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激光二极管抽运Cr4+:Nd3+:YAG自锁模自调Q激光器 总被引:1,自引:0,他引:1
采用光纤耦合半导体激光抽运,实现了Cr4+:Nd3+:YAG自锁模自调Q激光器1.06üm激光输出.当抽运功率超过阈值2.83 W时,激光器便运转在调Q锁模状态,其锁模调制深度达到80%以上.当抽运功率最大为5.72 W时,平均输出功率为233 mW,相应调Q包络的单脉冲能量为16.5üJ,调Q包络的脉冲宽度大约为120 ns.调Q包络中锁模脉冲之间的间隔为2.8 ns,这与光子在谐振腔内的往返时间相一致,对应的重复率为357 MHz,锁模脉冲宽度估计为560 ps.利用双曲正割函数,考虑腔内光子数密度的空间高斯分布、增益介质的受激辐射寿命和饱和吸收体的激发态寿命对激光特性的影响,建立了描述Cr4+:Nd3+:YAG晶体自调Q自锁模动力学过程的速率方程组.数值求解该方程组,与实验结果符合较好. 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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富勒烯抑制自由运转的Nd:YAG激光器中的自锁模 总被引:1,自引:1,他引:0
研究了放在Nd:YAG激光腔内的含富勒烯样品对激光波形的影响。实验发现,富勒烯的强非线性吸收可用于光滑纳秒范围的自锁模脉冲序列,估计这是由于双光子吸收引起的。 相似文献
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自调Q、自锁模铒/镱共掺光纤激光器 总被引:3,自引:1,他引:3
研究了结构新颖的环形腔铒/镱(Er/Yb)共掺双包层光纤激光器.为了获得高功率激光输出,使用6个激光二极管(LD)同时抽运Er/Yb共掺光纤,采用光纤光栅(FBG)Sagnac环作为波长选择器,得到了中心波长为1548.11 nm、谱线宽度为0.06 nm的窄线宽激光输出;并利用增益光纤作为可饱和吸收体,实现了自调Q、自锁模脉冲输出.当抽运功率为719 mW时,激光器输出自调Q脉冲,脉冲周期为20μs,脉冲宽度为2.8μs,脉冲的平均功率为38.4mW,峰值功率为274.3mW;当抽运功率为3.6 W时,激光器输出自锁模脉冲,脉冲宽度为4ns,平均功率为319 mW,脉冲峰值功率大于10 W,重复频率为7.937 MHz. 相似文献
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以高纯α-Al2O3、Y2O3、Nd2O3和Cr2O3粉体为原料,CaO为电荷补偿剂,正硅酸乙酯(TEOS)为烧结助剂,采用固相反应法和真空烧结技术成功制备了高质量的Cr4 ,Nd3 :YAG透明陶瓷.研究了其在室温下的吸收光谱和发射光谱性质,O.1%Cr,1.0%Nd:YAG(Cr,Nd为摩尔分数,下同)透明陶瓷在808 nm处的吸收截面为4.27×10-20 cm2,1 064 nm处的发射截面和荧光寿命分别为1.52×10-20 cm2和206μs.由Cr4 ,Nd3 :YAG透明陶瓷的吸收和发射光谱计算出的吸收和发射截面,进一步估算了材料的激光性能参数,并对其激光性能进行理论预测.Cr,Nd:YAG透明陶瓷很可能是一种具有潜力的自调Q激光材料. 相似文献
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利用Nd:YVO4激光晶体的自受激拉曼效应,结合Cr:YAG被动锁模技术和倍频技术,实现了结构紧凑的1176 nm和588 nm黄光锁模激光输出。激光器为LD端面泵浦,三镜折叠腔结构,并且采用了透过率为10%的输出镜。Nd:YVO4晶体长度为10 mm,Nd3+离子掺杂质量分数为0.2%,Cr:YAG晶体的初始透过率为67%。10 W激光泵浦时,1176 nm激光平均输出功率为123 mW,调Q包络宽度为6 ns,调Q包络内的锁模脉冲重复频率高达1 GHz。588.2 nm 黄光的平均输出功率为8 mW。 相似文献
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The self-Q-switched laser performance of monolithic Cr4+,Nd3+:YAG concave-planar resonator with 5-mm length was studied experimentally and theoretically. The slope efficiency is as high as 24% and pump threshold is as low as 64 mW. The pulse width, the single pulse energy and the pulse repetition rate of monolithic Cr,Nd:YAG self-Q-switched laser were measured as a function of absorbed pump power. With the increase of pump power, the pulse width decreases and the pulse energy and the pulse repetition rate increase. The average output power of 91 mW with pulse width of 7 ns at repletion rate of 35.5 kHz was obtained at the maximum absorbed pump power of 440 mW, the peak power is as high as 370 W. The theoretical prediction of pulse energy, pulse width and pulse repetition rate as a function of absorbed pump power based on rate equations is in a good agreement with our experimental data. This can lead to develop the diode laser-pumped monolithic self-Q-switched solid-state microchip lasers. 相似文献
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The dynamic and laser characteristics of the self-Q-switched Cr,Yb:YAG laser were studied by solving the coupled rate equations; the effects of the pump rate, reflectivity of the output couplers and the concentrations of the saturable absorbers on the laser performance were investigated in detail and the numerical simulation of the Cr,Yb:YAG lasers was in good agreement with the experimental data. Better laser performance of the Cr,Yb:YAG self-Q-switched laser can be obtained by using high pump rate, higher concentration of the saturable absorber and suitable reflectivity of the output coupler according to our numerical calculations. A typical self-Q-switched laser pulse of 269.5 J pulse energy with 319 ps pulse width (FWHM) at a repetition rate of 3.1 kHz can be obtained with a monolithic laser cavity, which results in 843.5 kW peak power. 相似文献
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The high efficient laser performance of self-Q-switched laser in the co-doped Cr4+,Nd3+:YAG microchip with 1.8 mm thickness was demonstrated. The slope efficiency is varied with the reflectivity of output coupler at 1064 nm, and the highest slope efficiency of 26% was obtained for 95% reflectivity of output coupler at 1064 nm. The pulse width, the single pulse energy and the pulse repetition rate for different reflectivity of the output couplers were measured, and the experimental results agree with the numerical calculations of the passively Q-switched rate equations. This can lead to develop the diode laser pumped monolithic self-Q-switched solid-state microchip lasers, especially for the intracavity frequency-doubled solid-state microchip lasers. 相似文献
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Passive mode locking of a Nd:YAG laser with co-doped Nd, Cr:YAG as saturable absorber 总被引:1,自引:0,他引:1 下载免费PDF全文
We demonstrate the characteristics of relatively low saturation intensity using co-doped Nd, Cr:YAG as saturable absorber for passively mode locking the Nd:YAG laser. The difference of the saturation intensity between Q-switched and mode-locked operation in co-doped Nd, Cr:YAG was only one to two orders of magnitude, while Cr:YAG was generally reported at a difference of five orders of magnitude. More than 80% mode locking modulation depth was achieved at an incident pump power of 4.4W, corresponding to an intracavity intensity of 6×10^4W/cm^2, using a 68cm long plano-concave cavity. 相似文献
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理论和实验研究了LD泵浦Nd∶Gd0.42Y0.58VO4/Cr4+∶YAG被动调Q锁模激光器.在分析Cr4+∶YAG晶体能级结构和调Q锁模物理过程的基础上,通过数值模拟给出了Cr4+∶YAG调Q锁模的参量要求,然后进行了实验验证.实验中Cr4+∶YAG的初始透过率T0分别为86.3%、95%,输出镜的透过率T分别为10%、20%,在其他条件不变的情况下构成四种不同的组合,均实现了激光器的调Q锁模运转.实验结果表明,降低Cr4+∶YAG的初始透过率T0或提高输出镜透过率T有利于获得较好的锁模效果,与理论分析一致. 相似文献
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The absorption and fluorescence spectra of Cr,Yb:YAG crystal were measured. There are two absorption bands at 940 nm and 968 nm although the absorption coefficient is lower than that of the absorption peak of Yb:YAG superimposed in Cr:YAG absorption peak. The emission peak intensity is 4 times lower than that of Yb:YAG, which may be caused by the existence of the ground state absorption of Cr4+ which quenches the Yb3+ emission intensity. Although the emission peak of Cr,Yb:YAG is lower than that of Yb:YAG, there is an advantage of this crystal which combines the saturable absorber and gain medium into one and can be a self-Q switching laser crystal if Cr,Yb:YAG crystal is pumped with high energy power. 相似文献
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报道了腔长为 1.1mm的激光二极管端面抽运的Cr4 +∶Nd3 +∶YAG自调Q微片激光器 ,连续抽运下获得了平均功率为 5~ 18mW、重复频率为 1~ 10kHz的稳定的调Q激光脉冲输出序列。并且对微片激光器的调Q输出激光的单脉冲特性参量、重复频率以及抽运阈值功率等进行了理论研究 ,计算结果和实验结果比较吻合。 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