2015
DOI: 10.1364/oe.23.003914
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Linear compression of chirped pulses in optical fibre with large step-index mode area

Abstract: The possibilities and limitations of linear compression of positively chirped pulses in the negative-dispersion region of a step-index large mode-area single-mode optical fibre are investigated for the first time. Analytical formulae for critical values of radiation power are found, below which pedestal-free pulse compression is possible down to the Fourier limit. It is demonstrated that at radiation powers exceeding these critical values, there exists an optimal compressing fibre length, over which laser puls… Show more

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Cited by 19 publications
(9 citation statements)
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“…Conversely, double-scale pulses present very limited possibilities of compression [24]. It has to be stressed that these limitations arise from the structure of the pulses themselves rather than from non-linear effects in fibre-optical compressors, which may also constrain compression coefficient of 'regular' laser pulses at sufficiently high-peak-power values [28].…”
Section: Pulse Compressionmentioning
confidence: 99%
“…Conversely, double-scale pulses present very limited possibilities of compression [24]. It has to be stressed that these limitations arise from the structure of the pulses themselves rather than from non-linear effects in fibre-optical compressors, which may also constrain compression coefficient of 'regular' laser pulses at sufficiently high-peak-power values [28].…”
Section: Pulse Compressionmentioning
confidence: 99%
“…LMA fibers can also be utilized in the latter part i.e. as a pulse compressor in an all-fiber CPA system since the chirped pulse propagation in an optical fiber engenders decrement in the temporal width of the pulse in the negative dispersion (anomalous) regime [5].…”
Section: Introductionmentioning
confidence: 99%
“…Frequently, temporally short pulses are realized with linear dispersion [8] or nonlinear dispersion [9] compression using external dispersive elements that have large chromatic dispersion. This function might be performed by a variety of photonic components such as gratings [10], prisms [11], chirped-mirrors [12] and gas-filled hollow-core fibers [13]. Nevertheless, they lack tunability, which is crucial for communication applications, and may be difficult to integrate with commercial systems.…”
Section: Introductionmentioning
confidence: 99%