Author Affiliations
1College of Information and Navigation, Air Force Engineering University, Xi’an 710077, China2Chongqing Optoelectronics Research Institute, Chongqing 400060, Chinashow less
Fig. 1. Configuration of the proposed approach for the generation of switchable multi-format linearly chirped signals. LD, laser diode; PC, polarization controller; DDMZM, dual-drive Mach–Zehnder modulator; PD, photodetector; EBPF, electrical bandpass filter; OSC, oscilloscope.
Fig. 2. Electrical spectra, time-domain waveform, frequency-time diagram, and recovered data of the generated linearly chirped signal with (a)–(d) FSK and (e)–(h) PSK formats. The coherent demodulation in (d) is, respectively, conducted by an LO with a frequency of 125–175 MHz (Demod.1) and 250–350 MHz (Demod.2).
Fig. 3. (a) Time-domain waveform, (b) electrical spectrum, (c), (d) frequency-time diagram, and (e), (f) recovered data of the generated dual-band linearly chirped signal with PSK format.
Fig. 4. (a) Time-domain waveform, (b) electrical spectrum, (c) frequency-time diagram, and (d) recovered data of the generated linearly chirped signal with the FSK/PSK format. The coherent demodulation is, respectively, conducted by an LO with a frequency of 125–175 MHz (Demod.1) and 250–350 MHz (Demod.2).
Fig. 5. (a) Electrical spectra without filtering. The green number n means the nth-order harmonic, and the red line depicts the amplitude response sketch of the EBPF. (b) The frequency-time diagram of the generated 5 Mbit/s 250–300/375–450 MHz FSK modulated linearly chirped signal.
Fig. 6. (a) Frequency-time diagram obtained by Hilbert transform in simulation. (b) The frequency-time diagram of the generated 100 Mbit/s 5–7/10–14 GHz FSK modulated linearly chirped signal with interference components.
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0 | J2(m) cos(2ωt + 2πkt2) | | J1(m) sin(ωt + πkt2) | | −J2(m) cos(2ωt + 2πkt2) | | −J1(m) sin(ωt + πkt2) | | J1(m) sin(ωt + πkt2) + J2(m) cos(2ωt + 2πkt2) | | J1(m) sin(ωt + πkt2) − J2(m) cos(2ωt + 2πkt2) | | −J1(m) sin(ωt + πkt2) + J2(m) cos(2ωt + 2πkt2) | | −J1(m) sin(ωt + πkt2) − J2(m) cos(2ωt + 2πkt2) |
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Table 1. The Results of i2(t) Corresponding to Specific θ(t)