共查询到16条相似文献,搜索用时 156 毫秒
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在对Nd:YAG调Q激光器进行分析和设计时,研究人员通常选择忽略激光下能级寿命对脉冲波形的影响。当激光脉宽远大于激光下能级寿命时,这种近似一般不会带来太大偏差;而当脉宽达到纳秒量级时,Nd:YAG晶体约30 ns的下能级寿命对脉冲波形的影响会变得非常严重。建立了Nd:YAG下能级寿命对输出脉冲波形影响的理论分析模型,并对窄脉宽的Nd:YAG调Q激光器的输出波形进行仿真研究。研究结果表明,在窄脉宽激光输出情形下,激光下能级寿命会导致调Q脉冲在主峰后出现尾峰,尾峰能量可达主峰能量的一倍以上。同时建立了Nd:YAG声光调Q激光器实验系统,在与仿真计算近似的条件下测量调Q脉冲波形,观察到与仿真结果一致的尾峰现象,实验验证了理论模型的正确性。 相似文献
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复杂激光脉冲波形的整形 总被引:14,自引:1,他引:13
介绍了用时空变换的方法对激光脉冲整形的原理;提出了由于硬边光通量调制器引入的动态的光脉冲强度空间分布的不一致性及其克服的方法,理论上用二维快速傅里叶变换(FFT)进行了验证;最后计算了系统光强透过率和光束焦斑大小,调制狭缝宽度的关系,为了显示本系统的复杂脉冲整形能力,在实验上获得了惯性约束核聚变(ICF)感兴趣的复杂激光脉冲波形。 相似文献
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报道了采用光纤耦合激光二极管(LD)模块端面抽运Nd:YVO4晶体实现高功率、高重复频率声光调Q 1342 nm波长的激光输出,以及采用考虑增益频谱分布的调Q速率方程模型仿真研究该脉冲激光器的结果.在激光器注入总功率40 W的情况下,可得到最高工作重复频率100 kHz;在50 kHz重复频率工作条件下,可得到11.0 W的平均输出功率及稳定的脉冲输出.应用与介质增益频谱相关的调Q速率方程模型对该脉冲激光器进行了仿真研究,得到了脉冲宽度、脉冲峰值功率、脉冲建立时间等计算结果,还给出了输出在频谱上的分布以及谱宽,并与实验结果进行了比较.考虑增益频谱分布的调Q速率方程模型不仅可以应用于分析、设计脉冲激光器的频谱,而且由于考虑了增益在频谱上的实际分布,基于该模型的仿真计算可以获得比传统单频调Q速率方程更为接近实际的结果. 相似文献
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A new method to investigate fast frequency modulation of a laser diode by applying optical pulse irradiation is presented. The self-delayed heterodyne technique and an autocorrelation method are used to detect beat in the heterodyne signal due to frequency shift by the irradiation. Autocorrelation of the beat signal is suggested to be calculated via its spectrum. 相似文献
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窄脉冲相干激光雷达偏频锁定系统仿真研究 总被引:1,自引:0,他引:1
鉴于偏频锁定技术在激光外差探测和激光雷达等方面的广泛作用,基于可编程逻辑器件,设计了适用于窄脉冲激光外差信号的偏频锁定控制系统。在设计中,使用超高速电压比较器进行波形变换、多脉冲鉴频和大概率均值滤波进行数字鉴频,采用小步长快速控制方法进行调频,利用数模转换器和线性放大电路输出调频信号。借助信号发生器产生40ns脉宽的模拟外差信号对系统进行了仿真,实现了设计功能。对系统进行鉴频和调频测试,在40ns脉宽时鉴频误差范围为-7.5MHz~+7.7MHz。 相似文献
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We demonstrated a 1.91 μm pumped, injection-seeded Q-switched Ho:YAG laser operating at room temperature. By inserting two Fabry-Perot etalons into the laser cavity, single-frequency Tm, Ho:YAG seed lasing was achieved at a wavelength of 2090.9 nm, with a typical output power of 60 mW. Single-frequency, nearly transform-limited Q-switched operation of the Ho:YAG laser was achieved by injection seeding. The output energy of the single-frequency Q-switched pulse is 7.6 mJ, with a pulse width of 132 ns and a repetition rate of 100 Hz. We measured the pulse spectrum, half-width of which was 3.5 MHz, by a heterodyne technique. 相似文献
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基于啁啾脉冲放大技术的超短脉冲激光系统是提供超快、超强激光的重要途径,具有良好输出波形和高损伤阈值的多层介质膜脉冲宽度压缩光栅是获得高峰值功率脉冲激光的关键. 基于傅里叶谱变换方法和严格模式理论,分析了多层介质膜光栅(MDG)在超短脉冲作用下的光学特性. 结果表明,当MDG的反射带宽小于具有高斯分布的入射脉冲的频谱宽度时,-1级反射脉冲呈非对称高斯分布,其前沿出现振荡,并且-1级反射脉冲能量开始剧烈下降. 讨论了MDG结构参数对其反射带宽的影响. 分析了MDG与超短脉冲作用时的近场光分布,对提高其抗激光损
关键词:
脉冲压缩光栅
傅里叶谱变换
模式理论
损伤阈值 相似文献
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T. Y. Dai Y. L. Ju X. M. Duan W. Liu B. Q. Yao Y. Z. Wang 《Applied physics. B, Lasers and optics》2013,111(1):89-92
A 1.91 μm-pumped, injection-seeded 2,118 nm Q-switched Ho:YAlO3 laser was demonstrated in this paper. Single-frequency and nearly transform-limited operation of Q-switched Ho:YAlO3 laser was achieved by injection-seeded. The single-frequency Q-switched Ho:YAlO3 laser output energy of 8 mJ at 100 Hz with a pulse width of 151 ns was obtained. The half-width of pulse spectrum measured by a heterodyne technique was 3.7 MHz. 相似文献
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A method of measuring micro-impulse with torsion pendulum based on multi-beam laser heterodyne 下载免费PDF全文
In this paper, we propose a novel method of multi-beam laser heterodyne measurement for micro-impulse. The measurement of the micro-impulse, which is converted into the measurement of the small tuning angle of the torsion pendulum, is realized by considering the interaction between pulse laser and working medium. Based on Doppler effect and heterodyne technology, the information regarding the small tuning angle is loaded to the frequency difference of the multi-beam laser heterodyne signal by the frequency modulation of the oscillating mirror, thereby obtaining many values of the small tuning angle after the multi-beam laser heterodyne signal demodulation simultaneously. Processing these values by weighted-average, the small tuning angle can be obtained accurately and the value of the micro-impulse can eventually be calculated. Using Polyvinylchlorid+2%C as a working medium, this novel method is used to simulate the value of the micro-impulse by MATLAB which is generated by considering the interaction between the pulse laser and the working medium, the obtained result shows that the relative error of this method is just 0.5%. 相似文献