{"title":"A compact-high efficiency-flashlamp pumped Ti:Al2O3 laser","authors":"F. Collier","doi":"10.1364/cleo_europe.1994.cthn1","DOIUrl":null,"url":null,"abstract":"Pumping a Ti:Al2O3 laser with another laser, such as a frequency-doubled Nd:YAG laser, limits both the energy of each pulse and the overall efficiency of the system. Pumping Ti:Al2O3 by flashlamps is difficult, however, because of the Ti3+ short radiative lifetime (3.2 μs). Also, we develope an all solid-state power supply that can deliver a 5 kA peak current to the flashlamp on the same time scale. The supply provides a 150 to 300 mA direct simmer current and 10 A pseudo-simmer current (risetime of 100 μs) to allow for spatial centering of the arc in the flashlamp bore. At the top of the pseudo-simmer pulse, the main electrical pulse is provided by an original circuit based on magnetic compression. A maximum energy of 110 J can be delivered to the two flashlamps (55 J per lamp) within 4.5 μs with 75% electrical efficiency.","PeriodicalId":276336,"journal":{"name":"1994 Conference on Lasers and Electro-Optics Europe","volume":"20 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"1994 Conference on Lasers and Electro-Optics Europe","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/cleo_europe.1994.cthn1","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
Pumping a Ti:Al2O3 laser with another laser, such as a frequency-doubled Nd:YAG laser, limits both the energy of each pulse and the overall efficiency of the system. Pumping Ti:Al2O3 by flashlamps is difficult, however, because of the Ti3+ short radiative lifetime (3.2 μs). Also, we develope an all solid-state power supply that can deliver a 5 kA peak current to the flashlamp on the same time scale. The supply provides a 150 to 300 mA direct simmer current and 10 A pseudo-simmer current (risetime of 100 μs) to allow for spatial centering of the arc in the flashlamp bore. At the top of the pseudo-simmer pulse, the main electrical pulse is provided by an original circuit based on magnetic compression. A maximum energy of 110 J can be delivered to the two flashlamps (55 J per lamp) within 4.5 μs with 75% electrical efficiency.