2006
DOI: 10.1109/jlt.2006.883641
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Circular-Birefringence Fiber for Nonlinear Optical Signal Processing

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Cited by 66 publications
(29 citation statements)
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“…The polarisation states of counter-propagating beams are made different through the use of a quarter-wave retarder (QWR) inserted in the loop after one of the coupler output ports. To prevent the nonlinear polarisation evolution from averaging out for each beam, twist is applied to the fibre, which then becomes optically active and behaves like an ideal isotropic fibre [24]. Starting from the coupled nonlinear differential equations for polarisation evolution in the continuous-wave case [25], a model was proposed in [21], which enabled a thorough study of this promising device (see for example [26][27][28]).…”
Section: Article In Pressmentioning
confidence: 99%
See 1 more Smart Citation
“…The polarisation states of counter-propagating beams are made different through the use of a quarter-wave retarder (QWR) inserted in the loop after one of the coupler output ports. To prevent the nonlinear polarisation evolution from averaging out for each beam, twist is applied to the fibre, which then becomes optically active and behaves like an ideal isotropic fibre [24]. Starting from the coupled nonlinear differential equations for polarisation evolution in the continuous-wave case [25], a model was proposed in [21], which enabled a thorough study of this promising device (see for example [26][27][28]).…”
Section: Article In Pressmentioning
confidence: 99%
“…Polarisation thus only rotates by $0.05N with respect to the birefringence axes in this case, so that the averaging out of birefringence is less effective. However, considering that the radius of curvature is not too small (say, 30 cm), a moderate twist rate of 1 turn/m can be sufficient to ensure nearly circular birefringence [24]. Taking for example r ¼ 62.5 mm, l 0 ¼ 1.55 mm and R ¼ 30 cm, one finds that the product 0.05NL B E13 is still quite large.…”
Section: Numerical Analysismentioning
confidence: 99%
“…21,22 Our approximation neglects the fiber dispersion and is valid when the pulse widths are sufficiently long to yield a dispersion length longer than the fiber length. 16 The next differential equations describe the polarization states of beams propagating in a birefringent twisted fiber along the z axis in the circular polarization basis:…”
Section: Polarization Equationsmentioning
confidence: 99%
“…In this general model, during the production phase, a twisting process of the fiber generates an induced circular birefringence. This production process has the advantage of a PMD decrease [6]. Another advantage of twisted fiber is the opportunity to better exploit the multilevel polarization modulations.…”
Section: Introductionmentioning
confidence: 99%