1997
DOI: 10.1049/el:19971297
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Modelling of polarisation mode dispersion in singlemode fibres

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Cited by 35 publications
(9 citation statements)
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“…In the limit of small PMD we get b 2 unc = 1 + 2x/3 because only 2 of the 3 orthogonal directions in Stokes space causes broadening (the two orthogonal to the PSPs). This will also cause the pulse width to be Rayleigh (rather than Maxwell) distributed in this limit, as found numerically in [20] and explained theoretically in [21].…”
Section: Statistics Of Pulse Broadeningmentioning
confidence: 77%
“…In the limit of small PMD we get b 2 unc = 1 + 2x/3 because only 2 of the 3 orthogonal directions in Stokes space causes broadening (the two orthogonal to the PSPs). This will also cause the pulse width to be Rayleigh (rather than Maxwell) distributed in this limit, as found numerically in [20] and explained theoretically in [21].…”
Section: Statistics Of Pulse Broadeningmentioning
confidence: 77%
“…Both DOP and eye opening penalty (EOP) are calculated at the receiver end for system performance evaluation. A long transmission fiber can be modeled as a concatenated series of linearly birefringent segments with statistically varying group delays and orientations of the birefringence axes [13]. At every junction between two segments, the energy from each incident pulse is split into two orthogonally polarized pulses, representing the mode coupling that occurs in the fiber due to perturbations in local birefringence.…”
Section: System Setup and Modellingmentioning
confidence: 99%
“…Finally, we simulated 14 Figure 9 shows the narrowed pulse obtained for such a fiber when its mean 15 DGD equals 35 ps. In this case it was possible to obtain a sharp reduction of the pulsewidth, of 9.018 ps, at the expense of high power loss.…”
Section: Computer Simulationmentioning
confidence: 99%