Abstract:Low cost, small footprint, highly efficient and mass producible on-chip wavelength-division-multiplexing (WDM) light sources are key components in future silicon electronic and photonic integrated circuits (EPICs) which can fulfill the rapidly increasing bandwidth and lower energy per bit requirements. We present here, for the first time, a low noise high-channel-count 20 GHz passively mode locked quantum dot laser grown on complementary metaloxide-semiconductor compatible on-axis (001) silicon substrate. The … Show more
“…Measurements without the use of the booster optical amplifier have shown that neither the −3 dB spectral width nor the timing jitter is influenced by the booster optical amplifier, only the baseline for L(f) at −120 dBc/Hz is increasing due to the lower power impinging onto the detector. The lowest identified value of 9 fs for the pulse-to-pulse timing jitter for this laser is 1.5 times higher than the one for the lowest timing jitter obtained so far by a passively mode-locked quantum dot laser on silicon of 6 fs at 20 GHz with a 1.6 times broader pulse width at this operation point [1] than the device presented in this work. in this area for nonlinear intensity auto-correlation.…”
Section: Mode-locking Pulse Train and Stability Characterizationcontrasting
confidence: 58%
“…In literature, line widths of 100 kHz (−3 dB) for a self mode-locked quantum dot laser on silicon [36] and 80 kHz for a similar device presented here [35] were reported indicating a 200-250 times broader repetition rate line width as compared to the here presented results although no precise pulse train stability analysis in terms of radio-frequency line width has been carried out yet for these devices. Additionally, in the results presented here, a 2.75 times narrower repetition rate line width is observed as compared to the reported repetition rate line width of 1.1 kHz from a complex tapered waveguide design from a silicon quantum-well laser [34] and 4.5 times narrower line width compared to the 1.8 kHz width reported for a monolithic InAs quantum dot passively mode-locked two-section laser on silicon [1]. Comparing the achieved timing stability with quantum dot passively mode-locked lasers on native substrates, except of silicon, repetition rate line widths ranging from 500 Hz up to 27 kHz [37,[39][40][41][42][43] have been reported.…”
Section: Mode-locking Pulse Train and Stability Characterizationcontrasting
confidence: 44%
“…Optical frequency comb passively mode-locked semiconductor quantum dot lasers directly grown on silicon are ideal sources for applications including high data rate optical communication applications in the O-band [1][2][3][4][5], spectroscopic sensing on a silicon photonics chip [6], dual-comb spectroscopy [7] and for silicon-chip based ultra-fast optical oscilloscopes [8]. Mode-locked quantum dot semiconductor lasers offer small size, higher functionality and lower energy consumption photonic integrated circuits on silicon, the material of choice for the photonics industry [2][3][4][9][10][11][12][13][14][15].…”
Section: Introductionmentioning
confidence: 99%
“…Subsequently, self mode-locking operation of a quantum dot on silicon laser without the need of any saturable absorber generated 490 fs short optical pulses has been reported at a repetition rate of 31 GHz and a repetition rate line width of 100 kHz [36]. The lowest repetition rate line width of a passively mode-locked quantum dot laser directly grown on silicon amounts to date to 1.8 kHz at a repetition rate of 20 GHz [1]. Shortest generated optical pulses from monolithic passively mode-locked quantum dot lasers grown on native substrates, except of silicon, are 360 fs [37] with a tapered waveguide design and 393 fs [38] for a two-section straight waveguide laser and 493 fs for a tapered three-section waveguide design [39].…”
Mode-locked InAs/InGaAs quantum dot lasers emitting optical frequency combs centered at 1310 nm are promising sources for high-speed and high-capacity communication applications. We report on the stable optical pulse train generation by a monolithic passively mode-locked edge-emitting two-section quantum dot laser based on a five-stack InAs/InGaAs dots-in-a-well structure directly grown on an on-axis (001) silicon substrate by solid-source molecular beam epitaxy. Optical pulses as short as 1.7 ps at a pulse repetition rate or intermode beat frequency of 9.4 GHz are obtained. A minimum pulse-to-pulse timing jitter of 9 fs, corresponding to a repetition rate line width of 400 Hz, is demonstrated. The generated optical frequency combs yield exceptional low amplitude jitter performance and comb widths exceed 5.5 nm at a −3 dB criteria, containing more than 100 comb carriers.
“…Measurements without the use of the booster optical amplifier have shown that neither the −3 dB spectral width nor the timing jitter is influenced by the booster optical amplifier, only the baseline for L(f) at −120 dBc/Hz is increasing due to the lower power impinging onto the detector. The lowest identified value of 9 fs for the pulse-to-pulse timing jitter for this laser is 1.5 times higher than the one for the lowest timing jitter obtained so far by a passively mode-locked quantum dot laser on silicon of 6 fs at 20 GHz with a 1.6 times broader pulse width at this operation point [1] than the device presented in this work. in this area for nonlinear intensity auto-correlation.…”
Section: Mode-locking Pulse Train and Stability Characterizationcontrasting
confidence: 58%
“…In literature, line widths of 100 kHz (−3 dB) for a self mode-locked quantum dot laser on silicon [36] and 80 kHz for a similar device presented here [35] were reported indicating a 200-250 times broader repetition rate line width as compared to the here presented results although no precise pulse train stability analysis in terms of radio-frequency line width has been carried out yet for these devices. Additionally, in the results presented here, a 2.75 times narrower repetition rate line width is observed as compared to the reported repetition rate line width of 1.1 kHz from a complex tapered waveguide design from a silicon quantum-well laser [34] and 4.5 times narrower line width compared to the 1.8 kHz width reported for a monolithic InAs quantum dot passively mode-locked two-section laser on silicon [1]. Comparing the achieved timing stability with quantum dot passively mode-locked lasers on native substrates, except of silicon, repetition rate line widths ranging from 500 Hz up to 27 kHz [37,[39][40][41][42][43] have been reported.…”
Section: Mode-locking Pulse Train and Stability Characterizationcontrasting
confidence: 44%
“…Optical frequency comb passively mode-locked semiconductor quantum dot lasers directly grown on silicon are ideal sources for applications including high data rate optical communication applications in the O-band [1][2][3][4][5], spectroscopic sensing on a silicon photonics chip [6], dual-comb spectroscopy [7] and for silicon-chip based ultra-fast optical oscilloscopes [8]. Mode-locked quantum dot semiconductor lasers offer small size, higher functionality and lower energy consumption photonic integrated circuits on silicon, the material of choice for the photonics industry [2][3][4][9][10][11][12][13][14][15].…”
Section: Introductionmentioning
confidence: 99%
“…Subsequently, self mode-locking operation of a quantum dot on silicon laser without the need of any saturable absorber generated 490 fs short optical pulses has been reported at a repetition rate of 31 GHz and a repetition rate line width of 100 kHz [36]. The lowest repetition rate line width of a passively mode-locked quantum dot laser directly grown on silicon amounts to date to 1.8 kHz at a repetition rate of 20 GHz [1]. Shortest generated optical pulses from monolithic passively mode-locked quantum dot lasers grown on native substrates, except of silicon, are 360 fs [37] with a tapered waveguide design and 393 fs [38] for a two-section straight waveguide laser and 493 fs for a tapered three-section waveguide design [39].…”
Mode-locked InAs/InGaAs quantum dot lasers emitting optical frequency combs centered at 1310 nm are promising sources for high-speed and high-capacity communication applications. We report on the stable optical pulse train generation by a monolithic passively mode-locked edge-emitting two-section quantum dot laser based on a five-stack InAs/InGaAs dots-in-a-well structure directly grown on an on-axis (001) silicon substrate by solid-source molecular beam epitaxy. Optical pulses as short as 1.7 ps at a pulse repetition rate or intermode beat frequency of 9.4 GHz are obtained. A minimum pulse-to-pulse timing jitter of 9 fs, corresponding to a repetition rate line width of 400 Hz, is demonstrated. The generated optical frequency combs yield exceptional low amplitude jitter performance and comb widths exceed 5.5 nm at a −3 dB criteria, containing more than 100 comb carriers.
“…Inhomogeneous broadening effect in self-assembled QD structure effectively broadens the optical gain bandwidth. It can enable widely tunable single-wavelength lasers [3] and large comb width to fit more wavelength channels [15]. But it also can easily support multiple longitudinal mode lasing in lasers without a fine wavelength selection mechanism, such as microring lasers whose lasing mode space is only determined by laser cavity free spectral range (FSR).…”
We demonstrate >6× modulation bandwidth extension of a heterogeneous quantum-dot microring laser using optical injection locking, obtaining 18 Gb/s on-off-keying modulation with clear open eyes. Single-mode lasing of all 11 longitudinal modes were achieved with >44 dB side-mode suppression and minimal 5 dB power increase.
Supercontinuum generation (SCG) through soliton fission provides high‐brightness, spectrally‐rich light needed for hyperspectral imaging, broadband spectroscopy, and fluorescence microscopy. The prospect of miniaturization has led to many demonstrations of this phenomenon in integrated platforms. However, due to the moderate dispersion and nonlinearity generally available in channel waveguides, femtosecond pulses have typically been required to date, as the use of picosecond pulses would require unpractically long devices to achieve soliton fission. Here, spectral bandwidth enhancement of the supercontinuum process through Bragg grating induced soliton‐effect compression and soliton fission is demonstrated. This approach uses picosecond pulses on a complementary metal oxide semiconductor (CMOS)‐compatible, millimeter‐scale platform, consisting of a monolithically integrated cladding‐modulated Bragg grating with a channel waveguide. The strong dispersion near the stopband of the grating enables compression and fission of picosecond higher‐order solitons, which enhances the spectral broadening in the channel waveguide. A 4.3 spectral bandwidth enhancement is reported, with respect to a reference waveguide of the same length. The output spectra are further studied both through simulations and experiments and determined to possess high spectral coherence. These results highlight a simple route to significantly augment the bandwidth of nonlinear processes such as SCG while maintaining low power and compact footprint.
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