knowledge, fine periodical evolutions of the pulse structure with the length of the external cavity have never been reported in short-pulse mode-locked extended-cavity laser diodes. In this communication, we demonstrate a strong inter-dependence between the external and intrinsic cavity lengths in these mode-locked laser systems when an external chirp compensation is used. We found that the length of the external cavity (l/sub e/) must be equal to a multiple of the intrinsic laser diode cavity length (l/sub i/) to produce standard pulse structures with one sub-pulse per intrinsic cavity roundtrip time. Similarly, the external cavity length must be equal to (m+1/n)*l/sub i/, with m being an integer, to obtain n sub-pulses per intrinsic cavity roundtrip time. In our experiments, we observed pronounced pulse structures for n up to 8. This latter value corresponds to the generation of /spl sim/250 fs pulse trains with a pulse repetition rate of /spl sim/300 GHz and a total energy /spl sim/20-30 pJ.\",\"PeriodicalId\":346992,\"journal\":{\"name\":\"Conference Digest. 15th IEEE International Semiconductor Laser Conference\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1996-10-13\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Conference Digest. 15th IEEE International Semiconductor Laser Conference\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ISLC.1996.553773\",\"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 Digest. 15th IEEE International Semiconductor Laser Conference","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ISLC.1996.553773","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Trains of 250 fs pulses at sub-intrinsic-cavity roundtrip intervals from chirped mode-locked laser diodes
To our knowledge, fine periodical evolutions of the pulse structure with the length of the external cavity have never been reported in short-pulse mode-locked extended-cavity laser diodes. In this communication, we demonstrate a strong inter-dependence between the external and intrinsic cavity lengths in these mode-locked laser systems when an external chirp compensation is used. We found that the length of the external cavity (l/sub e/) must be equal to a multiple of the intrinsic laser diode cavity length (l/sub i/) to produce standard pulse structures with one sub-pulse per intrinsic cavity roundtrip time. Similarly, the external cavity length must be equal to (m+1/n)*l/sub i/, with m being an integer, to obtain n sub-pulses per intrinsic cavity roundtrip time. In our experiments, we observed pronounced pulse structures for n up to 8. This latter value corresponds to the generation of /spl sim/250 fs pulse trains with a pulse repetition rate of /spl sim/300 GHz and a total energy /spl sim/20-30 pJ.