• Photonics Research
  • Vol. 7, Issue 11, 1244 (2019)
Shouzhu Niu1、2, Junqi Liu1、2、3、5、*, Fengmin Cheng1、2、3, Huan Wang1、2、3, Jinchuan Zhang1、2、3, Ning Zhuo1、2、3, Shenqiang Zhai1、2、3, Lijun Wang1、2、3, Shuman Liu1、2、3, Fengqi Liu1、2、3, Zhanguo Wang1、2、3, Xiaohua Wang1、2、4、*, and Zhipeng Wei1、2
Author Affiliations
  • 1State Key Laboratory of High Power Semiconductor Lasers, School of Science, Changchun University of Science and Technology, Changchun 130022, China
  • 2Key Laboratory of Semiconductor Materials Science, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
  • 3Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
  • 4e-mail: biewang2001@126.com
  • 5e-mail: jqliu@semi.ac.cn
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    DOI: 10.1364/PRJ.7.001244 Cite this Article Set citation alerts
    Shouzhu Niu, Junqi Liu, Fengmin Cheng, Huan Wang, Jinchuan Zhang, Ning Zhuo, Shenqiang Zhai, Lijun Wang, Shuman Liu, Fengqi Liu, Zhanguo Wang, Xiaohua Wang, Zhipeng Wei. 14 μm quantum cascade lasers based on diagonal transition and nonresonant extraction[J]. Photonics Research, 2019, 7(11): 1244 Copy Citation Text show less
    Schematic conduction band diagram of a portion of the active layers under an applied electronic field of 28 kV/cm. The moduli squared of the relevant wave functions are shown. The layer sequence of one period of the structure in angstroms starting from the injection barrier (toward the right side) is as follows: 41/31/9/59/7/60/8/56/9/51/15/49/21/48/23/43/29/40/30/38/31/35, where In0.52Al0.48As barrier layers are in bold, In0.53Ga0.47As quantum wells are in roman, and the doped layers (Si, 2.3×1017 cm−3) are underlined. The inset shows a schematic of the diagonal transition and nonresonant extraction scheme.
    Fig. 1. Schematic conduction band diagram of a portion of the active layers under an applied electronic field of 28 kV/cm. The moduli squared of the relevant wave functions are shown. The layer sequence of one period of the structure in angstroms starting from the injection barrier (toward the right side) is as follows: 41/31/9/59/7/60/8/56/9/51/15/49/21/48/23/43/29/40/30/38/31/35, where In0.52Al0.48As barrier layers are in bold, In0.53Ga0.47As quantum wells are in roman, and the doped layers (Si, 2.3×1017  cm3) are underlined. The inset shows a schematic of the diagonal transition and nonresonant extraction scheme.
    Lasing spectra of the QCL at various temperatures. The inset is a lateral far-field radiation pattern at the heat sink temperature of 293 K.
    Fig. 2. Lasing spectra of the QCL at various temperatures. The inset is a lateral far-field radiation pattern at the heat sink temperature of 293 K.
    Pulsed PIV characteristics for an HR-coated 4 mm long and 40 μm wide QCL at various heat sink temperatures. The frequency of driving current is 5 kHz, and the duration is 2 μs.
    Fig. 3. Pulsed PIV characteristics for an HR-coated 4 mm long and 40 μm wide QCL at various heat sink temperatures. The frequency of driving current is 5 kHz, and the duration is 2 μs.
    Threshold current density and slope efficiency at different temperatures, where the dashed curves are theoretical fittings.
    Fig. 4. Threshold current density and slope efficiency at different temperatures, where the dashed curves are theoretical fittings.
    Average output power characteristics of the laser at heat sink temperatures from 293 to 353 K.
    Fig. 5. Average output power characteristics of the laser at heat sink temperatures from 293 to 353 K.
    Shouzhu Niu, Junqi Liu, Fengmin Cheng, Huan Wang, Jinchuan Zhang, Ning Zhuo, Shenqiang Zhai, Lijun Wang, Shuman Liu, Fengqi Liu, Zhanguo Wang, Xiaohua Wang, Zhipeng Wei. 14 μm quantum cascade lasers based on diagonal transition and nonresonant extraction[J]. Photonics Research, 2019, 7(11): 1244
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