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Propagation Properties of Controllable Dark Hollow Laser Beams in Uniaxial Crystals Along the Optical Axis

机译:沿光轴单轴晶体中可控暗空心激光束的传播特性

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摘要

Analytical expressions of the ordinary and the extraordinary optical fields of controllable dark hollow laser beams propagating in uniaxial crystals along the optical axis are derived, respectively. The amplitude distribution, the intensity distribution, the distribution of the linearly polarized, the effective beam size, and the kurtosis parameter of the ordinary optical field, the extraordinary optical field, and the controllable dark hollow laser beam are investigated in the different observation planes of the uniaxial crystal, respectively. The amplitude distributions of the x-component of the ordinary and the extraordinary optical fields are both composed of two lobes, while those of the corresponding y-component have four lobes. Upon propagation in the uniaxial crystals, the x-component of a controllable dark hollow laser beam loses its circular symmetry. The intensity distribution of the extraordinary optical field is somewhat similar to that of the ordinary optical field rotating 90 degrees. When the observation plane is far enough, the dark region of the controllable dark hollow laser beam will appear in the sides of the light spot. The distribution of the linearly polarized angle of the controllable dark hollow laser beam is completely different from those of the ordinary and the extraordinary optical fields. When the observation plane is close to the boundary plane, the effective beam size of the controllable dark hollow laser beam is the largest among those of the ordinary optical field, the extraordinary optical field, and the controllable dark hollow laser beam, while the kurtosis parameter of the controllable dark hollow laser beam is the smallest. When the observation plane is far away from the boundary plane, the effective beam size of the controllable dark hollow laser beam is nearly same as that of the ordinary optical field, and the kurtosis parameter of the controllable dark hollow laser beam is the largest.
机译:分别推导出沿着光轴的单轴晶体中传播的普通和非凡光学场的分析表达式。在不同观察平面下研究了普通光学,非光学场的线性极化,有效光束尺寸的分布,有效光束尺寸和峰值参数的幅度分布,强度分布,有效光束尺寸和可控暗空心激光束的单轴晶体分别。普通和非凡光田的X分量的幅度分布均由两个裂片组成,而相应的Y组分的幅度均具有四个裂片。在单轴晶体中繁殖时,可控暗空心激光束的X组件失去了其圆形对称性。非凡光场的强度分布有点类似于旋转90度的普通光学场的强度分布。当观察平面足够远时,可控暗空心激光束的暗区将出现在光点的侧面。可控暗空心激光束的线性偏振角的分布与普通光场的线性偏振角完全不同。当观察平面接近边界平面时,可控暗空心激光束的有效光束尺寸是普通光场,非光学场和可控暗空心激光束的有效光束尺寸,而Kurtosis参数可控暗空心激光束是最小的。当观察平面远离边界平面时,可控暗空心激光束的有效光束尺寸与普通光学场的有效光束尺寸几乎相同,并且可控暗空心激光束的Kurtosis参数是最大的。

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