排序方式: 共有52条查询结果,搜索用时 15 毫秒
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非线性热晕效应自适应光学位相补偿 总被引:2,自引:1,他引:2
采用已建立的一套较完整的包括真实自适应光学位相补偿系统仿真的高能激光大气传输的数值模拟程序,对非线性热晕应相偿进行了计算。分析了非线性热晕效应位相补偿不稳定性的基本特征。 相似文献
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An analytical expression for the average intensity of four-petal Gaussian beams in turbulent atmosphere is derived. Studies show that in turbulent atmosphere, the contour lines of four-petal Gaussian beams with lower order N evolve into a number of petals with the increase in propagation distance, the contour lines with higher order N can reserve four-petal distribution at longer propagation distance than that with lower order N. These properties are similar to those in free space. However, with further increases of the propagation distance, the contours lines in turbulent atmosphere are different from those in free space. 相似文献
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扩展物体漫反射光传输及成像的数值模拟研究 总被引:4,自引:1,他引:4
对扩展漫反射体的成像进行了数值模拟研究,利用近轴近似标量波动方程及其分步相屏算法,对漫反射体反射的相对于接收孔径光轴的近轴光传输及其成像进行数值模拟计算分析,结果表明该模拟算法是可行的,也对图像传输的湍流效应进行了初步计算和讨论。 相似文献
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为了提高探测器阵列靶的到靶激光功率密度测量范围及入射角度宽容性,从防护取样衰减结构出发,基于全反射与透射散射理论设计镀金铜基面板、光纤取样和散射片所组成的防护取样衰减结构。同时,将所设计的结构应用于探测器阵列靶系统。通过激光辐照靶面热分析、光线追迹仿真及激光逐点扫描实验,对系统抗激光损伤能力、角度特性及通道响应一致性进行分析测试。结果表明,该防护取样衰减结构可以承受高功率密度激光的长时间辐照;在0°~30°的入射角度范围内,实测角度特性系数经余弦校正后相对于正入射偏差小于4%;各通道单元间的响应不一致性标准差均小于2%。 相似文献
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风速与风向对小尺度热晕不稳定性的影响 总被引:1,自引:0,他引:1
给出了两种特殊风向对小尺度热晕不稳定性扰动能量增长影响的实验及数值计算结果:当风向与扰动梯度方向平行时,风速对不稳定性有明显的抑制作用,而垂直优动梯度方向的风则对热晕不稳定性没有影响。 相似文献
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Comparison between relay propagation and direct propagation of Gaussian-Schell-model beam in turbulent atmosphere along a slant path 下载免费PDF全文
The relay propagation of Gaussian-Schell-model in turbulent atmosphere along a slant path is studied in this paper. Based on the extended Huygens-Fresnel principle and a quadratic approximation, an analytical formula of average intensity for Gaussian-Schell-model beams in turbulent atmosphere along a slant path is derived, and some special cases are discussed. From the study and the comparison with the direct propagation, we can see that the relay propagation has an advantage over the direct propagation. When the altitude of the target is low, the peak intensity of relay propagation is much larger than that of direct propagation. However, because of the limitation of the relay system aperture for relay propagation and the variation of coherence length for direct propagation, the difference in peak intensity between the two propagations decreases with the increase of the target altitude. 相似文献
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