[1] Ohtsubo J[M]. Semiconductor lasers: stability, instability and chaos(2012).

[2] Chan S C, Liu J M. Tunable narrow-linewidth photonic microwave generation using semiconductor laser dynamics[J]. IEEE Journal of Selected Topics in Quantum Electronics, 10, 1025-1032(2004).

[3] Feng L Y, Gao H Z, Zhang J X et al. FPGA-based digital chaotic anti-interference lidar system[J]. Optics Express, 29, 719-728(2021).

[4] Wang B J, Wang Y C, Kong L Q et al. Multi-target real-time ranging with chaotic laser radar[J]. Chinese Optics Letters, 6, 868-870(2008).

[5] Uchida A, Amano K, Inoue M et al. Fast physical random bit generation with chaotic semiconductor lasers[J]. Nature Photonics, 2, 728-732(2008).

[6] Wu J G, Wu Z M, Liu Y R et al. Simulation of bidirectional long-distance chaos communication performance in a novel fiber-optic chaos synchronization system[J]. Journal of Lightwave Technology, 31, 461-467(2013).

[7] Yan S L. Theory and technique of cross transmittance and alternate parallel reception of laser chaos in secure communication[J]. Chinese Journal of Lasers, 47, 0906001(2020).

[8] Wang L S, Mao X X, Wang A B et al. Scheme of coherent optical chaos communication[J]. Optics Letters, 45, 4762-4765(2020).

[9] Simpson T B. Mapping the nonlinear dynamics of a distributed feedback semiconductor laser subject to external optical injection[J]. Optics Communications, 215, 135-151(2003).

[10] Zhou H J, Chen M, Yao Q et al. Characteristics of distributed feedback semiconductor laser injection locking and applications to optical fiber sensing[J]. Chinese Journal of Lasers, 38, 0705002(2011).

[11] Hwang S K, Liu J M. Dynamical characteristics of an optically injected semiconductor laser[J]. Optics Communications, 183, 195-205(2000).

[12] Lin F Y, Tu S Y, Huang C C et al. Nonlinear dynamics of semiconductor lasers under repetitive optical pulse injection[J]. IEEE Journal of Selected Topics in Quantum Electronics, 15, 604-611(2009).

[13] Chan S C, Tang W K S. Chaotic dynamics of laser diodes with strongly modulated optical injection[J]. International Journal of Bifurcation and Chaos, 19, 3417-3424(2009).

[14] Tseng C H, Hwang S K. Broadband chaotic microwave generation through destabilization of period-one nonlinear dynamics in semiconductor lasers for radar applications[J]. Optics Letters, 45, 3777-3780(2020).

[15] Zeng Y, Zhou P, Huang Y et al. Optical chaos generated in semiconductor lasers with intensity-modulated optical injection: a numerical study[J]. Applied Optics, 60, 7963-7972(2021).

[16] Desmet R, Virte M. Laser diodes with modulated optical injection: towards a simple signal processing unit?[J]. Journal of Physics: Photonics, 2, 025002(2020).

[17] Vinckier Q, Duport F, Smerieri A et al. High-performance photonic reservoir computer based on a coherently driven passive cavity[J]. Optica, 2, 438-446(2015).

[18] Yoshimura K, Muramatsu J, Davis P et al. Secure key distribution using correlated randomness in lasers driven by common random light[J]. Physical Review Letters, 108, 070602(2012).

[19] Wu C R, Gao H, Wang L S et al. High-speed secure key distribution based on symmetric phase-shift-keying chaos synchronization[J]. Chinese Journal of Lasers, 49, 0406001(2022).

[20] Xu M F, Pan W, Zhang L Y. Secure remote synchronization and secure key distribution in electro-optic networks revealed by symmetries[J]. Optics Communications, 418, 41-45(2018).

[21] Nakayama J, Kanno K, Uchida A. Laser dynamical reservoir computing with consistency: an approach of a chaos mask signal[J]. Optics Express, 24, 8679-8692(2016).

[22] Yoshimura K, Valiusaityte I, Davis P. Synchronization induced by common colored noise in limit cycle and chaotic systems[J]. Physical Review E, 75, 026208(2007).

[23] Jiang N, Zhao A K, Liu S Q et al. Chaos synchronization and communication in closed-loop semiconductor lasers subject to common chaotic phase-modulated feedback[J]. Optics Express, 26, 32404-32416(2018).

[24] Gao H, Wang A B, Wang L S et al. 0.75 Gbit/s high-speed classical key distribution with mode-shift keying chaos synchronization of Fabry-Perot lasers[J]. Light: Science & Applications, 10, 172(2021).

[25] Guo G L, Jia Z W, Wang A B et al. Chaotic dynamics in DBR laser with noise-light injection[J]. Chinese Journal of Lasers, 48, 2301003(2021).

[26] Yoshimura K, Uchida A, Davis P et al. Synchronization of semiconductor lasers by common optical injection with constant-amplitude and random-phase modulation[J]. The Review of Laser Engineering, 39, 520-524(2011).

[27] Zhang J Z, Wang Y C, Wang A B. Improving performance of optical fibre chaotic communication by dispersion compensation techniques[J]. Chinese Physics B, 17, 3264-3269(2008).

[28] Sui Q, Zhang H Y, Downie J D et al. 256 Gb/s PM-16-QAM quasi-single-mode transmission over 2600 km using few-mode fiber with multi-path interference compensation[C], M3C.5(2014).

[29] VPIphotonics. VPIcomponentMaker photonic circuits user′s manual[EB/OL]. https://www.vpiphotonics.com/Tools/PhotonicCircuits

[30] Fraedrich K, Wang R S. Estimating the correlation dimension of an attractor from noisy and small datasets based on re-embedding[J]. Physica D, 65, 373-398(1993).

[31] Grassberger P, Procaccia I. Characterization of strange attractors[J]. Physical Review Letters, 50, 346-349(1983).

[32] Kim H S, Eykholt R, Salas J D. Nonlinear dynamics, delay times, and embedding windows[J]. Physica D, 127, 48-60(1999).

[33] Lin F Y, Chao Y K, Wu T C. Effective bandwidths of broadband chaotic signals[J]. IEEE Journal of Quantum Electronics, 48, 1010-1014(2012).