{"title":"一个0.5太瓦,125飞秒的钛蓝宝石激光器","authors":"J. Kmetec, J. J. Macklin, B. Lemoff, J. Young","doi":"10.1364/swcr.1991.tua13","DOIUrl":null,"url":null,"abstract":"Broadband, high-energy storage, solid state amplifiers and chirped-pulse amplification further extend the peak power obtainable from a laser source. Laser-generation of x-rays and strong-field experiments require focusable beams at terawatt power levels. We have constructed a system at 802 nm using Ti:sapphire amplifiers and the technique of chirped-pulse amplification. In our system, a dye laser produces a train of 85 fsec seed pulses. A positively-dispersive grating pair expander chirps these pulses, stretching the pulsewidth to 180 psec while preserving the femtosecond bandwidth. The stretched pulses seed a Ti:sapphire regenerative amplifier, producing 8 mJ, 180 psec output. Further amplification in a triple-passed Ti:sapphire amplifier increases the pulse energy to 120 mJ. A negatively-dispersive parallel grating pair removes the chirp, recompressing the pulse to 125 fsec. The final output contains 60 mJ of energy in a 125 fsec pulsewidth. The output beam is Gaussian and measured to be 1.2 times diffraction limited. Focusing with an f/6 lens achieves 87% transmission through a 10.8 micron pinhole. Hence, f/6 focusing will produce 1018W/cm2. Passage through a saturable absorber reduces the amplifier noise to signal power ratio to 10−9 in the leading edge of the short pulse, with a large signal, whole beam transmission of 70%. Both the regenerative and the final amplifier are pumped by the 532 nm frequency-doubled output of a single commercially available 10 Hz Nd:YAG laser.","PeriodicalId":286766,"journal":{"name":"Short-Wavelength Coherent Radiation: Generation and Application","volume":"11 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"A 0.5 Terawatt, 125 Femtosecond Ti:Sapphire Laser\",\"authors\":\"J. Kmetec, J. J. Macklin, B. Lemoff, J. Young\",\"doi\":\"10.1364/swcr.1991.tua13\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Broadband, high-energy storage, solid state amplifiers and chirped-pulse amplification further extend the peak power obtainable from a laser source. Laser-generation of x-rays and strong-field experiments require focusable beams at terawatt power levels. We have constructed a system at 802 nm using Ti:sapphire amplifiers and the technique of chirped-pulse amplification. In our system, a dye laser produces a train of 85 fsec seed pulses. A positively-dispersive grating pair expander chirps these pulses, stretching the pulsewidth to 180 psec while preserving the femtosecond bandwidth. The stretched pulses seed a Ti:sapphire regenerative amplifier, producing 8 mJ, 180 psec output. Further amplification in a triple-passed Ti:sapphire amplifier increases the pulse energy to 120 mJ. A negatively-dispersive parallel grating pair removes the chirp, recompressing the pulse to 125 fsec. The final output contains 60 mJ of energy in a 125 fsec pulsewidth. The output beam is Gaussian and measured to be 1.2 times diffraction limited. Focusing with an f/6 lens achieves 87% transmission through a 10.8 micron pinhole. Hence, f/6 focusing will produce 1018W/cm2. Passage through a saturable absorber reduces the amplifier noise to signal power ratio to 10−9 in the leading edge of the short pulse, with a large signal, whole beam transmission of 70%. Both the regenerative and the final amplifier are pumped by the 532 nm frequency-doubled output of a single commercially available 10 Hz Nd:YAG laser.\",\"PeriodicalId\":286766,\"journal\":{\"name\":\"Short-Wavelength Coherent Radiation: Generation and Application\",\"volume\":\"11 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Short-Wavelength Coherent Radiation: Generation and Application\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/swcr.1991.tua13\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Short-Wavelength Coherent Radiation: Generation and Application","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/swcr.1991.tua13","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Broadband, high-energy storage, solid state amplifiers and chirped-pulse amplification further extend the peak power obtainable from a laser source. Laser-generation of x-rays and strong-field experiments require focusable beams at terawatt power levels. We have constructed a system at 802 nm using Ti:sapphire amplifiers and the technique of chirped-pulse amplification. In our system, a dye laser produces a train of 85 fsec seed pulses. A positively-dispersive grating pair expander chirps these pulses, stretching the pulsewidth to 180 psec while preserving the femtosecond bandwidth. The stretched pulses seed a Ti:sapphire regenerative amplifier, producing 8 mJ, 180 psec output. Further amplification in a triple-passed Ti:sapphire amplifier increases the pulse energy to 120 mJ. A negatively-dispersive parallel grating pair removes the chirp, recompressing the pulse to 125 fsec. The final output contains 60 mJ of energy in a 125 fsec pulsewidth. The output beam is Gaussian and measured to be 1.2 times diffraction limited. Focusing with an f/6 lens achieves 87% transmission through a 10.8 micron pinhole. Hence, f/6 focusing will produce 1018W/cm2. Passage through a saturable absorber reduces the amplifier noise to signal power ratio to 10−9 in the leading edge of the short pulse, with a large signal, whole beam transmission of 70%. Both the regenerative and the final amplifier are pumped by the 532 nm frequency-doubled output of a single commercially available 10 Hz Nd:YAG laser.