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双针孔产生的相干涡旋。

Coherence vortices by binary pinholes.

作者信息

Gautam Akanksha, Agarwal Amit K, Singh Rakesh Kumar

机构信息

Laboratory of Information Photonics and Optical Metrology, Department of Physics, Indian Institute of Technology (Banaras Hindu University), Varanasi 221005, India.

Photonics Division, Instruments R&D Establishment, Dehradun 248001, India.

出版信息

Nanophotonics. 2024 Oct 17;13(24):4397-4407. doi: 10.1515/nanoph-2024-0380. eCollection 2024 Nov.

DOI:10.1515/nanoph-2024-0380
PMID:39679184
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11636419/
Abstract

Singularity in a two-point complex coherence function, known as coherence vortices, represents zero visibility with a helical phase structure. In this paper, we introduce a novel technique to generate the coherence vortices of different topological charges by incoherent source transmittance with exotic structured binary pinholes. The binary pinhole structures have been realized by lithography, followed by wet etching methods. We control the transmittance from the incoherent source plane using these exotic apertures, which finally results in a coherence vortex spectrum that features multiple and pure orbital angular momentum modes. The generation of the coherence vortices is achieved within the two-point complex spatial coherence function. The spatial coherence function exhibits the helical phase profile in its phase part, and its absolute part shows a doughnut-shaped structure. A theoretical basis is developed and validated with simulation, and experimental results. The coherence vortex spectra with OAM modes superposed with opposite topological charges, known as photonic gears, are also generated with the proposed theory.

摘要

两点复相干函数中的奇点,即相干涡旋,代表具有螺旋相位结构的零可见度。在本文中,我们介绍了一种新技术,通过具有奇异结构的二元针孔的非相干源透过率来生成不同拓扑电荷的相干涡旋。二元针孔结构已通过光刻技术实现,随后采用湿法蚀刻方法。我们使用这些奇异孔径来控制来自非相干源平面的透过率,最终得到具有多个纯轨道角动量模式的相干涡旋光谱。相干涡旋的生成是在两点复空间相干函数内实现的。空间相干函数在其相位部分呈现螺旋相位分布,其绝对值部分呈现环形结构。我们建立了理论基础,并通过模拟和实验结果进行了验证。利用所提出的理论还生成了叠加有相反拓扑电荷的轨道角动量模式的相干涡旋光谱,即所谓的光子齿轮。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e4c/11636419/eadcdf79528f/j_nanoph-2024-0380_fig_007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e4c/11636419/63791227b644/j_nanoph-2024-0380_fig_001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e4c/11636419/fcb4b6005d29/j_nanoph-2024-0380_fig_002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e4c/11636419/db4d2ebba909/j_nanoph-2024-0380_fig_003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e4c/11636419/b1f157f97629/j_nanoph-2024-0380_fig_004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e4c/11636419/4b654b6d5776/j_nanoph-2024-0380_fig_005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e4c/11636419/d10a18084204/j_nanoph-2024-0380_fig_006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e4c/11636419/eadcdf79528f/j_nanoph-2024-0380_fig_007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e4c/11636419/63791227b644/j_nanoph-2024-0380_fig_001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e4c/11636419/fcb4b6005d29/j_nanoph-2024-0380_fig_002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e4c/11636419/db4d2ebba909/j_nanoph-2024-0380_fig_003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e4c/11636419/b1f157f97629/j_nanoph-2024-0380_fig_004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e4c/11636419/4b654b6d5776/j_nanoph-2024-0380_fig_005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e4c/11636419/d10a18084204/j_nanoph-2024-0380_fig_006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e4c/11636419/eadcdf79528f/j_nanoph-2024-0380_fig_007.jpg

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