• Chinese Optics Letters
  • Vol. 21, Issue 4, 041406 (2023)
Jian Fan1、2, Xuyan Zhou1、3、4、**, Weiqiao Zhang1、2, Yufei Wang1、2、5, Hongwei Qu1、3, Aiyi Qi1、3, and Wanhua Zheng1、2、3、5、*
Author Affiliations
  • 1Laboratory of Solid-State Optoelectronics Information Technology, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3State Key Laboratory on Integrated Optoelectronics, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
  • 4Weifang Academy of Advanced Opto-Electronic Circuits, Weifang 261071, China
  • 5College of Future Technology, University of Chinese Academy of Sciences, Beijing 101408, China
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    DOI: 10.3788/COL202321.041406 Cite this Article Set citation alerts
    Jian Fan, Xuyan Zhou, Weiqiao Zhang, Yufei Wang, Hongwei Qu, Aiyi Qi, Wanhua Zheng. Improving the performance of high-power broad-area lasers by suppressing cavity modes propagating in the lateral dimension[J]. Chinese Optics Letters, 2023, 21(4): 041406 Copy Citation Text show less
    (a) Schematic diagram of SSC laser. The inset is the scanning electron microscope (SEM) image of the fabricated SSC structure. (b) Sketch of a rectangular F–P cavity of length L and width W. The wave vector can be separated into longitudinal and lateral components klo and kla, respectively.
    Fig. 1. (a) Schematic diagram of SSC laser. The inset is the scanning electron microscope (SEM) image of the fabricated SSC structure. (b) Sketch of a rectangular F–P cavity of length L and width W. The wave vector can be separated into longitudinal and lateral components klo and kla, respectively.
    The typical lateral oscillation mode distribution in the F–P cavity and the SSC cavity. The width is 40 µm, and the length is 50 µm; both the width and length of the triangle are 2 µm.
    Fig. 2. The typical lateral oscillation mode distribution in the F–P cavity and the SSC cavity. The width is 40 µm, and the length is 50 µm; both the width and length of the triangle are 2 µm.
    Calculated Q-factors of the lateral propagating modes in the SSC cavity (black dots) and the F–P cavity (red dots).
    Fig. 3. Calculated Q-factors of the lateral propagating modes in the SSC cavity (black dots) and the F–P cavity (red dots).
    (a) L-I-V characteristic curves of the four types of lasers measured at room temperature under the CW operation; (b) three microstructures with different sizes.
    Fig. 4. (a) L-I-V characteristic curves of the four types of lasers measured at room temperature under the CW operation; (b) three microstructures with different sizes.
    The ASE spectrum of the SSC lasers and the standard BA lasers at (a) 1.5 A and (b) 2.3 A, respectively.
    Fig. 5. The ASE spectrum of the SSC lasers and the standard BA lasers at (a) 1.5 A and (b) 2.3 A, respectively.
    Measured L-I-V curves and WPE as functions of the operating current of SSC lasers (solid line) and standard BA lasers (dotted Line) in CW mode at 0°C.
    Fig. 6. Measured L-I-V curves and WPE as functions of the operating current of SSC lasers (solid line) and standard BA lasers (dotted Line) in CW mode at 0°C.
    Jian Fan, Xuyan Zhou, Weiqiao Zhang, Yufei Wang, Hongwei Qu, Aiyi Qi, Wanhua Zheng. Improving the performance of high-power broad-area lasers by suppressing cavity modes propagating in the lateral dimension[J]. Chinese Optics Letters, 2023, 21(4): 041406
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