共查询到20条相似文献,搜索用时 15 毫秒
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We demonstrated the generation and characterization of 9.7 fs, 180 J pulses centered at 385 nm via the frequency doubling of few-cycle near-infrared pulses. Both moderate conversion efficiency(9.5%) and broad phase matching bandwidth(20 nm) were achieved by shaping the spectra of the fundamental pulses. The strong intensity dependence of second-order harmonic generation and well controlled material dispersion ensured the inexistence of satellite pulses, which was confirmed by the self-diffractio... 相似文献
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WANG Wenbo GAO Weijian YIN Jianping WANG Yuzhu 《Chinese Journal of Lasers》1998,7(2):108-114
TheoreticalAnalysisandExperimentalStudyonGenerationofaDarkHolowBeambyaMicron┐sizedHolowOpticalFiberWANGWenbo1,2GAOWeijian2YI... 相似文献
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《光子学报》2015,(9)
利用飞秒脉冲诱导生成的具有渐变折射率分布的等离子体通道产生空心光束.当飞秒脉冲在非线性介质中传输时将电离产生等离子体通道,该等离子体通道具有渐变的折射率分布,等离子体通道中激光束只能在电子密度低于临界等离子体密度的区域传播,故当探测光束在等离子体通道边缘传输时将偏转形成空心光束.当泵浦光束功率为8mW时,探测光束转变为典型的空心光束结构;当泵浦光束的入射功率、重复率或等离子体通道中轴向电子密度改变时,等离子体通道中可供探测光束通过的区域将随之发生改变,这将导致空心光束中黑斑的面积发生变化.因此通过调节泵浦光束的入射功率和重复率可以控制产生空心光束的黑斑大小. 相似文献
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光纤放大器中的自相似抛物脉冲 总被引:1,自引:1,他引:0
本文研究在含有增益色散、增益饱和、三阶色散、自频移、自陡峭等效应的光纤放大器中自相似抛物脉冲的产生和传输。结果表明,在渐近约束条件下,自相似脉冲的中心区域可用倒置的抛物脉冲来描绘,并且它的有效脉宽和功率都是线性增长的,而峰值振幅和频谱宽度保持常量。数值模拟结果与理论预期符合的非常好,这表明:在光纤放大器中,在适当的条件下初始输入脉冲可自相似地演化为抛物脉冲。 相似文献
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Isolated attosecond pulses with a duration of 88 as are generated in the spectral range of 29-72 eV using double optical gating technique.The gate width is set to be shorter than half the optical cycle to avoid carrier envelop phase stabilization of the 4.2 fs driving laser pulses centered at 800 nm.The attosecond pulse duration is measured with the technique of frequency resolved optical gating for complete reconstruction of attosecond bursts. 相似文献
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Kolykhalova E. D. Dyudelev V. V. Zazulin S. V. Losev S. N. Deryagin A. G. Kuchinskii V. I. Efanov M. V. Sokolovskii G. S. 《Technical Physics》2017,62(12):1885-1888
Technical Physics - Fiber-coupled semiconductor lasers are studied under pumping with high-power short current pulses. Appropriate parameters of the current pumping make it possible to... 相似文献
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OPA泵浦保偏光子晶体光纤产生超连续谱和非线性特性的研究 总被引:4,自引:8,他引:4
采用波长可调光参量放大器作为泵浦源,对保偏光子晶体光纤的超连续谱的产生和非线性特性进行了实验研究.将光参量放大器产生的中心波长为1.27 μm,脉宽约为250 fs,重复频率为250 kHz和单脉冲能量只有92 nJ的光脉冲耦合进0.2 m长的保偏光子晶体光纤,实验中观察到了光谱展宽和非线性效应,在1.3 μm 波长区域获得了谱宽为83 nm (1.2486 ~1.3318 μm)的超连续谱. 相似文献
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光纤中基于交叉相位调制的超短光脉冲串的产生 总被引:4,自引:1,他引:3
提出一种在单模光纤正常色散区由连续波产生超短光脉冲串的新方法,即让连续波和一个波长位于光纤正常色散区的调制脉冲串在光纤中同时传输,交叉相位调制效应和群速度色散效应的相互作用能使连续波演化成一串超短光脉冲,其脉冲宽度比调制脉冲串中的脉宽要小得多,本文还通过计算机模拟,对这一方法进行了全面的考察和分析。结果表明,该方法不仅实用,而且可取得较好的效果。 相似文献
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A theoretical model of ultrashort pulse difference-frequency generation (DFG) is presented and developed with quasi-phase
matching (QPM) gratings in the undepleted-pump, unamplified-signal approximation. An analytic solution to a case of ultrashort
pulse pumped DFG process, including group-velocity mismatching effects and input pulses with frequency chirp and time delay,
is obtained. The influences of group-velocity mismatching effects and input signal pulse parameters on the conversion efficiency
and output converted pulse characteristics are analyzed and discussed. The results indicate that the conversion efficiency
is increased due to the enhancement of pump and signal interaction. The output pulse is inevitable compressed under pulsed
pumping and can be compensated by introducing the initial frequency chirp and time delay. 相似文献
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在理论上研究了超短强激光脉冲与毛细管中惰性气体相互作用产生高次谐波的最佳相位匹配条件,在计算中发现了特定级次 相位匹配中截止驱动光强的存在。分析表明要想使高次谐波获得相位匹配,需要超短脉宽的驱动脉冲以及电离能大的气体工作介质。讨论了毛细管波导中的强场高次谐波选择性并指出了改善谐波选择性的措施。 相似文献
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凹形色散分布光纤中超连续谱特性分析 总被引:5,自引:0,他引:5
比较了在不同色散分布的色散渐减光纤中超连续(SC)谱的产生。结果表明,当光纤的色散值关于中心波长对称、且随着传输距离增加,经由反常色散区过渡到正常色散区的、凹形色散分布的色散渐减光纤更有利于产生平坦、带宽的超连续谱。从频域的全场方程出发,模拟了脉冲在光纤中的传输情形,发现脉冲在凹形色散分布的光纤中传输时,不仅在反常色散区能更大程度被压缩,在正常色散区由于存在零色散波长点,还能更进一步展宽,从而得到更宽、更平坦的超连续谱。在谱强为-27dB时,谱宽可达到298nm,比相同情况下的凸形色散的光纤中超连续谱增宽97nm。结果显示,凹形色散分布的光纤比凸形色散分布的光纤在超连续谱的产生上有更明显的优势,可以得到更宽的超连续谱。 相似文献
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《中国物理快报》2017,(7)
We demonstrate a self-starting erbium fiber oscillator-amplifier system based on the nonlinear polarization rotation mode-locked mechanism. The direct output pulse from the amplifier is 47 fs with an average power of 1.22 W and a repetition rate of 50 MHz, corresponding to a pulse energy of 24 nJ. The full width at half-maximum of the spectrum of the output pulses is approximately 93 nm at a central wavelength of 1572 nm so that the transformlimited pulse duration is as short as 39 fs. Due to the imperfect dispersion compensation, we compress the pulses to 47 fs in this experiment. 相似文献