• Photonics Research
  • Vol. 6, Issue 6, 641 (2018)
Xiaodong Qiu1, Fangshu Li1, Haigang Liu2, Xianfeng Chen2,3,*, and Lixiang Chen1,4,*
Author Affiliations
  • 1Department of Physics, Jiujiang Research Institute and Collaborative Innovation Center for Optoelectronic Semiconductors and Efficient Devices, Xiamen University, Xiamen 361005, China
  • 2State Key Laboratory of Advanced Optical Communication Systems and Networks, School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China
  • 3e-mail: xfchen@sjtu.edu.cn
  • 4e-mail: chenlx@xmu.edu.cn
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    DOI: 10.1364/PRJ.6.000641 Cite this Article Set citation alerts
    Xiaodong Qiu, Fangshu Li, Haigang Liu, Xianfeng Chen, Lixiang Chen, "Optical vortex copier and regenerator in the Fourier domain," Photonics Res. 6, 641 (2018) Copy Citation Text show less

    Abstract

    The generation and manipulation of optical vortices are of fundamental importance in a variety of promising applications. Here, we develop a nonlinear optical paradigm to implement self- and cross-convolution of optical vortex arrays, demonstrating the features of a vortex copier and regenerator. We use a phase-only spatial light modulator to prepare the 1064 nm invisible fundamental light to carry special optical vortex arrays and use a potassium titanyl phosphate crystal to perform type II second-harmonic generation in the Fourier domain to achieve 532 nm visible structured vortices. Based on pure cross-convolution, we succeed in copying arbitrary-order single vortices as well as their superposition states onto a prearranged array of fundamental Gaussian spots. Also, based on the simultaneous effect of self- and cross-convolutions, we can expand the initial vortex lattices to regenerate more vortices carrying various higher topological charges. Our presented method of realizing an optical vortex copier and regenerator could find direct applications in optical manipulation, optical imaging, optical communication, and quantum information processing with structured vortex arrays.
    E1(r,ϕ)=iA1,i(ri)exp(iliϕi),(1)

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    E2(r,ϕ)=jA2,j(rj)exp(iljϕj).(2)

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    dE˜3(ρ,φ)dz=iω32deffk3c2E˜1(ρ,φ)E˜2(ρ,φ),(3)

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    E3(r,ϕ)=αF[E˜1(ρ,ϕ)E˜2(ρ,ϕ)]=αij[A1,i(ri)exp(iliϕi)]*[A2,j(rj)exp(iljϕj)],(4)

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    [A1,i(ri)exp(iliϕi)]*[A2,j(rj)exp(iljϕj)]=F1{F[A1,i(ri)exp(iliϕi)]×F[A2,j(rj)exp(iljϕj)]}=2πw2(|li+lj|)!(2rw)|li+lj|exp(r2w2)exp[i(li+lj)ϕ],(5)

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    E3(r,ϕ)i[A1,i(ri)exp(iliϕi)]*[A1,i(ri)exp(iliϕi)]+ij[A1,i(ri)exp(iliϕi)]*[A1,j(rj)exp(iljϕj)].(6)

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    Xiaodong Qiu, Fangshu Li, Haigang Liu, Xianfeng Chen, Lixiang Chen, "Optical vortex copier and regenerator in the Fourier domain," Photonics Res. 6, 641 (2018)
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