2003
DOI: 10.1109/jlt.2003.819147
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Optical carrier supply module using flattened optical multicarrier generation based on sinusoidal amplitude and phase hybrid modulation

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Cited by 135 publications
(54 citation statements)
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“…The proper alignment of temporal phases in time between the modulators is critical for spectral flatness and can be achieved with phase shifters shown in the schematic. If the electric field of the input light is expressed as E in (t) = exp(iw c t), the electrical field of the output is E out (t) expressed as [13]: …”
Section: A Electro-optic Optical Frequency Comb Generatorsmentioning
confidence: 99%
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“…The proper alignment of temporal phases in time between the modulators is critical for spectral flatness and can be achieved with phase shifters shown in the schematic. If the electric field of the input light is expressed as E in (t) = exp(iw c t), the electrical field of the output is E out (t) expressed as [13]: …”
Section: A Electro-optic Optical Frequency Comb Generatorsmentioning
confidence: 99%
“…A total of 64 seed lasers were used to generate 512 carriers using two OCSMs. The work was followed by building a prototype providing, the evidence of how combs could be used in real nodes as a carrier source [13], [90]. Mao et al further investigated the crosstalk and the practical system design, using comb based carrier sources [91].…”
Section: A Electro-optic Optical Frequency Comb Generatorsmentioning
confidence: 99%
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“…Previously reported comb generation techniques include (1) the use of amplitude or frequency modulated (FM) mode-locked lasers (such as ERGO (Er:Yb:glass laser oscillator) lasers [1], fibre ring lasers [6], or mode-locked semiconductor lasers [7]), which give good optical signal-to-noise ratio (OSNR) values, but require precise control of the laser cavity length; (2) a wideband LiNbO3 phase modulator in self-oscillating mode [8] when driven with a feedback signal from its output, which makes oscillation easier to start and maintain than mode-locked lasers, but requires large RF power amplifiers with precise control of the output voltage, in addition to extra filters and photodiodes; (3) an amplitude modulator with a section of highly non-linear fibre [9], which also results in a good OSNR, but needs high optical launch powers, long fibre lengths and stimulated Brillouin scattering (SBS) suppression; and (4) concatenated Mach-Zehnder (MZ) and phase modulators [10], a method which gives good uniformity across the channels, but requires the use of large drive voltage amplifiers and precise control of the applied voltage. Techniques (1) and (2) generally require an appropriately shaped optical filter to produce reasonable flatness, whilst (3) produces a large number of unwanted comb lines; in each of these cases the power efficiency of the comb is reduced.…”
Section: Introductionmentioning
confidence: 99%
“…We mention, e.g., the optimization of dual-drive MachZehnder modulators [4,5]; concatenation of two electrooptic modulators [6,7]; or mixing of two sinusoidal RF signals in a single electro-optic phase modulator (EOPM) [8]. In these schemes, the spectral flatness is achieved by an accurate optimization of the physical parameters of the modulators, i.e., modulation indexes, bias voltages, and phase shifters.…”
mentioning
confidence: 99%