大数值孔径径向偏振光的焦斑偏振

Yun Xiao, Yunhai Zhang, Jian Chang, Tongda Wei
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引用次数: 0

摘要

根据Wolf和Richards矢量衍射理论,建立了大数值孔径径向偏振光的焦斑电场强度模型,分别分析了焦斑强度和电场偏振分量沿x、y、z轴的分布。在成像系统的反射模式共聚焦中,利用金纳米棒获得了焦点光斑的强度分布,利用金纳米棒获得了电场偏振分量沿x、y和z轴的强度分布。在入射光中,物镜前不存在沿z轴方向的偏振分量。但在物镜后面的焦斑中,存在相对于数值孔径的z轴偏振分量。当数值孔径从0.8增加到1.4时,沿z轴偏振分量最大值与沿x轴或y轴偏振分量最大值之比从0.57增加到3.16。结果表明:通过大数值孔径物镜的径向偏振光束的焦斑分别具有沿x、y和z轴的偏振分量,且沿z轴的偏振分量远大于其他方向。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Polarization of focal spot for high numerical aperture radially polarized beam
According to Wolf and Richards vectorial diffraction theory, an electric field intensity model of focal spot for high numerical aperture radially polarized beam is established to analyze the intensity distributions of the focal spot and the polarization components of the electric field along the x, y and z axis, separately. In the reflection-mode confocal of imaging system, the intensity distributions of focal spot is obtained utilizing the gold nanoparticles, and the intensity distributions of the polarization components of the electric field along the x, y and z axis are obtained utilizing the gold nanorods. In the incident light, the polarization component along the z axis is nonexistent in front of the objective. But there is the polarization component along the z axis, which is relative to the numerical aperture, in the focal spot behind the objective. When the numerical aperture increases from 0.8 to 1.4, the ratio of the polarization component maximum along the z axis to that along the x axis or y axis increases from 0.57 to 3.16. The results show that the focal spot of radially polarized beam through high numerical aperture objective have the polarization component along the x, y and z axis, separately, and polarization component along z axis is much more than the other.
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