Hanchen Wang, A. Meadows, E. Jankowska, B. Reagan, J. Rocca, C. Menoni
{"title":"大气、真空和低温条件下Yb:YAG有源反射镜的激光损伤(会议报告)","authors":"Hanchen Wang, A. Meadows, E. Jankowska, B. Reagan, J. Rocca, C. Menoni","doi":"10.1117/12.2501564","DOIUrl":null,"url":null,"abstract":"The demonstration of a Yb:YAG chirped pulse amplification laser producing 1 J, 5 ps pulses at 500 Hz repetition rate [1] and recently 1 J pulses at 1 kHz repetition rate [2] relied on efficient thermal management and high performance multilayer dielectric coatings on the laser amplifier active mirrors. In the active mirror configuration, the Yb:YAG amplifier crystals use HfO2/SiO2 multilayer dielectric anti-reflection (AR) and high reflection (HR) coatings. The Joule-level amplifier is operated in vacuum and at liquid nitrogen boiling temperature (77 K) with 1030 nm, 220 ps duration laser pulses making four reflections from each HR coating and 8 passes through each AR coating. The LIDT performance of these coatings is crucial to the future scaling of these amplifiers.\n\nIn this work we describe results of an investigation of the laser induced damage threshold (LIDT) of Yb:YAG active mirror laser amplifier disks at atmospheric, vacuum and cryogenic temperature conditions. The measurements were conducted for 220 ps pulses, the typical pulse duration of stretched pulses we are using to implement kW-class average power CPA laser amplifiers [1,2]. We measured the 1-on-1 (single-shot) and 3000-on-1 LIDT on Yb:YAG crystals with and without the coatings. The results show that the LIDT for single shot damage occurs near 20 J/cm2, and 100% damage probability occurs near 29 J/cm2 for either the uncoated or coated Yb:YAG crystal at atmospheric conditions. Similar results were obtained in the vacuum and cryogenic temperatures tests. This leads to the conclusion that the Yb:YAG material itself, and not the coatings, is the limiting factor in the LIDT. \nThis work was performed under the auspices of the U.S. Department of Energy, Office of High Energy Physics, Accelerator Stewardship Program under Award DE-SC0016136.\n\nReferences\n[1] C. Baumgarten, M. Pedicone, H. Bravo, H. Wang, L. Yin, C. S. Menoni, J. J. Rocca, and B. A. Reagan, Optics Letters 41, 3339 (2016).\n[2] Brendan A Reagan, Cory Baumgarten, Elzbieta Jankowska, Han Chi, Herman Bravo, Kristian Dehne, Michael Pedicone, Liang Yin, Hanchen Wang, Carmen S Menoni, Jorge J Rocca, High Power Laser Science and Engineering 6, e11 (2018).","PeriodicalId":374450,"journal":{"name":"Laser-Induced Damage in Optical Materials 2018: 50th Anniversary Conference","volume":"10 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2018-11-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Laser damage of Yb:YAG active mirrors under atmospheric, vacuum, and cryogenic conditions (Conference Presentation)\",\"authors\":\"Hanchen Wang, A. Meadows, E. Jankowska, B. Reagan, J. Rocca, C. Menoni\",\"doi\":\"10.1117/12.2501564\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The demonstration of a Yb:YAG chirped pulse amplification laser producing 1 J, 5 ps pulses at 500 Hz repetition rate [1] and recently 1 J pulses at 1 kHz repetition rate [2] relied on efficient thermal management and high performance multilayer dielectric coatings on the laser amplifier active mirrors. In the active mirror configuration, the Yb:YAG amplifier crystals use HfO2/SiO2 multilayer dielectric anti-reflection (AR) and high reflection (HR) coatings. The Joule-level amplifier is operated in vacuum and at liquid nitrogen boiling temperature (77 K) with 1030 nm, 220 ps duration laser pulses making four reflections from each HR coating and 8 passes through each AR coating. The LIDT performance of these coatings is crucial to the future scaling of these amplifiers.\\n\\nIn this work we describe results of an investigation of the laser induced damage threshold (LIDT) of Yb:YAG active mirror laser amplifier disks at atmospheric, vacuum and cryogenic temperature conditions. The measurements were conducted for 220 ps pulses, the typical pulse duration of stretched pulses we are using to implement kW-class average power CPA laser amplifiers [1,2]. We measured the 1-on-1 (single-shot) and 3000-on-1 LIDT on Yb:YAG crystals with and without the coatings. The results show that the LIDT for single shot damage occurs near 20 J/cm2, and 100% damage probability occurs near 29 J/cm2 for either the uncoated or coated Yb:YAG crystal at atmospheric conditions. Similar results were obtained in the vacuum and cryogenic temperatures tests. This leads to the conclusion that the Yb:YAG material itself, and not the coatings, is the limiting factor in the LIDT. \\nThis work was performed under the auspices of the U.S. Department of Energy, Office of High Energy Physics, Accelerator Stewardship Program under Award DE-SC0016136.\\n\\nReferences\\n[1] C. Baumgarten, M. Pedicone, H. Bravo, H. Wang, L. Yin, C. S. Menoni, J. J. Rocca, and B. A. 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引用次数: 0
摘要
Yb:YAG啁啾脉冲放大激光器在500 Hz重复频率下产生1 J, 5 ps脉冲[1],最近在1 kHz重复频率下产生1 J脉冲[2]的证明依赖于有效的热管理和激光放大器有源反射镜上的高性能多层介质涂层。在有源反射镜结构中,Yb:YAG放大器晶体采用HfO2/SiO2多层介质抗反射(AR)和高反射(HR)涂层。焦耳级放大器在真空和液氮沸腾温度(77 K)下工作,激光脉冲1030 nm,持续时间220 ps,每个HR涂层有4次反射,每个AR涂层有8次反射。这些涂层的LIDT性能对这些放大器的未来缩放至关重要。在本文中,我们描述了在大气、真空和低温条件下Yb:YAG有源镜激光放大盘激光诱导损伤阈值(LIDT)的研究结果。测量是针对220 ps脉冲进行的,这是我们用于实现kw级平均功率CPA激光放大器的拉伸脉冲的典型脉冲持续时间[1,2]。我们测量了有涂层和没有涂层的Yb:YAG晶体上的1对1(单次)和3000对1 LIDT。结果表明,在大气条件下,Yb:YAG晶体单次损伤的LIDT接近20 J/cm2,未涂层或涂层的Yb:YAG晶体100%损伤概率接近29 J/cm2。在真空和低温试验中也得到了类似的结果。由此得出结论,Yb:YAG材料本身,而不是涂层,是LIDT的限制因素。这项工作是在美国能源部高能物理办公室加速器管理项目的支持下进行的,项目编号为DE-SC0016136。参考文献[1]c -鲍姆加滕,m . Pedicone h·布拉沃h . Wang l .阴c . s . Menoni j·j·罗卡,和b·a·里根,光学快报41岁,3339(2016)。[2]Brendan A Reagan, Cory Baumgarten, Elzbieta Jankowska, Han Chi, Herman Bravo, Kristian Dehne, Michael Pedicone,尹亮,Wang Hanchen, Carmen S Menoni, Jorge J Rocca,高功率激光科学与工程,6(2018)。
Laser damage of Yb:YAG active mirrors under atmospheric, vacuum, and cryogenic conditions (Conference Presentation)
The demonstration of a Yb:YAG chirped pulse amplification laser producing 1 J, 5 ps pulses at 500 Hz repetition rate [1] and recently 1 J pulses at 1 kHz repetition rate [2] relied on efficient thermal management and high performance multilayer dielectric coatings on the laser amplifier active mirrors. In the active mirror configuration, the Yb:YAG amplifier crystals use HfO2/SiO2 multilayer dielectric anti-reflection (AR) and high reflection (HR) coatings. The Joule-level amplifier is operated in vacuum and at liquid nitrogen boiling temperature (77 K) with 1030 nm, 220 ps duration laser pulses making four reflections from each HR coating and 8 passes through each AR coating. The LIDT performance of these coatings is crucial to the future scaling of these amplifiers.
In this work we describe results of an investigation of the laser induced damage threshold (LIDT) of Yb:YAG active mirror laser amplifier disks at atmospheric, vacuum and cryogenic temperature conditions. The measurements were conducted for 220 ps pulses, the typical pulse duration of stretched pulses we are using to implement kW-class average power CPA laser amplifiers [1,2]. We measured the 1-on-1 (single-shot) and 3000-on-1 LIDT on Yb:YAG crystals with and without the coatings. The results show that the LIDT for single shot damage occurs near 20 J/cm2, and 100% damage probability occurs near 29 J/cm2 for either the uncoated or coated Yb:YAG crystal at atmospheric conditions. Similar results were obtained in the vacuum and cryogenic temperatures tests. This leads to the conclusion that the Yb:YAG material itself, and not the coatings, is the limiting factor in the LIDT.
This work was performed under the auspices of the U.S. Department of Energy, Office of High Energy Physics, Accelerator Stewardship Program under Award DE-SC0016136.
References
[1] C. Baumgarten, M. Pedicone, H. Bravo, H. Wang, L. Yin, C. S. Menoni, J. J. Rocca, and B. A. Reagan, Optics Letters 41, 3339 (2016).
[2] Brendan A Reagan, Cory Baumgarten, Elzbieta Jankowska, Han Chi, Herman Bravo, Kristian Dehne, Michael Pedicone, Liang Yin, Hanchen Wang, Carmen S Menoni, Jorge J Rocca, High Power Laser Science and Engineering 6, e11 (2018).