1996
DOI: 10.1006/ofte.1996.0033
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Impact of First- and Second-Order PMD in Optical Digital Transmission Systems

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Cited by 144 publications
(34 citation statements)
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“…As shown in the table, large dispersion as -40 ps/nm/km was realized with IDF-40, but A eff was 21μm 2 and attenuation loss became 0.26 dB/km. PMD also became larger and it also strictly limits transmission performance [27,28]. As aforementioned, the dispersion enlargement of IDF, which can be realized by changing a Δ1 value of a w-shaped profile, is advantageous for low nonlinear property in a total line, but it generally sacrifices A eff , loss and PMD properties.…”
Section: Dispersion Enlargement With Idfmentioning
confidence: 97%
“…As shown in the table, large dispersion as -40 ps/nm/km was realized with IDF-40, but A eff was 21μm 2 and attenuation loss became 0.26 dB/km. PMD also became larger and it also strictly limits transmission performance [27,28]. As aforementioned, the dispersion enlargement of IDF, which can be realized by changing a Δ1 value of a w-shaped profile, is advantageous for low nonlinear property in a total line, but it generally sacrifices A eff , loss and PMD properties.…”
Section: Dispersion Enlargement With Idfmentioning
confidence: 97%
“…The input field of birefringent segments is represented by Ein(t) = Ein(t)jin, where jin is the input Jones polarization vector which depends on the azimuth and the ellipticity of the input SOP. The output field is given by [7], [8] …”
Section: Wave Propagation In Optical Fibers In the Presence Of Pmdmentioning
confidence: 99%
“…where (ω)D(ω)R(ω), where R(ω) takes into account the rotation of PSPs, and the dispersive matrix D(ω) takes into account the different propagation speeds on the two PSPs [7], [8].…”
Section: Wave Propagation In Optical Fibers In the Presence Of Pmdmentioning
confidence: 99%
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