共查询到20条相似文献,搜索用时 171 毫秒
1.
2.
相干合成技术是实现高功率、高亮度光纤激光系统的重要技术途径.然而, 脉冲激光阵列中常常存在时域误差,这将影响脉冲激光的相干合成效果. 建立了脉冲激光存在时域误差时的相干合成理论模型,并在不同波形(方波、三角波、正弦波) 的脉冲激光存在时域误差时,对相干合成光束在远场的脉冲波形、峰值功率、 光强分布和桶中功率(PIB)等特性进行了数值计算和对比分析.计算结果表明: 方波脉冲激光相干合成光束的脉冲波形受时域误差影响严重,光强分布和PIB随着时域误差 的增大发生线性变化;三角波脉冲激光相干合成光束的脉冲波形和峰值功率受时域误差 影响严重,光强分布和PIB在时域误差较大时随着时域误差的增大发生较为剧烈的变化; 正弦波脉冲激光相干合成光束具有较好的输出特性,在两路正弦波脉冲激光相干合成中, 将两脉冲之间的时延控制在脉冲持续时间的10%以内,就能取得良好的合成效果. 相似文献
3.
利用超短脉冲放大过程中的光谱增益窄化效应以及标准具的滤波作用,提出了基于再生放大器的多脉冲相干叠加方案,并对该方案在多脉冲叠加阶段的工作原理进行了分析;在小信号增益区内,对多个超短脉冲相干叠加进行了理论分析和数值计算,数值模拟的结果表明,影响形成窄带平顶长脉冲的基本关系为子脉冲宽度、再生放大器中的损耗及其与振荡器的长度失配量对构成脉冲时间波形影响很大,而对其频谱影响很小;叠加脉冲个数、标准具的通带宽度对构成脉冲波形和光谱均有影响.
关键词:
超短脉冲
多脉冲叠加器
窄带平顶长脉冲
数值计算 相似文献
4.
5.
6.
采用两束圆偏振啁啾飞秒激光脉冲,非共线相干激发三原子分子CS2液体. 在相位匹配的方向上,探测到由CS2频率为397 cm-1的振动模式产生的强度对称分布的相干反斯托克斯拉曼散射(CARS)信号和相干斯托克斯拉曼散射(CSRS)信号. 当调整两束激发光的圆偏振状态时,CARS,CSRS信号的强度、偏振、波长均发生规律性的改变:CARS,CSRS信号的强度分布反映了CS2 在不同极化状态下的受激拉曼散射截面大小;信号光的
关键词:
啁啾脉冲
相干反斯托克斯拉曼散射(CARS)
相干斯托克斯拉曼散射(CSRS)
2')" href="#">CS2 相似文献
7.
从实验和理论上研究了受激布里渊散射(SBS)光脉冲波形.在Nd∶YAG调Q激光器中实验研究了SBS光脉冲波形随抽运光参数、结构参数和介质参数的变化规律,并利用SBS理论模型进行了数值模拟,实验与数值模拟结果的变化趋势基本一致.结果表明,抽运光能量越小,透镜焦距越短,镜-池间距越长,介质声子寿命越长,SBS光脉冲波形就越不容易出现调制现象.分析和讨论了抽运光参数、结构参数和介质参数对SBS光脉冲波形的影响机理.
关键词:
受激布里渊散射
脉冲波形
抽运光参数
结构参数 相似文献
8.
9.
在理论上介绍了用非相干光和相干的激光脉冲实现二能级或三能级原子或分子能态间转移的各种方法,包括光泵浦,受激辐射泵浦,共振相干激发,受激拉曼绝热过程(STIRAP),并在转移的效率和转移速度等方面进行了比较,指出适当运用相干脉冲序列转移粒子数要优于非相干脉冲,特别是受激拉曼绝热过程(STIRAP),可以实现粒子数的完全快速转移. 相似文献
10.
使用复互相干度的定义对时域光波分裂前后以及不同输入噪声、不同初始啁啾和波形下抽运脉冲在高非线性光纤中产生的超连续谱的相干度进行了数值计算,得到了光波分裂前后和不同输入噪声下生成的超连续谱的演化和相干性变化,结果表明:皮秒脉冲在高非线性光纤正常色散区产生超连续谱的相干性主要受到系统中噪声占比的影响,其中由光波分裂生成的频谱旁瓣的相干度低于由自相位调制生成的中心频谱的相干度:抽运脉冲啁啾和波形对在高非线性光纤正常色散区产生超连续谱的相干性的影响不明显,若想获得高相干的超连续谱,需要采用低噪声的脉冲进行抽运;若获得大谱宽高相干度的超连续谱,则需要合理选择皮秒脉冲的功率。 相似文献
11.
We study the quantum statistical properties of radiation in higher-order parametric processes and higher harmonic generation. Adopting the Heisenberg picture, we use the short-time approximation to solve the Heisenberg equations and to calculate the quantum characteristic functions and quasi-distributions. The lossy mechanism is included with or without rotating terms. We show that the statistical properties of radiation involved in these non-linear optical processes are described by the model of the superposition of coherent and chaotic fields with correlated components in this approximation. Generalizations of the well-known conservation laws for the number operators are derived. We show for parametric processes that the pumping mode has tendency to be coherent while the signal modes are obtaining a noise. In the higher-harmonic generation, the basic radiation is losing its coherence proportionally to its intensity while the generated higher-harmonic radiation has tendency to be coherent.The part of this paper devoted to thek-th harmonic generation describes a portion of the Diploma Work. 相似文献
12.
James H. Churnside 《Optics Communications》1984,51(3):207-212
The second harmonic generation process is considered using partially coherent light formed by the superposition of a coherent field and a chaotic field. The conversion efficiency is derived. Expressions are also presented for the variance and for the probability density function of the second harmonic intensity and of the transmitted intensity at the fundamental wavelength. 相似文献
13.
There are two physical phenomena in a strong laser intensity. One is the high-order harmonic emission; the other is x-ray emission from optical-field ionized plasmas. The experiment of conversion from high-order harmonics to x-ray emissions was given with a 105fs Ti:sapphire laser by adjusting laser intensities. The ingredient in plasma was investigated by the numerical simulations.Our experimental results suggested that the free electrons have detrimental effects on harmonic generation but are favourable for x-ray emission from optical-field ionized plasmas. If we want to obtain more intense harmonic signals as a coherent light source in the soft x-ray region, we must avoid the production of free electrons in plasmas. At the same time, if we want to observe x-rays for the development of high-repetition-rate table-top soft x-ray lasers, we should strip all atoms in the plasmas to a necessary ionized stage by the optical-field-ionization in the field of a high-intensity laser pulse. 相似文献
14.
15.
The statistical properties of the second harmonic and subharmonic are investigated on the basis of the generalized Fokker-Planck equation making use of the coherent state technique. An iterative procedure of solving the Fokker-Planck equation is adopted making it possible to obtain some recursion equations, particularly two iterations are explicitly performed providing approximate solutions for the normal and antinormal characteristic functions. Higher-order corrections to the superposition of coherent and chaotic fields are found in the subharmonic mode or if the coupling of modes is taken into account. Earlier results for the anticorrelation effect are rederived, the reservoir effect is obtained and the related problems of the existence of the Glauber-Sudarshan quasidistribution are discussed. 相似文献
16.
研究了简谐噪声激励下的FitzHugh-Nagumo神经元模型, 其放电形式、相干共振等动力学行为均受噪声阻尼参数和频率参数的影响.选择不同的参数所得到的神经元的放电形式不同.神经元存在共振特性,对某一频率的噪声有更强的响应,在此频率参数下的峰序列更有序,出现相干共振系数的极小值.噪声的阻尼参数越大,不同的频率成分越多,神经元的响应也变得杂乱,进而导致神经元与噪声的同步变弱,峰序列相干共振系数也相应增大. 相似文献
17.
通过数值求解含时Schr ö dinger方程,研究了氦离子在不同双色场下的高次谐波。结果显示,尽管倍频光强度仅为基频光的1/10,高次谐波辐射却发生了极大变化。虽然谐波级次推进不多,但效率大大提高了,平台区平均提高103倍,高倍频光对应的高次谐波产生效率提高104~105倍。氦离子在添加倍频光的双色场作用下高次谐波产生效率极大提高的原因是:倍频光极大地加快了电子电离到连续态及返回基态这一过程,使辐射出的高次谐波光子数大大增加,该初步阐释可为高次谐波真正应用到实际中提供一些理论启示。 相似文献
18.
研究了简谐噪声激励下的FitzHugh-Nagumo神经元模型, 其放电形式、相干共振等动力学行为均受噪声阻尼参数和频率参数的影响.选择不同的参数所得到的神经元的放电形式不同.神经元存在共振特性,对某一频率的噪声有更强的响应,在此频率参数下的峰序列更有序,出现相干共振系数的极小值.噪声的阻尼参数越大,不同的频率成分越多,神经元的响应也变得杂乱,进而导致神经元与噪声的同步变弱,峰序列相干共振系数也相应增大.
关键词:
简谐噪声
FitzHugh-Nagumo神经元
相干共振
峰峰间隔 相似文献
19.
J. Peřina 《Czechoslovak Journal of Physics》1976,26(2):140-150
We study the statistical properties of parametric processes (parametric amplification, frequency conversion, splitting of frequency, etc.) described by the trilinear Hamiltonian and of the second harmonic generation including the lossy mechanism and rotating terms. In a short-time approximation some conservation laws are derived and the existence of the Glauber-Sudarshan weighting function is discussed. It is shown in the second harmonic generation case that good coherence of the incident radiation is lost proportionally to the intensity in interaction while the second harmonic radiation has tendency to be coherent. The effects of the spontaneous emission of the medium and of the physical vacuum are also discussed. In this approximation the statistics is generally described by the superposition of coherent and chaotic fields with correlated components. 相似文献
20.
We investigate the nonlinear optical interaction through a periodic waveguide structure consisting of two alternating segments with different linear and nonlinear optical properties. A coupled equation system has been used to calculate the intensity of fundamental and second harmonic waves and the phase shift of the fundamental. The model has been experimentally tested with good results, but the effect of the phase shift has not been considered. Comparison with the quasi-phase match (QPM) technique has been presented. The novel features introduced by alternating segments with different linear and nonlinear optical properties have been discussed. The model shows a more flexible approach, which can be used in designing optical components based on coherent nonlinear interaction. Applications are straightforward for frequency doubler and all-optical switch. 相似文献