• Laser & Optoelectronics Progress
  • Vol. 62, Issue 3, 0300001 (2025)
Luotian Huang*, Gengqin Liang, Zongge Li, Peiguang Yan, and Jinchuan Guo
Author Affiliations
  • Guangdong Province Key Laboratory of Optoelectronic Devices and Systems, College of Physics and Optoelectronic Engineering, Shenzhen University, Shenzhen 518060, Guangdong , China
  • show less
    DOI: 10.3788/LOP241171 Cite this Article Set citation alerts
    Luotian Huang, Gengqin Liang, Zongge Li, Peiguang Yan, Jinchuan Guo. Research Progress on Tunable Narrow Linewidth Semiconductor Lasers Integrated with External Cavity[J]. Laser & Optoelectronics Progress, 2025, 62(3): 0300001 Copy Citation Text show less
    Structure diagram of passive external cavity semiconductor laser
    Fig. 1. Structure diagram of passive external cavity semiconductor laser
    Composite cavity can be equivalent to a mirror with equivalent reflectivity[19]
    Fig. 2. Composite cavity can be equivalent to a mirror with equivalent reflectivity[19]
    Structure diagram of a basically wide-tunable III-V/Si based on multi-ring mirrors[37]
    Fig. 3. Structure diagram of a basically wide-tunable III-V/Si based on multi-ring mirrors[37]
    Tunable laser with SOA and external resonator. (a) Structure diagram[38]; (b) spectra of tunable lasers with different wavelengths[38]; (c) schematic of laser structure with asymmetric MZI[41]; (d) wavelength tuning of laser with asymmetry MZI at 90 mA injection current[41]; (e) calculated and measured linewidth versus output power plot[41]; (f) schematic of tunable laser integrated with SOA and silicon photonic filter chip[43]; (g) laser spectrum in the 65 nm range[43]
    Fig. 4. Tunable laser with SOA and external resonator. (a) Structure diagram[38]; (b) spectra of tunable lasers with different wavelengths[38]; (c) schematic of laser structure with asymmetric MZI[41]; (d) wavelength tuning of laser with asymmetry MZI at 90 mA injection current[41]; (e) calculated and measured linewidth versus output power plot[41]; (f) schematic of tunable laser integrated with SOA and silicon photonic filter chip[43]; (g) laser spectrum in the 65 nm range[43]
    Concept diagram of a wide tunable laser array covering the entire low-loss fiber optic telecommunications window[46]. (a) Schematic of Si ring resonator lasers bonded with III-V gain materials in O-band, E-band, and S-C-L bands on common SOI wafers; (b) microscope images of ring resonators, phase shifters, and ring mirrors
    Fig. 5. Concept diagram of a wide tunable laser array covering the entire low-loss fiber optic telecommunications window[46]. (a) Schematic of Si ring resonator lasers bonded with III-V gain materials in O-band, E-band, and S-C-L bands on common SOI wafers; (b) microscope images of ring resonators, phase shifters, and ring mirrors
    Structure diagram of tunable laser based on an air bridge structure waveguide ring cavity[53]
    Fig. 6. Structure diagram of tunable laser based on an air bridge structure waveguide ring cavity[53]
    External cavity narrow linewidth laser[12]. (a) Structure diagram; (b) spectrum of lasers (tuning range is from 1545.5 nm to 1550.4 nm); (c) frequency noise of a free-running DFB laser and the proposed external cavity laser corresponding to an intrinsic linewidth of 49.70 kHz and 27.17 Hz, respectively
    Fig. 7. External cavity narrow linewidth laser[12]. (a) Structure diagram; (b) spectrum of lasers (tuning range is from 1545.5 nm to 1550.4 nm); (c) frequency noise of a free-running DFB laser and the proposed external cavity laser corresponding to an intrinsic linewidth of 49.70 kHz and 27.17 Hz, respectively
    InP-Si3N4 hybrid laser.(a) Schematic diagram of a hybrid laser[57]; (b) superimposed spectra when coarsely tuning over a 43 nm wide range (left), superimposed spectra when fine-tuning over a range of 0.8 nm via tuning both MRRs simultaneously (right), achieving a stepwise sweeping of the wavelength at the FSR of the whole laser cavity[59]; (c) recorded beat signal at a driving current of 196 mA and a laser output wavelength of 1578.12 nm, Lorentz fitting linewidth is 87 kHz[60]; (d) schematic diagram of a laser integrating InP and GaAs gain chips[61]; (e) superimposed spectra when thermally tuning a microresonator, and the tuning range is 46 nm[61]; (f) recorded RF beat spectrum (red dots), the blue line shows a Lorentzian fit corresponding to a laser linewidth of 18 kHz[61]; (g) schematic diagram of the III-V/Si3N4 hybrid laser[63]; (h) superimposed spectra, tuning range is 172 nm[64]
    Fig. 8. InP-Si3N4 hybrid laser.(a) Schematic diagram of a hybrid laser[57]; (b) superimposed spectra when coarsely tuning over a 43 nm wide range (left), superimposed spectra when fine-tuning over a range of 0.8 nm via tuning both MRRs simultaneously (right), achieving a stepwise sweeping of the wavelength at the FSR of the whole laser cavity[59]; (c) recorded beat signal at a driving current of 196 mA and a laser output wavelength of 1578.12 nm, Lorentz fitting linewidth is 87 kHz[60]; (d) schematic diagram of a laser integrating InP and GaAs gain chips[61]; (e) superimposed spectra when thermally tuning a microresonator, and the tuning range is 46 nm[61]; (f) recorded RF beat spectrum (red dots), the blue line shows a Lorentzian fit corresponding to a laser linewidth of 18 kHz[61]; (g) schematic diagram of the III-V/Si3N4 hybrid laser[63]; (h) superimposed spectra, tuning range is 172 nm[64]
    Vision of the integrated platform[65](inset: microscope image of the ring resonator before microheater deposition, and the waveguide is fabricated using 175 nm thick Si3N4 surrounded by SiO2)
    Fig. 9. Vision of the integrated platform[65](inset: microscope image of the ring resonator before microheater deposition, and the waveguide is fabricated using 175 nm thick Si3N4 surrounded by SiO2)
    Narrow linewidth self-injection locked laser. (a) Schematic of laser structure[75]; (b) comparison of linewidth between free-running DFB laser and laser locked into LN micro ring cavity by self-injection[75]; (c) tuning of laser wavelength by applying electrical power[75]; (d) schematic of narrow linewidth laser hybrid integration with external cavity chip and commercial DFB laser[78]; (e) frequency noise of the laser using LN external cavity chip is reduced by 1/169 compared to free-running DFB, and linewidth is reduced to 2.5 kHz[78]; (f) emission spectra[78]
    Fig. 10. Narrow linewidth self-injection locked laser. (a) Schematic of laser structure[75]; (b) comparison of linewidth between free-running DFB laser and laser locked into LN micro ring cavity by self-injection[75]; (c) tuning of laser wavelength by applying electrical power[75]; (d) schematic of narrow linewidth laser hybrid integration with external cavity chip and commercial DFB laser[78]; (e) frequency noise of the laser using LN external cavity chip is reduced by 1/169 compared to free-running DFB, and linewidth is reduced to 2.5 kHz[78]; (f) emission spectra[78]
    Integrated platformRefractive indexNonlinear coefficient /(10-19 m2·W-1Two-photon absorption /nmHighest Q /106
    SiO21.450.22280270
    SiN2.02.54602.6×105
    Si3.55022500.6
    LiNbO32.21.82.2
    Table 1. Performance comparison of different types of integrated photonic device platforms[30-33]
    Material

    Cavity

    structure

    Integrated methodYearWavelength /nmTuning rangeMaximum output powerLinewidthSMSR /dBRef.
    SiSGDBRHybrid integrated20081501‒151413 nm2.5 mW>3035
    MRRsHybrid integrated2009C and L38 nm1.6 mW>3038
    MRRs and Loop mirrorHybrid integrated20121570‒162044 nm5 mW<70 kHz>3013
    MRRs and Directional couplerHybrid integrated2014C35 nm20 mW0.22 pm4039
    MRRs and MZIHybrid integrated2015C42.7 nm30 mW12 kHz41
    MRRsHybrid integrated2019C65 nm21.5 dBm60 kHz>5043
    MRRs and loop mirrorHybrid integrated20201647‒169043 nm31.1 mW0.7 kHz46.0144
    MRRsHeterogeneous integrated2020S, C, and L110 nm3 mW220 Hz>5037
    MRRsHeterogeneous integrated2022S, C, and L118 nm15 mW<95 Hz>4011
    MRRsHeterogeneous integrated20231350‒140858 nm>10 mW20 kHz46
    SiO2MRRs and Sagnac reflector-2007C and L96 nm15 dBm>5052
    MRRs and loop mirror-2010C35 nm>16 dBm<100 kHz4553
    MRRs and MMIHybrid integrated2017C and L66 nm10 dBm1 kHz5055
    MRRs and directional couplerHybrid integrated20231545.5‒1550.44.9 nm27 Hz12
    SiNMRRsHybrid integrated2016C43 nm1.7 mW90 kHz3557
    MRRs and loop mirrorHybrid integrated20171500‒158181 nm13 mW290 Hz58
    MRRsHybrid integrated2019155046 nm15 mW18 kHz6061
    MRRs and tunable Sagnac loopHybrid integrated20201500‒1660160 nm17.5 mW26 kHz>4563
    MRRsHybrid integrated2021C30 mW1.2 Hz33
    MRRs and Sagnac reflectorHybrid integrated2022404‒78512.5 nm10 mW8 kHz>3565
    MRRsHybrid integrated2023C55 nm220 mW<8 kHz>5066
    LNMRRs and DBRHybrid integrated20211304‒134036 nm2.5 mW>6037
    MRRsHeterogeneous integrated(μTP)20211534‒155521 nm0.77 mW1.5 MHz>3079
    MRRs and DBR and MZMHybrid integrated2022132040 nm2 mW475 kHz>6076
    MRRHeterogeneous integrated20231555.41.2 GHz0.15 mW3 kHz5077
    MRRHybrid integrated202415503.18 mW2.5 kHz6078
    Table 2. Performance comparison of integrated passive external cavity semiconductor lasers with different materials
    Luotian Huang, Gengqin Liang, Zongge Li, Peiguang Yan, Jinchuan Guo. Research Progress on Tunable Narrow Linewidth Semiconductor Lasers Integrated with External Cavity[J]. Laser & Optoelectronics Progress, 2025, 62(3): 0300001
    Download Citation