共查询到18条相似文献,搜索用时 234 毫秒
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LD端面泵浦腔内倍频Yb∶YAG绿光激光器 总被引:3,自引:2,他引:1
报道了一种激光二极管(LD)端面泵浦10at%掺杂Yb∶YAG激光晶体(4×4×1 mm)和Ⅰ类临界相位匹配LBO的腔内倍频全固态绿光激光器.为了克服“绿光问题”,采用了两个激光二极管偏振耦合系统.在双路泵浦功率为1.2 W时,获得最高功率为40 mW 525 nm的连续基模激光输出.在腔内插入Cr4+:YAG饱和吸收体被动调Q,在泵浦功率为1.2 W时,可以获得平均功率为5.2 mW,脉冲重复频率为2.44 kHz,脉冲宽度为51.5 ns,峰值功率为41.7 W的515 nm脉冲激光输出.输出波长发生变化,而且515 nm脉冲激光输出的阈值仅为728 mW. 相似文献
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LD泵浦Nd:YAG/Cr:YAG腔外频率变换高功率紫外激光器 总被引:8,自引:4,他引:4
用KTP晶体对激光二极管端面泵浦的Nd:YAG晶体;Cr:YAG被动调Q产生的1064nm脉冲激光器进行腔外倍频,用BBO晶体四倍频产生266 nm紫外激光.用15 W的LD阵列;当LD泵浦功率为12 W的情况下;红外(1064 μm)调Q平均输出功率为2.2 W;脉冲序列周期为40 μs;脉宽为18ns;峰值功率高达4.9kW.采用KTP腔外二倍频;532nm的绿光输出平均功率为850mW;用BBO腔外四倍频;266nm的紫外光输出平均功率高达215mW,绿光-紫外光光转换效率为25.2%, 红外到紫外总的转换效率为9.8%. 相似文献
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用KTP晶体对激光二极管端面泵浦的Nd∶YAG晶体,Cr∶YAG被动调Q产生的1064 nm脉冲激光器进行腔外倍频,用BBO晶体四倍频产生266 nm紫外激光.用15 W的LD阵列,当LD泵浦功率为12 W的情况下,红外(1064μm)调Q平均输出功率为2.2 W,脉冲序列周期为40μs,脉宽为18 ns,峰值功率高达4.9 kW.采用KTP腔外二倍频,532 nm的绿光输出平均功率为850 mW;用BBO腔外四倍频,266 nm的紫外光输出平均功率高达215 mW,绿光-紫外光光转换效率为25.2%,红外到紫外总的转换效率为9.8%. 相似文献
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LD脉冲侧面泵浦Nd∶YAG电光调Q低重频窄脉宽紫外激光器 总被引:1,自引:0,他引:1
介绍了在1~20 Hz电光调Q情况下,半导体脉冲激光侧面泵浦Nd∶YAG晶体腔外四倍频266 nm紫外激光器的输出特性.实验采用直腔结构,在腔外分别利用KTP和BBO晶体产生532 nm倍频绿光、266 nm四倍频紫外激光.当泵浦电流为120 A、重复率为1 Hz时,266 nm紫外激光最大单脉冲能量为15.4 mJ、脉宽8 ns,峰值功率高达1.93 mW;重复率20 Hz时,获得了最大平均功率为156.2 mW的266 nm紫外激光输出,四倍频的转换效率为10.63%.同时利用一组分光镜,获得了352 mW的532 nm脉冲绿光和423 mW的1 064 nm脉冲红外光输出. 相似文献
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为了实现高可靠、窄脉宽、高峰值功率激光输出,采用侧面泵浦技术和电光调Q技术,设计出一种激光二极管侧面泵浦电光调Q全固态绿光激光器。采用结构简单、紧凑的平-平腔设计,其端镜和输出镜均为平面镜,获得较稳定的侧面泵浦Nd∶YAG腔外倍频KTP脉冲绿光激光输出。当泵浦电流为120A,重复频率为600Hz时,获得脉冲绿光的最高输出平均功率为3.62W,1064nm到532nm的转换效率为15.3%,其脉宽为21ns,峰值功率为300kW, 单脉冲能量为6.01mJ。实验结果表明:该激光器稳定性可靠,输出激光脉宽较窄、峰值功率高。 相似文献
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报道了LD泵浦的Nd∶YAG/KTP/Cr∶YAG结构被动调Q绿光激光器.当注入泵浦功率为750mW时,获得了平均功率38mW,脉冲宽度14.7ns,重复频率20.4kHz,峰值功率126.6W的调Q绿激光输出. 相似文献
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X. Y. Mi 《Laser Physics》2012,22(1):74-77
We report for the first time a continuous-wave (CW) green laser emission by sum-frequency mixing in Yb:YAG crystal. Using
type-I critical phase-matching LBO crystal, a green laser at 520 nm is obtained by 1030 and 1048 nm intracavity sum-frequency
mixing. The maximum laser output power of 269 mW is obtained when an incident pump laser of 17.8 W is used. At the output
power level of 269 mW, the output stability is better than 3.2%. 相似文献
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B. Z. Li C. G. Sun A. F. Zang X. H. Zhang M. Zhao J. B. Wang G. Y. Jin 《Laser Physics》2011,21(6):988-990
We describe the output performances of the 1048 nm transition in Yb:YAG under in-band pumping with diode laser at the 968 nm wavelength. An end-pumped Yb:YAG crystal yielded 787 mW of continuous-wave (CW) output power for 9.1 W of absorbed pump power. Furthermore, 104 mW 524 nm green light was acquired by frequency doubling. Comparative results obtained for the pump with diode laser at 940 nm are given in order to prove the advantages of the in-band pumping. 相似文献
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H. Z. Cao F. J. Liu H. M. Tan H. Y. Peng M. H. Zhang Y. Q. Chen B. Zhang B. L. Chen C. J. Wang 《Laser Physics》2009,19(5):919-922
With a type-I critical phase-matching LBO crystal, an intracavity frequency doubled solid-stated Yb:YAG green laser is reported. Using a plano-concave resonator, with pump power of 1.37 W, 24.5 mW TEM00 continuous wave laser at 525 nm was obtained. The optical conversion efficiency is 1.8%. By adjusting the placed angle of LBO, several lasers wavelength from 525.0 to 537.8 nm could be extracted. The maximum output power at 537.8 nm is 3.1 mW. 相似文献
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A laser diode end-pumped 10 at.% doped Yb:YAG microchip crystal intracavity frequency doubled all solid-stated green laser is reported in this paper. Using one plano-concave resonator, with the pump power of 1.2 W, 44.2 mW TEM00 continuous wave (CW) laser at 525 nm was obtained, the optical conversion efficiency was about 3.7%. When a Cr:YAG crystal with initial transmission of 95.5% inserted in the resonator, the maximum output power of 6.4 mW, pulse duration width of 49.1 ns, pulse repetition rate of 2.45 kHz, and peak power of 53.1 W at 515 nm were achieved when the pump power was 1.2 W. The wavelength changed from 525 nm to 515 nm and the threshold was only 725 mW. 相似文献
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We describe the output performances of the 1030 nm transition in Yb:YAG under in-band pumping with diode laser at the 968
nm wavelength. An end-pumped Yb:YAG crystal yielded 1.93 W of continuous-wave (CW) output power for 9.1 W of absorbed pump
power. The slope efficiency with respect to the absorbed pump power was 23.6%. Furthermore, 205 mW 515 nm green light was
acquired by frequency doubling, resulting in an optical-to-optical efficiency with respect to the absorbed pump power of 2.7%.
Comparative results obtained for the pump with diode laser at 940 nm are given in order to prove the advantages of the in-band
pumping. 相似文献
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A LD-pumped, LBO intracavity frequency doubled and Cr:YAG passively Q-switched Nd:YAG green laser was reported in this letter. With 600 mW incident pump laser, Q-switched green laser with average power of 27 mW, pulse width of 15.2 ns, repetition rate of 16.4 kHz and peak power of 108.1 W was obtained. 相似文献
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The study of green laser performances by using composite crystals of different initial transmissions
This paper reported a passively Q-switched green laser of LD pumped linear cavity structure by using Nd:YAG/Cr4+:YAG composite crystal and the type II phase matching KTP crystal. The dependence of average output power, pulse width and pulse repetition rate on pump power at different initial transmissions of Cr4+:YAG were measured and analyzed. With Cr4+:YAG of 80% initial transmission, under pump power of 13.97 W, the output average power is up to 681 mW, with pulse width of 200 ns and pulse repetition rate of 9.1 kHz. The laser operates in a fundamental mode. 相似文献
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利用外腔谐振倍频获得高效倍频绿光 总被引:3,自引:0,他引:3
用全固化单频Nd:YAG激光器输出的红外激光泵浦由分离元件组成的MgO:LiNbO3倍频腔。通过优化倍频腔的结构,在倍频腔的红外激光输入为440mW时,获得330mW单纵模绿光输出,倍频效率达75%。 相似文献