2005
DOI: 10.1364/ol.30.001231
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Ultralow-noise mode-locked laser with coupled optoelectronic oscillator configuration

Abstract: We describe simultaneous generation of ultralow-noise optical pulses and microwave signal with a mode-locked fiber laser in a coupled optoelectronic oscillator configuration. We demonstrate 9.2-GHz optical and microwave signals with the measured phase noise of -140 dBc/Hz at 10-kHz offset frequency. We show that the mode-locked laser in the photonic oscillator serves as a high-Q filter and is responsible for the observed low phase noise.

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Cited by 77 publications
(24 citation statements)
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“…Some of them involve multiple loops in order to suppress the spurious peaks [5], [6]. Others lock the oscillator to atomic resonances [7], or enhance the functionalities of the optical branch to improve the phase noise figure [8], the tunability of the oscillator [9], or to mode-lock the optical modes [10], [11] for ultralow jitter pulse generation.…”
Section: Introductionmentioning
confidence: 99%
“…Some of them involve multiple loops in order to suppress the spurious peaks [5], [6]. Others lock the oscillator to atomic resonances [7], or enhance the functionalities of the optical branch to improve the phase noise figure [8], the tunability of the oscillator [9], or to mode-lock the optical modes [10], [11] for ultralow jitter pulse generation.…”
Section: Introductionmentioning
confidence: 99%
“…The pulse repetition rate is determined by the frequency of the OEO and the timing jitter of the optical pulses matches closely to the low phase noise of the RF signal generated by the OEO. A demonstration of the C-OEO showed the phase noise of the optical pulses is −140 dBc/Hz at 10 kHz offset [48].…”
Section: Optical Pulse Generation Oeomentioning
confidence: 99%
“…The additional phase shift introduced in the resonant loop by components such as amplifiers and transmission lines causes the phase self-locking behavior of the circuit to resonate at a different frequency. 29 The round-trip phase shift at the resonant frequency must be a multiple of 2π radians to satisfy the Barkhausen oscillation condition. 30 Depending on the phase shift, this may result in a stable f dyn of greater or less than f stat .…”
Section: B Dynamic Resonant Frequency (F Dyn )mentioning
confidence: 99%