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本文讨论了分数傅里叶变换与菲涅耳衍射的关系,提出球面衍射过程就是一种具有尺度因子的分数傅里叶变换,并应用分数傅里叶变换进行衍射光学元件的设计。 相似文献
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运用矩阵光学技巧,球面镜光腔的往返一周光束变换矩阵可分解为两矩阵之积,它们各对应于一分数付里叶变换,因而光腔的振荡本质就是不断作用分数付里叶变换的过程。其稳定条件和束腰位置可用分数阶次描述,分数阶次可为复数。同时,给出了可能的拓展。 相似文献
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基于角谱分析的分数傅里叶变换数值模拟算法 总被引:2,自引:0,他引:2
从分数傅里叶变换的表达式入手,分析了分数傅里叶变换与菲涅尔衍射积分之间的关系,针对采用衍射积分的方法计算分数傅里叶变换的局限性,提出了基于角谱分析的数值模拟方法。文中给出了计算方法的理论描述和计算实例。 相似文献
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分数傅里叶变换与菲涅耳衍射的等效性 总被引:8,自引:0,他引:8
用波前相因子判断法,分析了分数傅里叶变换频变分布与球面波照明物体的自由空间菲涅耳衍射光场分布的等效性,给出了分数傅里叶变换与菲涅耳衍射相互转化的约束条件。结果表明:分数傅里叶变换是适应于菲涅耳衍射的数学工具。计算机模拟实验证明了结论的可靠与可行。 相似文献
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利用描述光波傍轴传输的光学分数傅里叶变换基本关系式,对单透镜系统进行分析,结果表明,单透镜系统可实现任意阶分数傅里叶变换,Lohmann第一类光学分数傅里叶变换装置是其特例,单透镜成像过程是进行阶次为π的分数傅里叶变换,进一步表明光学分数傅里叶变换的物理实质是光波的菲涅耳衍射。 相似文献
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A simple but general formulation for the unified analysis of many different varieties of unstable optical resonators is obtained by expressing the round-trip Huygens' integral for the resonator in terms of the round-trip paraxial ray matrix. Complicated multielement resonators, ring resonators, and unstable resonators with variable-reflectivity output mirrors are thereby all reduced to a single equivalent collimated-beam diffraction problem. Essential assumptions in the analysis are that all elements in the resonator obey paraxial ray theory and that there is only one significant output coupler or limiting aperture per round trip inside the resonator. The only parameters needed to describe an arbitrary unstable resonator in this formulation are the round-trip magnificationM and either the equivalent Fresnel number Neq or else an equivalent collimated Fresnel numberN_{c} = [2M^{2}/(M^{2} - 1)] N_{eq} , plus for variable-reflectivity mirrors a specification of the mirror reflectivity profile. 相似文献
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Richard P. Fischer Arne W. Fliflet 《Journal of Infrared, Millimeter and Terahertz Waves》2002,23(9):1297-1313
This paper presents the design and test of asymmetric quasioptical resonators for gyrotron applications, where most of the diffraction output coupling comes from the smaller of two mirrors. A computer code based on scalar diffraction theory is used to calculate the resonator losses and the electric field near the mirrors. Resonators with mirror separations approaching confocal have reduced side lobes in the diffraction patterns, which should allow for better power transmission and focusing. Cold tests have been performed at 94 and 141 GHz to measure the quality factor of the asymmetric resonators as a function of mirror separation and mirror misalignment. Typical resonator parameters include 65 cm mirror separation, 1-3% output coupling and 85% of the losses from the small mirror. A half-symmetric resonator with one flat and one curved mirror has also been investigated. The calculated values of Q are in reasonably good agreement with the cold test measurements. 相似文献
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Unstable optical resonators for laser applications 总被引:2,自引:0,他引:2
A simple geometrical analysis has been developed which describes the lowest-order transverse mode of any large-Fresnel-number optical resonator located in the unstable or high-loss region of the resonator mode chart. Such resonators include, for example, resonators in which one or both of the mirrors are divergent spherical surfaces. The lowest mode in such a resonator is assumed to consist of two oppositely traveling divergent spherical waves which uniformly illuminate the end mirrors. The centers of curvature of these spherical waves do not, in general, coincide with the mirror centers of curvature, but are found by requiring that each center be the image of the other upon reflection from the appropriate mirror. The resonator losses are found from purely geometrical considerations, and are given by simple analytical expressions. These losses turn out to be independent of the mirror sizes, so that hyperbolic universal equiloss contours can be drawn on the resonator mode chart. The losses agree well with more exact results obtained by Fox and Li for a few specific cases. Experimental results in good agreement with the analysis have been obtained using a ruby laser rod having a divergent spherical surface ground directly onto one end of the laser rod. Unstable resonators, particularly the "Cassegrainian" unstable configuration used in the experiments, appear potentially useful for diffraction output coupling applications, and possibly also for transverse mode control, in ruby and other high-gain lasers. 相似文献
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一、概述稳定球面两镜腔的模式理论是建立在其与共焦腔等价的基础上的.在许多文献中,为了证明等价共焦腔存在的唯一性,都假设稳定球面两镜腔本征模式的等相位面曲率半径ρ_(Gi),在腔镜处等于腔镜的曲率半径ρ_i:ρ_(Gi)=ρ_i (1)由于上式并不普遍成立,因此文献[1]的作者对等价共焦腔方法提出质疑.鉴于这个问题的重要性,有 相似文献
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高斯反射率方形平凹腔激光模场的有限元分析 总被引:7,自引:0,他引:7
利用柯林斯公式和边界有限元方法,将方形球面镜腔的衍射积分方程转化为矩阵方程,并对高斯反射率方形平凹腔的模场分布进行了数值计算。研究结果表明,高斯反射率方形平凹腔具有较好的选模性能,可以应用于高功率激光器以获得高质量的激光光束。 相似文献
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本文利用自再现理论,将高斯反射二维腔的衍射积分析方程转化为有限阶国方程,对高斯反射平凹二维腔的横模选择特性进行数值分析,研究结果表明,高斯反射平凹二维腔选横模的性能优越,可应用于大功率激光器,从而为激光材料表面处理提供优质的激光光束。 相似文献
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为了研究激光在高斯镜平凸非稳腔中的模式和相位特征,在SIEGMAN分析多元件非稳腔的理论基础上,采用有限元数值方法计算耦合输出镜镜面反射率为高斯分布的圆镜平凸非稳腔本征模场分布。将光场在腔内一次往返的ABCD系数代入惠更斯-基尔霍夫衍射积分方程,可以写出光场往返一次的衍射积分方程。将镜面分割成若干个等宽圆环,把衍射积分方程转化成矩阵相乘形式,经过数值计算,得到理想空腔和非共轴空腔优先起振的光场本征模式分布结果与相位特性。计算结果表明,当合适选择输出镜半径与高斯反射率分布,可以得到光斑半径为0.3cm的基模高斯光束输出,此计算结果与实验结果相符。同时也讨论了耦合输出镜对光束质量的影响。 相似文献