• Journal of Semiconductors
  • Vol. 42, Issue 11, 112301 (2021)
Teng Fei1、2、3, Shenqiang Zhai1、2, Jinchuan Zhang1、2, Ning Zhuo1、2, Junqi Liu1、2、3, Lijun Wang1、2、3, Shuman Liu1、2, Zhiwei Jia1、2, Kun Li1、2、3, Yongqiang Sun1、2、3, Kai Guo1、2, Fengqi Liu1、2、3, and Zhanguo Wang1、2、3
Author Affiliations
  • 1Key Laboratory of Semiconductor Materials Science, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
  • 2Beijing Key Laboratory of Low Dimensional Semiconductor Materials and Devices, Beijing 100083, China
  • 3Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
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    DOI: 10.1088/1674-4926/42/11/112301 Cite this Article
    Teng Fei, Shenqiang Zhai, Jinchuan Zhang, Ning Zhuo, Junqi Liu, Lijun Wang, Shuman Liu, Zhiwei Jia, Kun Li, Yongqiang Sun, Kai Guo, Fengqi Liu, Zhanguo Wang. High power λ ~ 8.5 μm quantum cascade laser grown by MOCVD operating continuous-wave up to 408 K[J]. Journal of Semiconductors, 2021, 42(11): 112301 Copy Citation Text show less

    Abstract

    Robust quantum cascade laser (QCL) enduring high temperature continuous-wave (CW) operation is of critical importance for some applications. We report on the realization of lattice-matched InGaAs/InAlAs/InP QCL materials grown by metal-organic chemical vapor deposition (MOCVD). High interface quality structures designed for light emission at 8.5 μm are achieved by optimizing and precise controlling of growth conditions. A CW output power of 1.04 W at 288 K was obtained from a 4 mm-long and 10 μm-wide coated laser. Corresponding maximum wall-plug efficiency and threshold current density were 7.1% and 1.18 kA/cm2, respectively. The device can operate in CW mode up to 408 K with an output power of 160 mW.
    $ {J}_{\mathrm{t}\mathrm{h}}={J}_{0}\mathrm{e}\mathrm{x}\mathrm{p}\left(T/{T}_{0}\right) , $ ()

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    $ {\eta }_{\mathrm{s}\mathrm{l}\mathrm{o}\mathrm{p}\mathrm{e}}={\eta }_{0}\mathrm{e}\mathrm{x}\mathrm{p}\left(-T/{T}_{1}\right) , $ ()

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    $ \hslash {\tau }_{\rm{IFR}}^{-1}=\frac{\pi {m}^{*}}{{{\hslash }}^{2}}{{\varDelta }}^{2}{{\Lambda }}^{2}\delta {U}^{2}{\sum }_{i}\left[{\phi }_{2}\left({z}_{i}\right){\phi }_{1}{\left({z}_{i}\right)}\right]^{2}{\rm e}^{\frac{-{{\Lambda }}^{2}{q}_{21}^{2}}{4}} , $ ()

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    Teng Fei, Shenqiang Zhai, Jinchuan Zhang, Ning Zhuo, Junqi Liu, Lijun Wang, Shuman Liu, Zhiwei Jia, Kun Li, Yongqiang Sun, Kai Guo, Fengqi Liu, Zhanguo Wang. High power λ ~ 8.5 μm quantum cascade laser grown by MOCVD operating continuous-wave up to 408 K[J]. Journal of Semiconductors, 2021, 42(11): 112301
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