• Photonics Research
  • Vol. 8, Issue 9, 1428 (2020)
Zeyu Zhang1、2、*, Justin C. Norman2, Songtao Liu3, Aditya Malik1, and John E. Bowers1、2、3
Author Affiliations
  • 1Electrical and Computer Engineering Department, University of California Santa Barbara, Santa Barbara, California 93106, USA
  • 2Materials Department, University of California Santa Barbara, Santa Barbara, California 93106, USA
  • 3Institute for Energy Efficiency, University of California, Santa Barbara, California 93106, USA
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    DOI: 10.1364/PRJ.397175 Cite this Article Set citation alerts
    Zeyu Zhang, Justin C. Norman, Songtao Liu, Aditya Malik, John E. Bowers. Integrated dispersion compensated mode-locked quantum dot laser[J]. Photonics Research, 2020, 8(9): 1428 Copy Citation Text show less
    (a) Schematic diagram of the epitaxial structure of OQD devices. (b) Optical confinement as functions of passive GaAs WG thickness.
    Fig. 1. (a) Schematic diagram of the epitaxial structure of OQD devices. (b) Optical confinement as functions of passive GaAs WG thickness.
    (a) Schematic diagram of OQD MLL above the bottom cladding. The rendering is not to scale. The WG spiral termination is not illustrated here for simplicity. Scanning electron microscope (SEM) images of (b) mesa cross section after the nonselective GaAs etch, (c) passive GaAs WG cross section with 1 μm thick silicon dioxide upper cladding, (d) GaAs WG with gratings etched on the sidewall, and (e) taper transition from the active to the passive WG section.
    Fig. 2. (a) Schematic diagram of OQD MLL above the bottom cladding. The rendering is not to scale. The WG spiral termination is not illustrated here for simplicity. Scanning electron microscope (SEM) images of (b) mesa cross section after the nonselective GaAs etch, (c) passive GaAs WG cross section with 1 μm thick silicon dioxide upper cladding, (d) GaAs WG with gratings etched on the sidewall, and (e) taper transition from the active to the passive WG section.
    (a) Reflectivities and (b) group delay responses of several grating designs simulated with the transmission matrix technique. Red: uniform grating, κ=162 cm−1. Pink: linearly chirped grating, CR=−0.032 nm/μm. Blue and green: chirped and apodized gratings, CR=−0.032 nm/μm. For pink and blue, κ=162 cm−1 at the half length of the grating. For green, κ=243 cm−1 at the half length.
    Fig. 3. (a) Reflectivities and (b) group delay responses of several grating designs simulated with the transmission matrix technique. Red: uniform grating, κ=162  cm1. Pink: linearly chirped grating, CR=0.032  nm/μm. Blue and green: chirped and apodized gratings, CR=0.032  nm/μm. For pink and blue, κ=162  cm1 at the half length of the grating. For green, κ=243  cm1 at the half length.
    (a) CW LIV curves for 20 GHz OQD MLL with SA in a floating state. Blue: laser A. Pink: laser B. Green: laser C. (b) Optical spectra under the bias conditions Igain=129 mA, 179 mA, 94 mA and VSA=5.6 V, 2.7 V, 4.3 V for lasers A–C, respectively. (c) RF spectrum for laser C under the same bias condition in 50 GHz span view.
    Fig. 4. (a) CW LIV curves for 20 GHz OQD MLL with SA in a floating state. Blue: laser A. Pink: laser B. Green: laser C. (b) Optical spectra under the bias conditions Igain=129  mA, 179 mA, 94 mA and VSA=5.6  V, 2.7 V, 4.3 V for lasers A–C, respectively. (c) RF spectrum for laser C under the same bias condition in 50 GHz span view.
    Pulse width mapping as a function of gain section current and SA section reverse bias voltage under passive mode-locking operation for laser C. Regions marked by white indicate unsuccessful PML.
    Fig. 5. Pulse width mapping as a function of gain section current and SA section reverse bias voltage under passive mode-locking operation for laser C. Regions marked by white indicate unsuccessful PML.
    (a) Autocorrelator traces of the narrowest pulses of OQD MLLs with various grating designs. Blue, red, green, pink, and brown circles represent lasers A–E, respectively. Sech2 fitting gives pulse widths of 12.8, 14.4, 5.3, 7.6, and 4.5 ps. The bias conditions for narrowest pulses are Igain=129 mA, 179 mA, 94 mA, 108 mA, 101 mA and VSA=5.6 V, 2.7 V, 4.3 V, 0 V, 6.2 V, for lasers A–E, respectively.
    Fig. 6. (a) Autocorrelator traces of the narrowest pulses of OQD MLLs with various grating designs. Blue, red, green, pink, and brown circles represent lasers A–E, respectively. Sech2 fitting gives pulse widths of 12.8, 14.4, 5.3, 7.6, and 4.5 ps. The bias conditions for narrowest pulses are Igain=129  mA, 179 mA, 94 mA, 108 mA, 101 mA and VSA=5.6  V, 2.7 V, 4.3 V, 0 V, 6.2 V, for lasers A–E, respectively.
     MLL AMLL BMLL CMLL DMLL E
    ApodizationNoneGaussianGaussianGaussianGaussian
    CR (nm/μm)00.032−0.032−0.016−0.032
    κ at grating center (cm1)260260260260350
    Threshold current (mA)6158798391
    Wavelength at grating reflection peak (nm)1293.11292.11297.21295.21288.4
    Minimum pulse width (ps)12.814.45.37.64.5
    Table 1. MLL Design and Performance Parameters
    Zeyu Zhang, Justin C. Norman, Songtao Liu, Aditya Malik, John E. Bowers. Integrated dispersion compensated mode-locked quantum dot laser[J]. Photonics Research, 2020, 8(9): 1428
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