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Ultrashort pulse breaking in optical fiber with third-order dispersion and quintic nonlinearity

Ultrashort pulse breaking in optical fiber with third-order dispersion and quintic nonlinearity
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摘要 The optical wave breaking (OWB) characteristics in terms of the pulse shape, spectrum, and frequency chirp, in the normal dispersion regime of an optical fiber with both the third-order dispersion (TOD) and quintic nonlinearity (QN) are numerically calculated. The results show that the TOD causes the asymmetry of the temporal- and spectral-domain, and the chirp characteristics. The OWB generally appears near the pulse center and at the trailing edge of the pulse, instead of at the two edges of the pulse symmetrically in the case of no TOD. With the increase of distance, the relation of OWB to the TOD near the pulse center increases quickly, leading to the generation of ultra-short pulse trains, while the OWB resulting from the case of no TOD at the trailing edge of the pulse disappears gradually. In addition, the positive (negative) QN enhances (weakens) the chirp amount and the fine structures, thereby inducing the OWB phenomena to appear earlier (later). Thus, the TOD and the positive (negative) QN are beneficial (detrimental) to the OWB and the generation of ultra-short pulse trains. The optical wave breaking (OWB) characteristics in terms of the pulse shape, spectrum, and frequency chirp, in the normal dispersion regime of an optical fiber with both the third-order dispersion (TOD) and quintic nonlinearity (QN) are numerically calculated. The results show that the TOD causes the asymmetry of the temporal- and spectral-domain, and the chirp characteristics. The OWB generally appears near the pulse center and at the trailing edge of the pulse, instead of at the two edges of the pulse symmetrically in the case of no TOD. With the increase of distance, the relation of OWB to the TOD near the pulse center increases quickly, leading to the generation of ultra-short pulse trains, while the OWB resulting from the case of no TOD at the trailing edge of the pulse disappears gradually. In addition, the positive (negative) QN enhances (weakens) the chirp amount and the fine structures, thereby inducing the OWB phenomena to appear earlier (later). Thus, the TOD and the positive (negative) QN are beneficial (detrimental) to the OWB and the generation of ultra-short pulse trains.
出处 《Chinese Physics B》 SCIE EI CAS CSCD 2014年第6期239-245,共7页 中国物理B(英文版)
基金 supported by the Postdoctoral Fund of China(Grant No.2011M501402) the National Natural Science Foundation of China(Grant No.61275039) the 973 Program of China(Grant No.2012CB315702) the Key Project of the Chinese Ministry of Education,China(Grant No.210186) the Major Project of the Natural Science Foundation supported by the Educational Department of Sichuan Province,China(Grant Nos.13ZA0081 and 12ZB019)
关键词 optical wave breaking third-order dispersion quintic nonlinearity optical wave breaking, third-order dispersion, quintic nonlinearity
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