1988
DOI: 10.1109/3.135
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Optical pulse compression using high-frequency electrooptic phase modulation

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Cited by 161 publications
(69 citation statements)
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“…Relative phases of the lines are measured for lines (-6 to 5}. Lines (I, 0, -3, and -5} are 71 out of phase with the rest, which agree with calculation using a Bessel series [8]. Fig.…”
Section: B Experimental Resultssupporting
confidence: 59%
“…Relative phases of the lines are measured for lines (-6 to 5}. Lines (I, 0, -3, and -5} are 71 out of phase with the rest, which agree with calculation using a Bessel series [8]. Fig.…”
Section: B Experimental Resultssupporting
confidence: 59%
“…The CW light emitted from an external cavity laser (ECL) operating at 1080 nm was coupled into a LiNbO 3 phase modulator (PM) and a 10 GHz sinusoidal phase modulation was applied to the CW light. The sinusoidally phase-modulated light can be converted into an optical pulse train by applying group delay dispersion (GVD) to the light [4,5]. As a GVD device, we used a linearly chirped fiber Bragg grating (CFBG) with a −1 dB bandwidth of 20 nm and a dispersion parameter D of 60 ps/nm.…”
Section: Introductionmentioning
confidence: 99%
“…2 shows the setup used for PE measurements. The pulse source consists of a continuous wave (CW) laser centered at 1548.32 nm, a Mach-Zehnder modulator (MZM) used to carve 50% duty cycle pulses, and a phase modulator (PM) followed by a length of standard single mode fibre (SMF) for pulse compression [12]. The PM is driven by a 40 GHz radio frequency (RF) signal with V pp = 2V π , where V pp is the peak-to-peak voltage of the RF signal and V π is the half-wave voltage of the PM.…”
Section: Introductionmentioning
confidence: 99%