2016
DOI: 10.1364/ol.41.004927
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Polarization evolution of vector wave amplitudes in twisted fibers pumped by single and paired pulses

Abstract: Nonlinear polarization dynamics of single and paired pulses in twisted fibers is experimentally and numerically studied. Accompanying a dramatic difference in the output spectrum when a single- or double-amplified soliton pulse is launched in the fiber, the output polarization for the two cases also reveals very different characteristics.

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Cited by 12 publications
(5 citation statements)
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“…Hence, nonlinear effects integrate over much longer lengths of fibre, allowing SC generation even in fibres whose nonlinear and dispersive properties are not optimized for this purpose, as it will be observed in the present work. Spectral broadening in such media could also be strongly enhanced by the nonlinear interaction between the NLP components (inner sub-pulses); although the underlying physical mechanisms are not clear at this stage, the effects of pulse interaction were illustrated in a recent experimental work [22], in which the spectrum produced by a pair of pulses after travelling through a segment of conventional fibre was much broader than a single pulse. Another advantage of NLPs is a high energy per pulse, up to 100s of nJ (~1000 times that of a soliton) [23][24][25], because a NLP is not a simple pulse but a large bunch of radiation.…”
Section: Introductionmentioning
confidence: 99%
“…Hence, nonlinear effects integrate over much longer lengths of fibre, allowing SC generation even in fibres whose nonlinear and dispersive properties are not optimized for this purpose, as it will be observed in the present work. Spectral broadening in such media could also be strongly enhanced by the nonlinear interaction between the NLP components (inner sub-pulses); although the underlying physical mechanisms are not clear at this stage, the effects of pulse interaction were illustrated in a recent experimental work [22], in which the spectrum produced by a pair of pulses after travelling through a segment of conventional fibre was much broader than a single pulse. Another advantage of NLPs is a high energy per pulse, up to 100s of nJ (~1000 times that of a soliton) [23][24][25], because a NLP is not a simple pulse but a large bunch of radiation.…”
Section: Introductionmentioning
confidence: 99%
“…A delay line is used as a non-linear and dispersive media where the non-linear and dispersive effects interact to generate different types of dynamics in the function of different parameters as the nonlinearity, dispersion, length, pump power, and polarization of the light [17]. To ensure the total polarization control in the cavity, and therefore the NPR effect, the delay line is commonly a twist conventional SMF fiber [19]. The twisted fiber in the cavity is used to maintain constant ellipticity during propagation.…”
Section: Theoretical Modelmentioning
confidence: 99%
“…Twisted fibre operates in a way similar to an isotropic fibre [50], although it also introduces circular birefringence (thus causing a rotation of the ellipse) and a group velocity mismatch between circular right and left polarization components. This mismatch is small however, ranging as ~0.3 fs m −1 for a twist rate of 5 turns m −1 [51,52]. The same value for the nonlinear Kerr coefficient, γ = 1.5/W/ km (corre sponding to standard telecom fibre), is taken for all sections of fibre.…”
Section: Laser Setup and Numerical Modelmentioning
confidence: 99%