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Focusing by a single lens based on an optically thinner medium

机译:基于光学更薄的介质,通过单透镜聚焦

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This paper investigates the focusing properties by a single lens, based on the optically thinner medium(OTM). The lens model is of a plano-concave shape, made from the OTM with refractive index 0.5 at wavelength λ=6.328e-4mm, named the plano-concave OTM thick lens. Any geometrical approximation is not included in deducing, which ensures that the full geometrical aberrations are included. The intensity distribution, in its focal region, can be calculated by Huygens-Fresnel integral, using the phase and intensity distributions on the reference plane. The on-axis intensity distribution in the focal region of the plano-convex optically denser medium(ODM) thick lens is given correctly. The intensity distribution in the focal region of the plano-concave OTM thick lens is plotted in two dimensions, no symmetry about the geometrical focal plane. The plano-concave OTM thick lens has smaller focal depth than the plano-convex ODM thick lens has, when they have the same aperture radius, equal curvature radius (not including the sign), and equal medium index difference quantity (not including the sign also) from the environmental medium air. The half width at the full maximum(HWFM) of the radial intensity distribution, on the near end peak plane in the focal region of the planoconcave OTM thick lens with its total spherical aberration, is smaller than that of the Airy disk and breaks down the traditional diffraction limit. Therefore the plano-concave OTM thick lens will exhibit its focusing ability breaking down the traditional diffraction limit, if the energy outside the near end peak can be moved into it.
机译:本文根据光学较薄的介质(OTM)来调查单个镜头的聚焦性质。镜头型号是凹陷形状,由具有折射率0.5的OTM以波长λ= 6.328e-4mm制成,命名为Plano-凹面的OTM厚透镜。在推导中不包括任何几何近似,这确保了包括完整的几何像差。在其焦点区域中,强度分布可以通过惠更斯 - 菲涅耳积分,使用参考平面上的相位和强度分布来计算。正确地给出了Plano-Convex光学更厚透镜的焦点区域的轴轴强度分布。平面凹面厚透镜的焦点区域中的强度分布在两个尺寸中绘制,几何焦平面无对称性。当它们具有相同的光圈半径时,平面凹面OTM厚透镜具有比Plano-Convex ODM厚透镜更小的焦点深度,相同的曲率半径(不包括标志)和等于中等指数差分(不包括标志)另外)来自环境媒体。在径向强度分布的全部最大值(HWFM)的半宽度,在PlanoConcave OTM厚透镜的圆形峰值平面上,其总球面像差小于通风盘的近端峰值,并且断开了传统的衍射极限。因此,如果近端峰值外部的能量移动到其中,则平面凹面OTM厚透镜将表现出其对传统衍射极限的聚焦能力。

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