2001
DOI: 10.1364/josab.18.000919
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Theory of nonlinear loop mirrors with twisted low-birefringence fiber

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Cited by 72 publications
(50 citation statements)
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“…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%
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“…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%
“…͑1͒ and ͑2͒, into the often used eigenmode polarization basis. 16 We transform complex amplitudes C + and C − into polarization eigenmodes S + and S − .…”
Section: Polarization Equationsmentioning
confidence: 99%
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“…Still, fibre birefringence and polarisation evolution modify the NOLM operation, and a few groups tried to figure out how it happens. Some of the first studies of polarisation effects in NOLMs can be found in [19,20], but a comprehensive study of polarisation effects in NOLMs [21] would follow by more than a decade the funding paper by Doran et al [1]. In [22], the first thorough study of the impairments imposed by residual birefringence on the NOLM operation was presented.…”
Section: Introductionmentioning
confidence: 99%