Photonics Research, Volume. 13, Issue 1, 31(2025)

Ultra-linear FMCW laser based on time-frequency self-injection locking Editors' Pick

Jichen Zhang, Shangyuan Li, Xiaoping Zheng, and Xiaoxiao Xue*
Author Affiliations
  • Department of Electronic Engineering, Tsinghua University, Beijing 100084, China
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    Figures & Tables(12)
    (a) Schematic diagram of the time-frequency self-injection locking. (b) Illustration of the frequency-shifted self-injection locking.
    Simulation results of instantaneous laser linewidth. (a) Drive current. (b) Instantaneous frequency (red) and residual error (blue) corresponding to (a). (c) Normalized spectrum of a free-running laser calculated by removing the frequency chirp. The linewidth is approximately 5 MHz. (d) Evolution of laser linewidth with feedback ratio. (e)–(l) Spectra of a self-injection locked laser with various feedback ratio and loop phase shift: (e) −70 dB, π/2; (f) −55 dB, π/2; (g) −40 dB, π/2; (h) −25 dB, π/2; (i) −70 dB, 3π/2; (j) −55 dB, 3π/2; (k) −40 dB, 3π/2; and (l) −25 dB, 3π/2. The insets are enlarged spectra.
    Simulation results of frequency-sweep nonlinearity. (a)–(c) Residual error of a free-running laser with the harmonic orders of 2, 20, and 100. (d)–(o) Residual error of a self-injection locked laser with various feedback ratios and harmonic orders: (d) −70 dB, m=2; (e) −70 dB, m=20; (f) −70 dB, m=100; (g) −55 dB, m=2; (h) −55 dB, m=20; (i) −55 dB, m=100; (j) −40 dB, m=2; (k) −40 dB, m=20; (l) −40 dB, m=100; (m) −20 dB, m=2; (n) −20 dB, m=20; (o) −20 dB, m=100; and (p) evolution of sweep nonlinearity with feedback ratio.
    Simulation results when both the laser spontaneous emission noise and the sweep nonlinearity are considered. (a) Residual frequency-sweep error of the free-running (blue) and self-injection locked (red) laser. (b) Zoom-in plot of the result of self-injection locked laser.
    Experimental setup of the self-injection locked frequency-swept laser. DFB, distributed feedback; AOM, acousto-optic modulator; EDFA, erbium-doped fiber amplifier; AFG, arbitrary function generator; RF, radio frequency.
    Laser frequency noise and linewidth measurement. (a) Schematic diagram of the setup. LUT, light under test; AOM, acousto-optic modulator; RF, radio frequency; PD, photodetector; PNA, phase noise analyzer; ESA, electrical spectrum analyzer. (b) Frequency noise of the free-running and self-injection locked laser. (c) Beat note spectra of the free-running (FR) laser and self-injection locked laser (SIL); the inset is the enlarged spectrum of the self-injection locked laser.
    Predistortion method and results. (a) Schematic diagram of the predistortion for frequency-sweep linearization without self-injection. AFG, arbitrary function generator; MZI, Mach–Zehnder interferometer; BPD, balanced photodetector; OSC, oscilloscope. (b) Averaged residual RMS evolution with the number of iterations. (c) Predistorted drive current. (d) and (e) Residual RMS of free-running laser driven by predistorted current in (d) down and (e) up ramp, respectively. (f) and (g) Residual RMS of free-running laser driven by initial current in (f) down and (g) up ramp, respectively.
    Self-injection locking results. (a) Beat signal spectra of the free-running (FR) and self-injection locked (SIL) lasers. (b) Enlarged spectra of (a); the central frequency is 2.046 MHz. (c), (d) Residual errors with and without self-injection locking in down and up ramps. (e), (f) Enlarged residual errors of injected laser in down and up ramps.
    Laser ranging setup and results. (a) Schematic diagram of the FMCW LiDAR. PD, photodetector; OSC, oscilloscope. (b) Range resolution versus target distance and the theoretical resolution limits with a self-injection locked laser. (c)–(e) Beat signal spectra of free-running laser (blue) and self-injection locked laser (red) at different distances: (c) 21.118 m, (d) 1018.85 m, and (e) 10,002.1 m.
    Range and velocity measurement accuracies. (a) Range accuracy versus target distance. (b) Velocity measurement result and accuracy versus target distance.
    • Table 1. Simulation Parameters

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      Table 1. Simulation Parameters

      ParameterValueUnitMeaning
      ξ4×103s1Differential gain coefficient
      ΓE8.3×1011s1Photon decay rate
      ΓN1×109s1Carrier decay rate
      Nth2.5×108 Carrier inversion at threshold
      β1×104s1Spontaneous emission coupling coefficient
      α6 Linewidth enhancement factor
      Rs0.36 Facet reflection coefficient
      τs45.3psDiode-cavity round-trip time
      τe60nsExternal round-trip time
      εν1.283×1019JSingle photon energy
      Ω0193.55×10122π×rad/sLaser frequency at threshold
      T0300KRoom temperature
      αT5×106K1Thermal expansion coefficient
      βT5×105K1Temperature coefficient of refractive index
      Kd9×102W/KHeat dissipation rate
      CT2×106J/KTotal heat capacity
    • Table 2. Methods and Metrics of Several Typical FMCW Light Sources

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      Table 2. Methods and Metrics of Several Typical FMCW Light Sources

      Ref.LaserBandwidthRelative NonlinearityRange Resolution (in Air)Method
      [23]DFB15 GHz1.6×105External modulation
      [6]VCSEL155 GHz4.2×1050.97 mm at 38 cmCurrent predistortion
      [7]DFB26 GHz5.8×1055.8 mm at 50 cmCurrent predistortion
      [10]DFB50 GHz1.8×10626.3 cm at 1.13 kmComposite phase-locked loop
      [11]DFB60 GHz2.7×1062.5 mm at 4.8 kmPhase-locking to a swept comb
      [16]DFB10.3 GHz9.3×1053 cm at 252 mMicro-resonator self-injection locking
      This workDFB100 GHz6.4×1071.6 mm at 300 m, 8.1 mm at 1 kmTime-frequency self-injection locking
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    Jichen Zhang, Shangyuan Li, Xiaoping Zheng, Xiaoxiao Xue, "Ultra-linear FMCW laser based on time-frequency self-injection locking," Photonics Res. 13, 31 (2025)

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    Paper Information

    Category: Lasers and Laser Optics

    Received: Jul. 29, 2024

    Accepted: Oct. 11, 2024

    Published Online: Dec. 13, 2024

    The Author Email: Xiaoxiao Xue (xuexx@tsinghua.edu.cn)

    DOI:10.1364/PRJ.537952

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