Chinese Journal of Lasers, Volume. 48, Issue 20, 2006001(2021)
Arbitrary Waveform Generation Based on Simple Design of Linearly Chirped Fiber Bragg Grating and Frequency-to-Time Mapping
Fig. 1. Schematic diagrams of the proposed arbitrary waveform generation system using a linearly chirped fiber Bragg grating
Fig. 2. Refractive index modulation and reflection spectra of grating varying with refractive index modulation scaling factor M1 when Rmax is set to be 0.9 or 0.95. (a) (c) Index modulations; (b) (d) reflection spectra
Fig. 3. Influence of normalized spectral position of refractive index modulated vertex M2 on design error. (a) Index modulations; (b) reflection spectra
Fig. 4. Simulation results with different normalized spectral position of refractive index modulated vertex M2. (a)(c) Index modulations; (b)(d) reflection spectra
Fig. 5. Simulation results with different grating lengths (L=1,2,3,4,5 cm). (a) Index modulations; (b) reflection spectra
Fig. 6. Simulation results with different chirp coefficients (C=0.4,0.5,0.6,0.7,0.8 nm/cm ). (a) Index modulations; (b) reflection spectra
Fig. 7. Simulation results with different index modulation errors. (a) Index modulations; (b) reflection spectra
Fig. 8. Simulation results with different CFBG period errors. (a) Chirp coefficients; (b) reflection spectra
Fig. 9. Simulation results of the CFBGs with trapezoidal-shaped spectra and rectangular-shaped spectra. (a) Index modulation for M2=1/3; (b) corresponding reflection spectrum for M2=1/3; (c) index modulations for M2=0, 1/20, 1/10, 1/5, and 2/5; (d) corresponding reflection spectra for M2=0, 1/20, 1/10, 1/5, and 2/5
Fig. 10. Simulation results of the CFBG with Gaussian-shaped spectrum. (a) Index modulation; (b) reflection spectrum
Fig. 11. Simulation results of the CFBG with parabolic-shaped spectrum. (a) Index modulation; (b) reflection spectrum
Fig. 13. Simulation results of grating reflection spectra and time-domain pulses after frequency-to-time mapping under different number of segments W. (a) Triangular-shaped spectrum with W=100; (b) triangular pulses with W=100; (c) triangular-shaped spectrum with W=500; (d) triangular pulses with W=500
Fig. 14. Simulated reflection spectra with different shapes and the corresponding output pulses. (a)(c)(e)(g)(i) Designed reflection spectra; (b)(d)(f)(h)(j) output pulses after frequency-to-time mapping (black dashed lines are ideal pulses)
Fig. 15. Simulation results with different grating lengths and pulse repetition rates. (a)(b) Parabolic-shaped pulse sequence after frequency-to-time mapping for grating length L=2.5 cm and 8 cm, respectively; (c)(d) parabolic-shaped pulse sequence after frequency-to-time mapping for repetition rate of 0.5 GHz and 2 GHz, respectively (black dashed lines are ideal pulses)
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Min Li, Hongqian Mu, Muguang Wang, Xinhang Wei, Xiangshuai Guan. Arbitrary Waveform Generation Based on Simple Design of Linearly Chirped Fiber Bragg Grating and Frequency-to-Time Mapping[J]. Chinese Journal of Lasers, 2021, 48(20): 2006001
Category: fiber optics and optical communications
Received: Jan. 4, 2021
Accepted: Mar. 12, 2021
Published Online: Oct. 12, 2021
The Author Email: Mu Hongqian (hongqianmu@bjtu.edu.cn)