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Kerr-lens mode-locked polycrystalline Cr:ZnS femtosecond laser pumped by a monolithic Er:YAG laser 下载免费PDF全文
We demonstrated a Kerr-lens mode-locked polycrystalline Cr:ZnS laser pumped by a narrow-linewidth linearpolarised monolithic Er:YAG nonplanar ring oscillator operated at 1645 nm. With a 5-mm-thick sapphire plate for intracavity dispersion compensation, a compact and stable Kerr-lens mode-locking operation was realised. The oscillator delivered 125-fs pulses at 2347 nm with an average power of 80 m W. Owing to the special polycrystalline structure of the Cr:ZnS crystal, the second to fourth harmonic generation was observed by random quasi-phase-matching. 相似文献
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Nd:YAG激光器中的自锁模 总被引:3,自引:2,他引:3
本文报道在Nd:YAG激光器中首次获得的自锁模脉冲序列.自锁模是由于Nd:YAG棒中的自相位调制引起的.在主被动对撞锁模运转情况下,自锁模对脉冲波形有较大的影响. 相似文献
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Weili Zhang Ching-yue Wang Jiangshan Zhao Lu Chai Qirong Xing 《Optics & Laser Technology》1998,30(8):551-554
We report a blue-lines pumped femtosecond Kerr-lens mode-locked Cr:LiSGaF laser based on a tight-focusing geometry. With a combination of 488, 476 and 458 nm lines as a pump source, 58 fs pulses centered at 845 nm were generated. The average output power is 30 mW, and time–band product is 0.331, assuming a sec h2 pulse shape. Neither acousto-modulator nor physical aperture or slit were used in this cavity. 相似文献
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Hirano Y Yanagisawa T Ueno S Tajime T Uchino O Nagai T Nagasawa C 《Optics letters》2000,25(16):1168-1170
A high-average-power conduction-cooled diode-pumped Nd:YLF rod laser has been developed. A new conduction-cooled side-pumping scheme with a solid prismatic pump-light confinement cavity was employed. A transparent, high-thermal-conductivity MgF>(2) prism was used as a highly efficient pump cavity as well as a low-thermal-resistance heat spreader. The pumping efficiency and thermal resistance of the cavity were 85% and 0.20 degrees C degrees W, respectively. When this scheme was combined with heat pipes for heat removal, a maximum average output power of 72 W was demonstrated, with an optical slope efficiency as high as 49%. 相似文献
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Jianqiang Zhu Zhuhong Zhang Shaohe Chen Taolue Chen Youming Chen Qirong Lu Xiaodong Guo Dianyuan Fan Ximing Deng 《Chinese Journal of Lasers》1993,2(2):109-112
A picosecond colliding pulse mode-locked Nd: YLF laser with negative feedback provided by GaAs photoconductive switch was described. Optical pulse with~4ps duration, 10μJ energy and about 7μs long pulse train were generated. 相似文献
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The design and operation characteristics of a distributed feedback dye laser (DFDL) system pumped by the second harmonic of a flashlamp pumped mode-locked Nd: YAG laser are described. The DFDL oscillator facilitates a large tuning range with nearly Fourier limited pulse durations of about 1.6 ps. The combined action of saturated absorption and amplification results in a pulse shortening to about 600 fs, with small fluctuations in the pulse duration. Output pulse energies of more than 400 J are achieved, corresponding to a peak power of more than 650 MW. Since the dye amplifiers are pumped by pulses of only 25 ps duration the amplified spontaneous emission (ASE) is very low, typically less than 10–4. 相似文献
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CW acousto-optical mode-locked diode pumped Tm:YAlO3 laser at 1.936 μm was experimentally studied. Lasing with output power ~100 mW, pulse repetition rate 103.4 MHz and laser pulse durations in the range of 30–200 ps was realized. The problem of laser intensity stabilization is discussed. 相似文献
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Fiber optical parametric oscillator based on photonic crystal fiber pumped with all-normal-dispersion mode-locked Yb:fiber laser 下载免费PDF全文
We demonstrate a cost effective, linearly tunable fiber optical parametric oscillator based on a home-made photonic crystal fiber pumped with a mode-locked ytterbium-doped fiber laser, providing linely tuning ranges from 1018 nm to 1038 nm for the idler wavelength and from 1097 nm to 1117 nm for the signal wavelength by tuning the pump wavelength and the cavity length. In order to obtain the desired fiber with a zero dispersion wavelength around 1060 rim, eight sam- ples of photonic crystal fibers with gradually changed structural parameters are fabricated for the reason that it is difficult to accurately customize the structural dimensions during fabrication. We verify the usability of the fabricated fiber experimen- tally via optical parametric generation and conclude a successful procedure of design, fabirication, and verification. A seed source of home-made all-normal-dispersion mode-locked ytterbium-doped fiber laser with 38.57 ps pulsewidth around the 1064 nm wavelength is used to pump the fiber optical parametric oscillator. The wide picosecond pulse pump laser enables a larger walk-off tolerance between the pump light and the oscillating light as well as a longer photonic crystal fiber of 20 m superior to the femtosecond pulse lasers, resulting in a larger parametric amplification and a lower threshold pump power of 15.8 dBm of the fiber optical parametric oscillator. 相似文献
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We first experimentally demonstrate a laser-diode end-pumped self-Q-switched and mode-locked Nd,Cr:YAG green laser with a KTP crystal as the intra-cavity frequency doubler. The device produces
an average output power of 680 mW at 532 nm. The corresponding pulse width of the Q-switched envelope of the green laser is 170±20 ns. The mode-locked pulses have a repetition rate of approximately 183
MHz and the average pulse duration is estimated to be around sub-nanosecond. It is found that the intra-cavity frequency doubling greatly improves the modulation depth and stability of the
mode-locked pulses within the Q-switched envelope. 相似文献
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用脉冲输出功率50mW,中心波长为800nm的双异质结激光二极管列阵泵浦磷酸盐钕璃璃激光器,得到1.053μm波长激光输出.泵浦阈值功率为9mW.计算了DPL输出的尖峰功率、脉冲宽度和弛豫振荡波形,与实验结果一致. 相似文献
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利用光纤的非线性偏振旋转效应产生可饱和吸收体的锁模机制,从掺Yb3+光纤环形激光器中得到稳定高阶谐波锁模光脉冲。理论分析了工作于正色散区的掺Yb3+光纤环形激光器的特性。实验中观测到了掺Yb3+光纤环形激光器3种不同演化方式产生高阶锁模光脉冲。4阶谐波锁模脉冲(107.2 MHz重复频率)经过1 m长高掺杂Yb3+光纤放大器放大后产生了平均功率100 mW,脉宽22.8 ps的脉冲,最后经过光栅压缩得到了平均输出功率20 mW,脉宽307 fs,脉冲中心波长1 051.2 nm,带宽13.76 nm的激光。 相似文献
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Jintao Bai Nuo Wangan Petroleum Institute XV an PRC)Jinxing Cai Yibin Zhang Shuicai Wang 《Chinese Journal of Lasers》1992,1(2):101-104
Experimental results of 200 MHz CW actively mode-locked KTP two-pass in-tracavity frequency-doubled Nd:YAG laser are reported.The primary factors influencingthe continuous-wave frequency-doubled conversion efficiency are analyzed.High efficiencylaser output was achieved by L-type folded-arm-cavity two-pass frequency-doubling.15 Waverage mode-locked power and 1.5W average mode-locked SHG green light output were ob-tained at 3.5kW single lamp input power respectively. 相似文献
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A mode-locked external-cavity laser emitting at 1.17-μm wavelength using an InAs/GaAs quantum-dot gain medium and a discrete semiconductor saturable absorber mirror is demonstrated. By changing the external-cavity length, repetition rates of 854, 912, and 969 MHz are achieved respectively. The narrowest -3-dB radio-frequency linewidth obtained is 38 kHz, indicating that the laser is under stable mode-locking operation. 相似文献
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We have demonstrated passively Q-switched mode-locked all-solid-state Nd:YLF laser with an uncoated GaAs wafer as saturable absorber and output mirror simultaneously. Q-switched mode-locking pulses laser with about 100% modulation depth were obtained. The average output power is 890 mW at the incident pump power of 5.76 W, corresponding to an optical slop efficiency of 20%. The temporal duration of mode-locked pulses was about 21 ps. At the Q-switched repetition rate of 30 kHz, the energy and peak power of a single pulse near the maximum of the Q-switched envelope was estimated to be about 1.6 μJ and 76 kW. 相似文献
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E. Roissé V. Couderc A. Barthélémy F. Louradour 《Applied physics. B, Lasers and optics》1999,69(2):89-91
We report the first diode-pumped solid-state laser operating in cw-mode-locked regime and simultaneously achieving intracavity
frequency-tripling. This laser provide UV picosecond pulses (λ=355 nm) of 10 ps duration with 0.5 mW average power at 150 MHz
repetition rate. A different set of adjustments gave rise to a Q-switched mode-locked regime. Trains of hundred UV pulses
of 60 ps duration and 4 W peak power were produced in this latter case at 50 kHz repetition rate.
Received: 12 October 1998 / Revised version: 12 December 1998 / Published online: 26 May 1999 相似文献