• Journal of Semiconductors
  • Vol. 42, Issue 12, 122803 (2021)
Ting Zhi1、2, Tao Tao3、4, Xiaoyan Liu1、2, Junjun Xue1、2, Jin Wang1、2, Zhikuo Tao1、2, Yi Li5、6, Zili Xie3、4, and Bin Liu3、4
Author Affiliations
  • 1College of Electronic and Optical Engineering, Nanjing University of Posts and Telecommunications, Nanjing 210023, China
  • 2College of Microelectronics, Nanjing University of Posts and Telecommunications, Nanjing 210023, China
  • 3Jiangsu Provincial Key Laboratory of Advanced Photonic and Electronic Materials, School of Electronic Science and Engineering, Nanjing University, Nanjing 210093, China
  • 4Nanjing National Laboratory of Microstructures, Nanjing University, Nanjing 210093, China
  • 5School of Information Science and Technology, Nantong University, Nantong 226019, China
  • 6Tongke School of Microelectronics, Nantong University, Nantong 226019, China
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    DOI: 10.1088/1674-4926/42/12/122803 Cite this Article
    Ting Zhi, Tao Tao, Xiaoyan Liu, Junjun Xue, Jin Wang, Zhikuo Tao, Yi Li, Zili Xie, Bin Liu. Low-threshold lasing in a plasmonic laser using nanoplate InGaN/GaN[J]. Journal of Semiconductors, 2021, 42(12): 122803 Copy Citation Text show less
    (Color online) (a) Schematic of the nano-plate based SPASER sample, where a thin nano-plate atop silver layer separated by a 10 nm SiO2 gap. (b) SEM image of nano-plate arrays. (c) SEM image of SPASER with single nano-plate (200 nm in width, 1 μm in length, 3μm in height).
    Fig. 1. (Color online) (a) Schematic of the nano-plate based SPASER sample, where a thin nano-plate atop silver layer separated by a 10 nm SiO2 gap. (b) SEM image of nano-plate arrays. (c) SEM image of SPASER with single nano-plate (200 nm in width, 1 μm in length, 3μm in height).
    (Color online) (a) The PL spectra of nano-plate without Ag film under different optical pumping power density. (b) Corresponding L–L curve of the PL peak intensity and the FWHM in the log–log scale as a function of optical pumping power density. (c) PL emission of SPASER with increasing the same optical pumping power density. (d) Corresponding L–L curve and FWHM of the dominant lasing peak at 502 nm as a function of the excited power density.
    Fig. 2. (Color online) (a) The PL spectra of nano-plate without Ag film under different optical pumping power density. (b) Corresponding L–L curve of the PL peak intensity and the FWHM in the log–log scale as a function of optical pumping power density. (c) PL emission of SPASER with increasing the same optical pumping power density. (d) Corresponding L–L curve and FWHM of the dominant lasing peak at 502 nm as a function of the excited power density.
    (Color online) (a) Simulated electric field distribution of plasmonic laser at 502 nm. (b) Simulated electric field distribution of the Nano-plate gain material without Ag film at 520 nm.
    Fig. 3. (Color online) (a) Simulated electric field distribution of plasmonic laser at 502 nm. (b) Simulated electric field distribution of the Nano-plate gain material without Ag film at 520 nm.
    (Color online) TRPL spectra of SPASER at the peak of 502 nm (red line) and InGaN/GaN nano-plate at the peak of 520 nm (black line).
    Fig. 4. (Color online) TRPL spectra of SPASER at the peak of 502 nm (red line) and InGaN/GaN nano-plate at the peak of 520 nm (black line).
    Ting Zhi, Tao Tao, Xiaoyan Liu, Junjun Xue, Jin Wang, Zhikuo Tao, Yi Li, Zili Xie, Bin Liu. Low-threshold lasing in a plasmonic laser using nanoplate InGaN/GaN[J]. Journal of Semiconductors, 2021, 42(12): 122803
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