• Photonics Insights
  • Vol. 1, Issue 1, R04 (2022)
Sanjib Ghosh1, Rui Su2、*, Jiaxin Zhao2, Antonio Fieramosca2, Jinqi Wu2, Tengfei Li1, Qing Zhang3、4, Feng Li5, Zhanghai Chen6, Timothy Liew2, Daniele Sanvitto7, and Qihua Xiong1、8、9、10、*
Author Affiliations
  • 1Beijing Academy of Quantum Information Sciences, Beijing, China
  • 2Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore, Singapore
  • 3School of Materials Science and Engineering, Peking University, Beijing, China
  • 4Research Center for Wide Gap Semiconductor, Peking University, Beijing, China
  • 5Key Laboratory for Physical Electronics and Devices of the Ministry of Education & Shaanxi Key Laboratory of Information Photonic Technique, School of Electronic Science and Engineering, Faculty of Electronic and Information Engineering, Xi’an Jiaotong University, Xi’an, China
  • 6Department of Physics, College of Physical Science and Technology, Xiamen University, Xiamen, China
  • 7CNR NANOTEC, Campus Ecotekne, Lecce, Italy
  • 8State Key Laboratory of Low-Dimensional Quantum Physics and Department of Physics, Tsinghua University, Beijing, China
  • 9Frontier Science Center for Quantum Information, Beijing, China
  • 10Beijing Innovation Center for Future Chips, Tsinghua University, Beijing, China
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    DOI: 10.3788/PI.2022.R04 Cite this Article Set citation alerts
    Sanjib Ghosh, Rui Su, Jiaxin Zhao, Antonio Fieramosca, Jinqi Wu, Tengfei Li, Qing Zhang, Feng Li, Zhanghai Chen, Timothy Liew, Daniele Sanvitto, Qihua Xiong. Microcavity exciton polaritons at room temperature[J]. Photonics Insights, 2022, 1(1): R04 Copy Citation Text show less

    Abstract

    The quest for realizing novel fundamental physical effects and practical applications in ambient conditions has led to tremendous interest in microcavity exciton polaritons working in the strong coupling regime at room temperature. In the past few decades, a wide range of novel semiconductor systems supporting robust exciton polaritons have emerged, which has led to the realization of various fascinating phenomena and practical applications. This paper aims to review recent theoretical and experimental developments of exciton polaritons operating at room temperature, and includes a comprehensive theoretical background, descriptions of intriguing phenomena observed in various physical systems, as well as accounts of optoelectronic applications. Specifically, an in-depth review of physical systems achieving room temperature exciton polaritons will be presented, including the early development of ZnO and GaN microcavities and other emerging systems such as organics, halide perovskite semiconductors, carbon nanotubes, and transition metal dichalcogenides. Finally, a perspective of outlooking future developments will be elaborated.

    Story Video to the Review Article

    [Ψσ(r),Ψσ(r)]=δ(rr)δσσ,[Ψσ(r),Ψσ(r)]=0,[Ψσ(r),Ψσ(r)]=0,

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    Ψσ(r)=1(2π)2dkbσ(k)eikr,Ψσ(r)=1(2π)2dkbσ(k)eikr.

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    [bσ(k),bσ(k)]=(2π)2δ(kk)δσσ,[bσ(k),bσ(k)]=0,[bσ(k),bσ(k)]=0.

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    ɛ(k)ɛ(0)+(ℏ︀k)22m,

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    Hph=σdrΨCσ(r)[ɛσ(0)ℏ︀222mσ]ΨCσ(r).

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    Hph=σdkɛσ(k)bCσ(k)bCσ(k),

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    E(r,z)=1(2π)2σeσdkuσk(z)bCσ(k)eikr+h.c.,

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    Hphg=σσdkɛσσ(k)bCσ(k)bCσ(k).

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    ɛS(k)ɛS(0)+ℏ︀2kx22mxS+ℏ︀2ky22myS,

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    Hex=σdkɛX(k)bXσ(k)bXσ(k),

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    Hint=ℏ︀ΩRσ,sdk[bCσ(k)bXσ(k)+bXσ(k)bCσ(k)],

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    aLPσ(k)=ηXσ(k)bXσ(k)+ηCσ(k)bCσ(k),aUPσ(k)=ηCσ(k)bXσ(k)ηXσ(k)bCσ(k).

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    ELPσ/UPσ(k)=ɛex(k)+ɛσ(k)2(ℏ︀ΩR)2+[ɛex(k)ɛσ(k)]24.

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    Hep=dkσELPσ(k)aLPσ(k)aLPσ(k).

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    HPP=12σσασσLPdrΨLPσ(r)ΨLPσ(r)ΨLPσ(r)ΨLPσ(r),

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    ΨLPσ(r)=1(2π)2dkaLPσ(k)eikr.

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    VLP(r)=|ηCσ|2Vph(r),

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    iℏ︀ψ˙LP(r,t)=[ℏ︀22mLP2+VLP(r)]ψLP(r,t)+αLP|ψLP(r,t)|2ψLP(r,t),

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    iℏ︀ψ˙LP(r,t)=[ℏ︀22mLP2+VLP(r)iγLP2]ψLP(r,t)+αLP|ψLP(r,t)|2ψLP(r,t),

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    iℏ︀ψ˙LP(r,t)=[ℏ︀222mLP+VLP(r)iγLP2+αLP|ψLP(r,t)|2]×ψLP(r,t)+iηLP(r)F(r,t),

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    iℏ︀ψ˙LP(r,t)=[ℏ︀22mLP2+VLP(r)iγLP2+i2Pin(r)]×ψLP(r,t)+α˜LP|ψLP(r,t)|2ψLP(r,t).

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    iℏ︀ψ˙LP(r,t)=[ℏ︀222mLP+VLP(r)+iRRnR(r,t)iγLP2]××ψLP(r,t)+αLP|ψLP(r,t)|2ψLP(r,t),

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    n˙R(r,t)=PR(r)RRnR(r,t)|ψLP(r,t)|2γRnR(r,t),

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    nB(ɛ)=1exp(ɛμkBT)1,

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    [ℏ︀22mLP2iγLP2+i2Pin(r)]ψLP(r,t)+α˜LP|ψLP(r,t)|2ψLP(r,t)=0.

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    [ɛLP(kp)ℏ︀ωpiγLP2]ϕLP+αLP|ϕLP|2ϕLP+Pco=0,

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    NLP=2[ℏ︀ωpɛLP(kp)]±[ℏ︀ωpɛLP(kp)]23γLP243αLP.

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    ɛBOG(k)=ɛ(k)[ɛ(k)+2Ncαk],

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    ψLP(r)=NLP(r)eiθ(r),

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    Cθ(r).dl=2πQv,

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    v(r)=ℏ︀QvrmLPeφ,

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    HQC=ɛQCjajaj+JQCjk(ajak+akaj)+αQCjajajajaj+j[ajFQC(t)+FQC(t)*aj],

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    iℏ︀ρ˙=[HQC,ρ]+iℏ︀γQC2j(2ajρajajajρρajaj),

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    Hiso=ɛaa+αaaaa+F*a+aF,

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    g2(t,τ)=a(t)a(t+τ)a(t+τ)a(t)a(t+τ)a(t+τ)a(t)a(t).

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    Hf=Ωfn^+αn^2+2PNccos(ϕθ^),

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    HLattice=jE0j|φ0jφ0j|+jk(Jjk|φ0jφ0k|+Jjk*|φ0kφ0j|),

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    Jjkℏ︀22mLP,xSdr[φ0j(r)*2x2φ0k(r)],

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    HBH=Jij(aiaj+ajai)+Uiaiaiaiai.

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    HQ=ε·σ,

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    Sanjib Ghosh, Rui Su, Jiaxin Zhao, Antonio Fieramosca, Jinqi Wu, Tengfei Li, Qing Zhang, Feng Li, Zhanghai Chen, Timothy Liew, Daniele Sanvitto, Qihua Xiong. Microcavity exciton polaritons at room temperature[J]. Photonics Insights, 2022, 1(1): R04
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