The nonlinear dynamical characteristics of an integrated mutual-injection semiconductor laser (IMSL) with three-section are numerically simulated, and Hopf bifurcation diagrams of its output characteristics varying with different input parameters are presented. The simulation results in this paper indicate that by varying some operating parameters such as coupling strength and detuning frequency of an IMSL, its output exhibits rich nonlinear dynamical behaviors such as injection locking, period-one oscillations, period-two oscillations, multi-period oscillations, quasi-period oscillations, and chaos oscillations. In this paper, we explore the effect of parameter changes of IMSL on its output characteristics, numerically simulate these phenomena and reflect in the Hopf bifurcation diagram.
The integrated mutual injection laser consists of a front section laser (FSL), a phase-section laser and a rear section laser (RSL). By adjusting the current of the two DFB lasers, the cavity modes of the FSL and RSL coexist in a period-one (P1) state, and the integrated laser is a dual-mode output. The beat frequency (fLO) can be obtained as the optical local oscillator (LO) frequency. When the linear frequency modulation (LFM) signal is directly modulated onto the front section laser of the integrated laser, after passing through the photodetector, the two main oscillation modes will beat with the first-order optical modulation sideband of the other mode, thereby generating the new frequency signals (fLO±fLFM). When the fundamental frequency signal or fLO is tuned, a double chirp signal with opposite chirp rate can be generated in different frequency ranges. In the simulation experiment demonstration, DCMWs in the frequency range of 11~17 GHz and 5~9 GHz are obtained respectively, and the corresponding time bandwidth product (TBWP) reaches 800. The full width at half maximum (FWHM) can reach 0.272 ns, and the peak sidelobe ratio (PSR) can reach 21.45 dB. The scheme is beneficial to further enrich the transmitting frequency band of radar detection signal. The principle is simple, the integration is high, the operation is convenient, and the frequency is adjustable.
KEYWORDS: Signal generators, Radar signal processing, Laser frequency, Picosecond phenomena, Signal processing, Frequency response, Frequency modulation, X band, Spectrum analysis, Microwave photonics
In this paper, the simple multi-band triangular frequency modulation (TFM) signals generation with multiplying bandwidth and center frequency using photon-photon resonance (PPR) effect in three-section monolithic integrated directly-modulated laser (TS_MIDML) has been experimentally demonstrated. The traditional optical-injection system replaced by the TS_MIDML, and the high-speed external modulator, polarization controller and filter are eliminated in this paper. A three-band TFM signals with carrier frequencies ranging from X-band to K-band are given as an example, and the time bandwidth product (TBWP) up to 20000. The numbers of bands and TBWP of generated signals could be easily adjusted by tuning the reference signal from arbitrary waveform generator (AWG). The results of auto-correlations of the generated waveforms are also given.
A simple photonic approach to generating the wideband optical frequency comb (OFC) based on the monolithic integrated semiconductor laser (MISL) subject to the gain-switching effect is proposed and experimentally demonstrated in this work. The impressive hotspots focus on the two following aspects. One is the core device, i.e., MISL, which integrates two DFB lasers onto one chip simultaneously. It is equipped with numerous physical characteristics such as low volume, power consumption, easily integration and so on at the mean time of guaranteeing the nonlinear dynamics of the semiconductor laser itself. The other advantage is the OFC generator (OFCG) is fully self-oscillating attributing to the fact that the feedback RF signal applied to modulate the laser is provided by the MISL itself. In this case, no additional microwave driver is required, leading to the system flexible and convenient. In the experiment, one discernible OFC with a bandwidth of 70.2 GHz and a comb line of 11 within 5-dB amplitude variation is obtained, suggesting this method huge effectiveness.
Recent advances in monolithically integrated multi-section semiconductor lasers (MI-MSSLs) have propelled microwave photonic technologies to new potentials with a compact, reliable, and green implementation. Much research has examined that MI-MSSLs can realize the same or even better microwave photonic functions compared to discrete lasers by taking advantages of enhanced light–matter interactions. They are beneficial towards the future of integrated microwave photonics (IMWP) once integrating the other optical components such as modulators, amplifiers, transmission waveguide and so on. Herein, these recent advances in this emerging field are reviewed and discussed. Three main kinds of MI-MSSL structures are demonstrated including passive feedback laser, active feedback laser, as well as monolithically integrated mutually injected semiconductor laser. Their pros and cons are distinguished and compared through analyzing the desired characteristic indicators in modern MWP subsystems. The focus of this paper is on the photonic microwave techniques based on the nonlinear dynamics of MI-MSSLs, consisting of electro-optic conversion characteristics enhancement, photonic microwave generation, microwave photonic filter, as well as multiwavelength laser array for wavelength division multiplexing radio-over-fiber (WDM-RoF) networks. We also take a look at the future prospective at the research directions and challenges in this area.
Optical injection is an effective way to generate a tuned microwave photonic filter (MPF). However, the tuning range of the optical injection-based MPF is limited by the nonlinear dynamics and the nonideal roll-off optical filter. To enlarge the tuning range of the MPF, a polarization modulated optical signal injection distributed feedback semiconductor laser is employed. The method is free from the nonlinear dynamics and the nonideal roll-off optical filter. The experimental result shows that the proposed MPF can be tuned from 0 to 40 GHz by directly tuning the center wavelength of the optical carrier. The tuning range can be increased if polarization modulator and photodetector with larger bandwidth are exploited. To the best of our knowledge, this is the largest frequency tuning range of optical injection-based MPF.
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