Chinese Journal of Lasers, Volume. 47, Issue 7, 701007(2020)

Progress in Quantum Cascade Lasers

Liu Fengqi1,2、*, Zhang Jinchuan1, Liu Junqi1,2, Zhuo Ning1, Wang Lijun1,2, Liu Shuman1,2, Zhai Shenqiang1, Liang Ping1, Hu Ying1, and Wang Zhanguo1,2
Author Affiliations
  • 1Key Laboratory of Semiconductor Materials Science, 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
  • show less
    Figures & Tables(15)
    Structure of light emission using intersubband transitions in quantum wells. (a) Photon-assisted quantum tunneling in cascaded quantum wells to achieve optical amplification; (b) photon-assisted quantum tunneling structure in cascaded quantum wells
    Diagram of conduction band structure under the bias of QCL active region
    Growth structure of the QCL
    Band structure of QCL active designs. (a) Double-LO phonon resonance[6]; (b) non-resonant extraction[8]
    Conduction band diagram of coupled quantum wells active region responsible for laser action under an applied electric field. (a) In0.53Ga0.47As/In0.52Al0.48As material lattice matched to InP with ΔEc=520 meV; (b) strain compensated In1-xGaxAs/In1-yAlyAs material on InP with ΔEc>520 meV, where xy>0.48
    Parameters of different material systems. (a) Lattice constant; (b) energy gap; (c) band offset
    Band structure and performance of long-infrared InAs-based QCL. (a) Conduction band diagram of InAs/AlSb QCL emitting at 20 μm. (b) voltage-current and light-current characteristics of a laser in pulsed mode, insert is emission spectrum of the laser
    Highest continuous-wave optical power for room temperature QCLs reported in the wavelength range from 3.5 μm to 10.7 μm[32]
    Typical band structures of QCL. (a) Band diagram of an In0.72Ga0.28As/In0.22Al0.78As QCL structure based on non-resonant extraction design for light emission at 4.7 μm[36]; (b) band diagram of an In0.53Ga0.47As/In0.52Al0.48As/In0.69Ga0.31As/In0.36Al0.64As/AlAs QCL structure based on shallow-well combined with tall ba
    Structure of an eight element buried ridge type QCL array by a tree-array multimode interferometer[44]
    Band structure and performance of broad-gain spectrum QCL[51]. (a) Active conduction band diagram based on dual-upper-state to multiple-lower-state design for center emission at 6.8 μm, the material is strain-balanced In0.6Ga0.4As/ In0.44Al0.56As; (b) EL spectra at room temperature QCL
    Low power consumption substrate emitting DFB-QCL. (a) Schematic of substrate emitting porous InP DFB-QCL; (b) light-current characteristics of a substrate emitting DFB-QCL laser in continuous wave mode at room temperature
    • Table 1. Thermal conductivity and coefficient of thermal expansion of different heatsinks

      View table

      Table 1. Thermal conductivity and coefficient of thermal expansion of different heatsinks

      MaterialThermal conductivity /[W/(m·K)]Coefficient of thermalexpansion /K-1
      InP704.5×10-6
      Cu39317×10-6
      AlN2304.5×10-6
      SiC5004.0×10-6
      Diamond20002.3×10-6
    • Table 2. Companies and research institutes for infrared QCLs and application-packages

      View table

      Table 2. Companies and research institutes for infrared QCLs and application-packages

      Company nameCountryQCLwaferQCLmoduleQCLcomponentQCLsystem
      AdTech Optics Inc.CA
      Alpes LasersSwitzerland
      Pranalytica Inc.USA
      NanoplusGermany
      Cascade TechnologiesUSA
      Daylight Solution Inc.USA
      HamamatsuJapan
      Alcatel-Thales III-V LabFrance
      Institute of SemiconductorsChina
      AKELA laserUSA
      Frankfurt LaserGermany
      Thorlab (Maxion Technologies)USA
      Sacher LasertechnikGermany
      Physical Sciences Inc.New England
      Block EngineeringUSA
      Wavelength Opto-ElectronicUSA
      Neoplas Control InC.Germany
      Opto-Knowledge SystemsUSA
    • Table 3. Comparison of results from low threshold and power consumption of DFB-QCLs

      View table

      Table 3. Comparison of results from low threshold and power consumption of DFB-QCLs

      Research group /countryWavelength /μmThresholdcurrent /mADevice size /(μm×mm)Jth /(kA/cm2)Threshold powerconsumption /W
      ETH-Zürich/Switzerland4.558@20 ℃3×11.930.8
      Corning/USA4.570@20 ℃3×1.51.560.69
      Transmission DevicesR&D Lab/Japan7.465@27 ℃5×0.52.60.52
      California Institute ofTechnology, Pasadena,California/USA4.876.2@20 ℃4×11.910.76
      4.548@20 ℃3.5×0.751.830.5
      Alpes Lasers/Switzerland5.258@20 ℃6.6×0.751.170.5
      7.8100@20 ℃10.5×0.751.270.75
      Transmission DevicesR&D Lab/Japan7.452@20 ℃5×0.52.080.44
      Institute ofSemiconductors/China4.2126@20 ℃8×20.791.4
      4.6180@20 ℃14×1.50.862.3
      7.2150@20 ℃9.5×20.791.9
      4.9(surfaces-emitting)100@20 ℃13×10.811.27
      57.4@20 ℃9×10.640.7
      30@20 ℃9×0.50.670.42
    Tools

    Get Citation

    Copy Citation Text

    Liu Fengqi, Zhang Jinchuan, Liu Junqi, Zhuo Ning, Wang Lijun, Liu Shuman, Zhai Shenqiang, Liang Ping, Hu Ying, Wang Zhanguo. Progress in Quantum Cascade Lasers[J]. Chinese Journal of Lasers, 2020, 47(7): 701007

    Download Citation

    EndNote(RIS)BibTexPlain Text
    Save article for my favorites
    Paper Information

    Special Issue:

    Received: Mar. 9, 2020

    Accepted: --

    Published Online: Jul. 10, 2020

    The Author Email: Fengqi Liu (fqliu@semi.ac.cn)

    DOI:10.3788/CJL202047.0701007

    Topics