• Photonics Insights
  • Vol. 2, Issue 1, R01 (2023)
Tao Li1、*, Chen Chen1、*, Xingjian Xiao1, Ji Chen2, Shanshan Hu1, and Shining Zhu1、*
Author Affiliations
  • 1National Laboratory of Solid State Microstructures, Key Laboratory of Intelligent Optical Sensing and Manipulation, Jiangsu Key Laboratory of Artificial Functional Materials, College of Engineering and Applied Sciences, School of Physics, Nanjing University, Nanjing, China
  • 2National Mobile Communications Research Laboratory, School of Information Science and Engineering, Frontiers Science Center for Mobile Information Communication and Security, Southeast University, Nanjing, China
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    DOI: 10.3788/PI.2023.R01 Cite this Article Set citation alerts
    Tao Li, Chen Chen, Xingjian Xiao, Ji Chen, Shanshan Hu, Shining Zhu. Revolutionary meta-imaging: from superlens to metalens[J]. Photonics Insights, 2023, 2(1): R01 Copy Citation Text show less

    Abstract

    The refractive-lens technique has been well developed over a long period of evolution, offering powerful imaging functionalities, such as microscopes, telescopes, and spectroscopes. Nevertheless, the ever-growing requirements continue to urge further enhanced imaging capabilities and upgraded devices that are more compact for convenience. Metamaterial as a fascinating concept has inspired unprecedented new explorations in physics, material science, and optics, not only in fundamental researches but also novel applications. Along with the imaging topic, this paper reviews the progress of the flat lens as an important branch of metamaterials, covering the early superlens with super-diffraction capability and current hot topics of metalenses including a paralleled strategy of multilevel diffractive lenses. Numerous efforts and approaches have been dedicated to areas ranging from the new fascinating physics to feasible applications. This review provides a clear picture of the flat-lens evolution from the perspective of metamaterial design, elucidating the relation and comparison between a superlens and metalens, and addressing derivative designs. Finally, application scenarios that favor the ultrathin lens technique are emphasized with respect to possible revolutionary imaging devices, followed by conclusive remarks and prospects.

    Story Video to the Review Article

    E=E0(x,y)exp(ikzziωt),

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    limμ1ɛ1TP=limμ1ɛ12ɛkzɛkz+kz2kzkz+ɛkz×exp(ikzd)1(kzɛkzkz+ɛkz)2exp(2ikzd)=exp(ikzd),

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    ɛ=(ɛx000ɛy000ɛz).

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    (ω2c2ɛk2)[ω4c4ɛɛω2c2ɛ(kx2+ky2)ω2c2ɛkz2]=0,

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    ω2c2ɛk2=0,(5a)

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    ω4c4ɛɛω2c2ɛ(kx2+ky2)ω2c2ɛkz2=0.(5b)

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    ω2c2=kx2ɛ+kz2ɛ,

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    ceff=cjJ0[A4π2n0Pλ(xjxj1)],

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    {sinθrsinθi=λ02πnidφdx,ntsinθtnisinθi=λ02πdφdx,,

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    Et=t^(ϕ)|σ=to+te2|σ+tote2ei2σθ|σ,

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    ϕ(R)=2πλ(fR2+f2),

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    ϕ(R,ω)=ϕ(R,ωd)+ϕ(R,ω)ω|ω=ωd(ωωd)+2ϕ(R,ω)2ω2|ω=ωd(ωωd)2+.

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    ΔωΔωmax=κc(f2+R2f)=κc1(NA/nb)2f[11(NA/nb)2],

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    κ=ωdhc(nmaxnmin),

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    κ=ωdh23c|(nmax2nb2)/nb2|,

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    ϕ(r,λ,θ)=2πλ[rsinθ+(rftanθ)2+f2fcosθ].

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    ϕ(r,θ)=k02fr2k0xsinθ=k02f[(x+fsinθ)2+y2]+k0fsin2θ2,

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    ηm=[sin(mπ/2)mπ]2.

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    ϕ(r,λ)=2πλ[n(λ)1]h(r),

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    h(r)=λ02π[n(λ0)1](ϕ0mod2π),

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    ηm={sin[π(m1)]π(m1)}2.

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    ηmN={sin[π(1m)]π(1m)}2[sin(π/N)π/N]2,

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    ηmN={sin{π[α(λ)m]}π(α(λ)m)}2[sin(π/N)π/N]2,

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    ηm={sin{π[Mα(λ)m]}π[Mα(λ)m]}2.

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    maxF(H)s.t.0h(r)H0rR,

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    F=1NλλI0(λ),

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    F=1NλNλ01.5wI(r,λ)rdr0RI(r,λ)rdr,

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    ϕ(ρ,ω)=ωc(ρ2+F2F)+Δϕ(ρ,ω).

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    Jω(ρ1,ρ2)=eiΔϕ(ρ1,ω)eiΔϕ(ρ2,ω)ω,

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    Dmax4(nmax1)H[11maxJω(F)]NA,

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    ϕSP(kx,ky,deff)=deff(|k|2kx2ky2)1/2.

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    Tao Li, Chen Chen, Xingjian Xiao, Ji Chen, Shanshan Hu, Shining Zhu. Revolutionary meta-imaging: from superlens to metalens[J]. Photonics Insights, 2023, 2(1): R01
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