2020
DOI: 10.1016/j.ijleo.2019.164134
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Modulation instabilities in nonlinear two-core optical fibers with fourth order dispersion

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Cited by 7 publications
(11 citation statements)
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“…After the mergence, another new MI band arises, however, the gain of this band is relatively very weak. The MI evolution is similar with the symmetric CW and the antisymmetric CW states as shown by figures 2, 8 and 12 in [81] in terms that new MI bands can be generated in the high frequency. The main difference is that two new MI bands are always present for the asymemtric CW state, in contrast with the situation for the symmetric and antisymmetric CW states that only one new MI band can be generated.…”
supporting
confidence: 65%
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“…After the mergence, another new MI band arises, however, the gain of this band is relatively very weak. The MI evolution is similar with the symmetric CW and the antisymmetric CW states as shown by figures 2, 8 and 12 in [81] in terms that new MI bands can be generated in the high frequency. The main difference is that two new MI bands are always present for the asymemtric CW state, in contrast with the situation for the symmetric and antisymmetric CW states that only one new MI band can be generated.…”
supporting
confidence: 65%
“…In conclusion, for the anomalous dispersion, in comparison with the FOD behaviors for the symmetric and antisymmetric CW states in [80,81], the main similarity is that new MI band(s) in the high frequency can be generated; the main difference is that FOD can generate two new MI bands at a given total power for the asymemtric CW state, which can never merge with the original MI band, in constrast to the situation for the symmetric and antisymmetric CW states that only one new MI band in the high frequency is generated, and can merge with the orignal MI band. Now, we consider the normal dispersion.…”
mentioning
confidence: 88%
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