2021
DOI: 10.1109/lpt.2021.3112485
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Roll-Off Factor Analysis of Optical Nyquist Pulses Generated by an On-Chip Mach-Zehnder Modulator

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Cited by 11 publications
(9 citation statements)
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“…The intensity transfer function of the simulation is different from that in the experiment because of insufficiencies in the fabrication process. At 1.2 V DC bias, a modulation depth of around -12 dB was obtained, and working at this low modulation depth will increase the effect of the higher order sidebands and hence the quality of the sampling [26] [27]. For sampling, the LD with an input power of 0 dBm was adjusted to the resonance point of the ring modulator (1553.43 nm).…”
Section: A Simulation Resultsmentioning
confidence: 99%
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“…The intensity transfer function of the simulation is different from that in the experiment because of insufficiencies in the fabrication process. At 1.2 V DC bias, a modulation depth of around -12 dB was obtained, and working at this low modulation depth will increase the effect of the higher order sidebands and hence the quality of the sampling [26] [27]. For sampling, the LD with an input power of 0 dBm was adjusted to the resonance point of the ring modulator (1553.43 nm).…”
Section: A Simulation Resultsmentioning
confidence: 99%
“…A bias of 0.95 V would result in a higher bandwidth of 1 GHz but also in a low modulation depth of 5 dB, since there is a tradeoff between the bandwidth and modulation depth [28]. Working at lower modulation depths would increase the sideband power and affects the flatness of the frequency comb, which would result in lower quality sampling [26] [27].…”
Section: B Experimental Resultsmentioning
confidence: 99%
“…In the past decade, many methods for generating Nyquist pulses have been reported, such as digital signal processing [10], spectral filtering shaper [11], and optical parametric amplifier [12]. Recently, direct synthesizing Nyquist pulses of exceptional quality using optical frequency comb (OFC) modulated by electro-optic modulators (EOMs) has been proposed [13], [14], [15], [16], [17], [18], [19], [20]. The pulse repetition rate is determined by the frequency interval f m between adjacent spectral lines of OFC and the zero-crossing pulse duration τ r is τ r = 2/(N • f m )(N is the number of spectral lines of OFC).…”
Section: Introductionmentioning
confidence: 99%
“…Nyquist pulse by increasing the number of spectral lines N because the limited f m decided by the bandwidth of the modulator used. A single Mach-Zehnder modulator (MZM) [13] or a single dual-parallel Mach-Zehnder modulator (DPMZM) [14] could achieve up to 3 or 5 flat spectral lines and the corresponding Nyquist pulse duration is about 100 ps. Two cascaded MZMs were proposed in [1], [15], [16], while the number of generated spectral lines is still no more than 9, resulting in a pulse duration of minimum 12.8 ps.…”
Section: Introductionmentioning
confidence: 99%
“…The most popular design satisfying the above mentioned requirements is the socalled raised-cosine (RC) pulse [3], which has been widely employed in numerous practical digital communications systems, e.g. see [5], [6], [7], [8], [9], [10], and [11] and references therein.…”
Section: Introductionmentioning
confidence: 99%