• Photonics Research
  • Vol. 12, Issue 2, 235 (2024)
Jingxuan Zhang1, Chenni Xu1、2, Patrick Sebbah2, and Li-Gang Wang1、*
Author Affiliations
  • 1School of Physics, Zhejiang University, Hangzhou 310058, China
  • 2Department of Physics, The Jack and Pearl Resnick Institute for Advanced Technology, Bar-Ilan University, Ramat-Gan 5290002, Israel
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    DOI: 10.1364/PRJ.503223 Cite this Article Set citation alerts
    Jingxuan Zhang, Chenni Xu, Patrick Sebbah, Li-Gang Wang. Diffraction limit of light in curved space[J]. Photonics Research, 2024, 12(2): 235 Copy Citation Text show less

    Abstract

    Overcoming the diffraction limit is crucial for obtaining high-resolution images and observing fine microstructures. With this conventional difficulty still puzzling us and the prosperous development of wave dynamics of light interacting with gravitational fields in recent years, how spatial curvature affects the diffraction limit is an attractive and important question. Here we investigate the issue of the diffraction limit and optical resolution on two-dimensional curved space—surfaces of revolution (SORs) with constant or variable spatial curvature. We show that the diffraction limit decreases and the resolution is improved on SORs with positive Gaussian curvature, opening a new avenue to super-resolution. The diffraction limit is also influenced by the propagation direction, as well as the propagation distance in curved space with variable spatial curvature. These results provide a possible method to control the optical resolution in curved space or equivalent waveguides with varying refractive index distribution and may allow one to detect the presence of the nonuniform strong gravitational effect by probing locally the optical resolution.
    ds2=dz2+r02cosq2(z/R)dφ2,

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    ΔgU+(k2+H2K)U=0,

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    2Uz2qtanq(z/R)RUz+[r0cosq(z/R)]22Uφ2+k2U=0.

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    hq(φ,θ,z)=1iλRsinq(z/R)exp[ikz+i2k0zVeff,q(z)dz]×exp[ikr02(φθ)22Rtanq(z/R)],

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    Iqs(θ,z)=|ar0ar0U(z=0)hq(φ,θ,z)r0dφ|2=1Rsinq(z/R)sinc2[kar0θRtanq(z/R)].

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    Iqd(θ,z)=1Rsinq(z/R)sinc2[kar0θRtanq(z/R)]×cos2[kr0θ(a+d/2)Rtanq(z/R)].

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    d2xσds2+Γμνσdxμdsdxνds=0,

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    dφ=±κqr0cosq(z/R)r02cosq2(z/R)κq2dz,

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    x(z)=Rarcsin[r0sin(z/R)r02κ12]Rarcsin[r0sin(z0/R)r02κ12],

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    x(z)=ln|sinh(z/R)+sinh2(z/R)+1κ12/r02sinh(z0/R)+sinh2(z0/R)+1κ12/r02|.

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    ±(φφ0)=Rr0arcsin[κ1tan(z/R)r02κ12]Rr0arcsin[κ1tan(z0/R)r02κ12],

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    ±(φφ0)=Rr0ln[tanh(z/R)+tanh2(z/R)+r02/κ121tanh(z0/R)+tanh2(z0/R)+r02/κ121].

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    Uoutput(P)=1iλlUinput(P0)eikL(P0,P)L(P0,P)A(P0,P)dl,

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    ds2=(1rsr)c2dt2+(1rsr)1dr2+r2sin2Ψdφ2+r2dΨ2,

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    ds2=(1rsr)1dr2+r2dφ2,

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    ds2=(1rsrΛr23)1dr2+r2dφ2,

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    ds2=dz2+[αBcos(zβ+ε)]2dφ2,

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    Jingxuan Zhang, Chenni Xu, Patrick Sebbah, Li-Gang Wang. Diffraction limit of light in curved space[J]. Photonics Research, 2024, 12(2): 235
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