• Journal of Semiconductors
  • Vol. 40, Issue 7, 071905 (2019)
Zhe He1, Jiawei Yang2, Lidan Zhou2, Yan Chen3, Tianming Zhao1, Ying Yu2, and Jin Liu1
Author Affiliations
  • 1State Key Laboratory of Optoelectronic Materials and Technologies, School of Physics, Sun Yat-sen University, Guangzhou 510275, China
  • 2State Key Laboratory of Optoelectronic Materials and Technologies, School of Electronics and Information Technology, Sun Yat-sen University, Guangzhou 510275, China
  • 3Institute for Integrative Nanosciences, Leibniz IFW Dresden, Helmholtzstrasse 20, Dresden 01069, Germany
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    DOI: 10.1088/1674-4926/40/7/071905 Cite this Article
    Zhe He, Jiawei Yang, Lidan Zhou, Yan Chen, Tianming Zhao, Ying Yu, Jin Liu. Broadband photonic structures for quantum light sources[J]. Journal of Semiconductors, 2019, 40(7): 071905 Copy Citation Text show less
    (Color online) (a–b) Scanning electron microscopy (SEM) image (a) of a top–down tapered GaAs nanowire waveguide with an embedded InAs QD, together with the intensity profile for a 2D-cut along the nanowire growth axis by FDTD simulation (b). (c–d) SEM image (c) of a top–down GaAs photonic trumpet with an embedded InAs QD, together with the intensity profile for a 2D-cut along the nanowire growth axis by FDTD simulation (d). (e) SEM image of a bottom–up tapered InP nanowire waveguide containing a single InAsP QD[51], reprinted with permission, Copyright 2012, Springer Nature.
    Fig. 1. (Color online) (a–b) Scanning electron microscopy (SEM) image (a) of a top–down tapered GaAs nanowire waveguide with an embedded InAs QD, together with the intensity profile for a 2D-cut along the nanowire growth axis by FDTD simulation (b). (c–d) SEM image (c) of a top–down GaAs photonic trumpet with an embedded InAs QD, together with the intensity profile for a 2D-cut along the nanowire growth axis by FDTD simulation (d). (e) SEM image of a bottom–up tapered InP nanowire waveguide containing a single InAsP QD[51], reprinted with permission, Copyright 2012, Springer Nature.
    (Color online) (a) Illustration of a finite PCW with a single QD embedded. (b) The band structure and waveguide modes of PCWs. (c) SEM picture of a PCW. (d) Decay dynamics for QDs that couple and uncouple to the PCWs[68], reprinted with permission, Copyright 2014, American Physical Society.
    Fig. 2. (Color online) (a) Illustration of a finite PCW with a single QD embedded. (b) The band structure and waveguide modes of PCWs. (c) SEM picture of a PCW. (d) Decay dynamics for QDs that couple and uncouple to the PCWs[68], reprinted with permission, Copyright 2014, American Physical Society.
    (Color online) (a) The dielectric antenna consists of, from bottom to top, a silver layer, an AlGaAs membrane (with embedded QDs), a low refractive index PMMA spacer and the GaP SIL. Most photon emission is funneled into the GaP SIL[70], reprinted with permission, Copyright 2018, Springer Nature. (b) Comparison of the photon-extraction efficiency for different micro-lens mirror structures. With DBR bottom mirror, the photon extraction efficiency reaches to a plateau value of only around 23%, while with a gold bottom mirror, it is improved to more than 80% for large numerical aperture collection objectives[71], reprinted with permission, Copyright 2015, Springer Nature. (c) Schematic view of the QD micro-lens/micro-objective device. A micro-objective is printed directed on top of a QD micro-lens[73], reprinted with permission, Copyright 2017, American Chemical Society.
    Fig. 3. (Color online) (a) The dielectric antenna consists of, from bottom to top, a silver layer, an AlGaAs membrane (with embedded QDs), a low refractive index PMMA spacer and the GaP SIL. Most photon emission is funneled into the GaP SIL[70], reprinted with permission, Copyright 2018, Springer Nature. (b) Comparison of the photon-extraction efficiency for different micro-lens mirror structures. With DBR bottom mirror, the photon extraction efficiency reaches to a plateau value of only around 23%, while with a gold bottom mirror, it is improved to more than 80% for large numerical aperture collection objectives[71], reprinted with permission, Copyright 2015, Springer Nature. (c) Schematic view of the QD micro-lens/micro-objective device. A micro-objective is printed directed on top of a QD micro-lens[73], reprinted with permission, Copyright 2017, American Chemical Society.
    (Color online) (a–c) SEM images of CBG structure[7], (a–c) are reprinted with permission, Copyright 2011, AIP Publishing. (d) The schematic of the CBR-HBR. (e) Simulated Purcell facor and collection efficiency of the CBR-HBR[3], (d) and (e) are reprinted with permission, Copyright 2019, Nature Springer.
    Fig. 4. (Color online) (a–c) SEM images of CBG structure[7], (a–c) are reprinted with permission, Copyright 2011, AIP Publishing. (d) The schematic of the CBR-HBR. (e) Simulated Purcell facor and collection efficiency of the CBR-HBR[3], (d) and (e) are reprinted with permission, Copyright 2019, Nature Springer.
    Zhe He, Jiawei Yang, Lidan Zhou, Yan Chen, Tianming Zhao, Ying Yu, Jin Liu. Broadband photonic structures for quantum light sources[J]. Journal of Semiconductors, 2019, 40(7): 071905
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