• Photonics Research
  • Vol. 9, Issue 9, 1699 (2021)
Zhe Zhang1, Leona Nest1、2, Suo Wang1, Si-Yi Wang1, and Ren-Min Ma1、3、4、*
Author Affiliations
  • 1State Key Laboratory for Mesoscopic Physics, School of Physics, Peking University, Beijing 100871, China
  • 2Department of Physics, Free University Berlin, Berlin 14195, Germany
  • 3Frontiers Science Center for Nano-optoelectronics & Collaborative Innovation Center of Quantum Matter, Beijing 100871, China
  • 4Yangtze Delta Institute of Optoelectronics, Peking University, Nantong 226010, China
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    DOI: 10.1364/PRJ.431612 Cite this Article Set citation alerts
    Zhe Zhang, Leona Nest, Suo Wang, Si-Yi Wang, Ren-Min Ma. Lasing-enhanced surface plasmon resonance spectroscopy and sensing[J]. Photonics Research, 2021, 9(9): 1699 Copy Citation Text show less

    Abstract

    Surface plasmon resonance (SPR) sensors are a prominent means to detect biological and chemical analytes and to investigate biomolecular interactions in various fields. However, the performance of SPR sensors is ultimately limited by ohmic loss, which substantially weakens the resonance signal and broadens the response linewidth. Recent studies have shown that ohmic loss can be fully compensated in plasmonic nanolasers, which leads to a novel class of lasing-enhanced surface plasmon resonance (LESPR) sensors with improved sensing performance. In this paper, we detail the underlying physical mechanisms of LESPR sensors and present their implementation in various sensing devices. We review recent progress on their applications, particularly for refractive index sensing, gas detection and biological imaging, labeling, tracking, and diagnosis. We then summarize the review and highlight remaining challenges of LESPR sensing technology.
    Ej(x,y)=(Ejx,0,Ejz)eiβxekj|z|,

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    Hj(x,y)=(0,Hjy,0)eiβxekj|z|,

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    β=ωcε1ε2ε1+ε2,

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    β=kx(θ0)=ωcnprsinθ0

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    R(θ)=|r01+r12exp(2ik1d1)1+r01r12exp(2ik1d1)|2.

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    kj=εj(ωc)2kx(θ)2

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    R(θ)R0[14γiγr+δ(θ)(kxβΔβ)2+(γi+γr)2],

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    δ(θ)=4(kxβΔβ)Im(r01)Im(e2ikz0d1)/ξ,

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    ξ=c(ε2ε1)2ω(ε2+ε1ε2ε1)32.

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    γi=Im(β)=k02(ε1ε12+ε2ε22)(ε1ε2ε1+ε2)32,

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    γr=Im(r01e2ikz0d1)ξ.

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    Δβ=Re(r01e2ikz0d1)ξ.

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    L1=2(γi+γr),

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    ××E+ω2c2[ε(r,ω)+εg(r,ω)]E=0,

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    Zhe Zhang, Leona Nest, Suo Wang, Si-Yi Wang, Ren-Min Ma. Lasing-enhanced surface plasmon resonance spectroscopy and sensing[J]. Photonics Research, 2021, 9(9): 1699
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