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Cited by 548

The DOI matches its Crossref record; 24 of the 24 references it cites were found in a registry or an index.

Origins and control of polarization effects in single-mode fibers

Rashleigh, S.·1983·Journal of Lightwave Technology

Abstract

The polarization state of light in single-mode fibers is very sensitive to any perturbation which is not symmetric about the fiber axis. While this is a source of noise, drift, or signal fading in some applications, it can also be exploited in novel guided-wave devices. The basic birefringences that couple the two modes and change the polarization state along the fiber are reviewed. The three cases of uniform, phase-matched, and random coupling are considered. Polarization preservation in both low- and high-birefringence fibers is achieved by reducing this coupling. In addition to polarization-state changes, bireftingent fibers can quickly reduce the polarization degree of nonmonochromatic light if both modes are excited, a characteristic that greatly simplifies evaluation of the degree of polarization preservation in these fibers. Current evaluations of the birefringence and the polarization-holding ability of state-of-the-art fibers are discussed, and it is concluded that fibers with good polarization-holding properties are becoming available.

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Crossref · 10.1109/jlt.1983.1072121

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Metadata

Authors
Rashleigh, S.
Venue
Journal of Lightwave Technology
Published
1983
Volume
1
Issue
2
Pages
312-331
ISSN
0733-8724 (ISSN-L)
OpenAlex
W2003508608
Cited by
548
References
24
FWCI
22.23
Type
journal article
Language
en
Open access
closed

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CoChat. (2026). Citation check: Origins and control of polarization effects in single-mode fibers. https://app.cochat.ai/papers/10.1109/jlt.1983.1072121
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Rashleigh, S. (1983). Origins and control of polarization effects in single-mode fibers. Journal of Lightwave Technology. https://doi.org/10.1109/jlt.1983.1072121

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Contains information from the Semantic Scholar Academic Graph Datasets, made available under the ODC Attribution License (ODC-BY 1.0).

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