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

doi:10.1088/1674-1056/23/6/064207

中国物理B ›› 2014, Vol. 23 ›› Issue (6): 64207-064207.doi: 10.1088/1674-1056/23/6/064207

• ELECTROMAGNETISM, OPTICS, ACOUSTICS, HEAT TRANSFER, CLASSICAL MECHANICS, AND FLUID DYNAMICS • 上一篇下一篇

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

钟先琼^{a b}, 张晓霞^a, 程科^b, 向安平^b

a State Key Laboratory of Electronic Thin Films and Integrated Devices, School of Optoelectronic Information, University of Electronic Science and Technology of China, Chengdu 610054, China;
b College of Optoelectronic Technology, Chengdu University of Information Technology, Chengdu 610225, China

收稿日期:2013-07-18 修回日期:2013-10-30 出版日期:2014-06-15 发布日期:2014-06-15
基金资助:
Project 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), and the Major Project of the Natural Science Foundation supported by the Educational Department of Sichuan Province, China (Grant Nos. 13ZA0081 and 12ZB019).

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

Zhong Xian-Qiong (钟先琼)^{a b}, Zhang Xiao-Xia (张晓霞)^a, Cheng Ke (程科)^b, Xiang An-Ping (向安平)^b

a State Key Laboratory of Electronic Thin Films and Integrated Devices, School of Optoelectronic Information, University of Electronic Science and Technology of China, Chengdu 610054, China;
b College of Optoelectronic Technology, Chengdu University of Information Technology, Chengdu 610225, China

Received:2013-07-18 Revised:2013-10-30 Online:2014-06-15 Published:2014-06-15
Contact: Zhong Xian-Qiong E-mail:zxqlxh@yeah.net
Supported by:
Project 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), and the Major Project of the Natural Science Foundation supported by the Educational Department of Sichuan Province, China (Grant Nos. 13ZA0081 and 12ZB019).

摘要/Abstract

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.

关键词: optical wave breaking, third-order dispersion, quintic nonlinearity

Abstract: 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.

Key words: optical wave breaking, third-order dispersion, quintic nonlinearity

中图分类号: (Ultrafast processes; optical pulse generation and pulse compression)

42.65.Re

42.65.Sf (Dynamics of nonlinear optical systems; optical instabilities, optical chaos and complexity, and optical spatio-temporal dynamics) 42.70.Nq (Other nonlinear optical materials; photorefractive and semiconductor materials)

钟先琼, 张晓霞, 程科, 向安平. Ultrashort pulse breaking in optical fiber with third-order dispersion and quintic nonlinearity[J]. 中国物理B, 2014, 23(6): 64207-064207.

Zhong Xian-Qiong (钟先琼), Zhang Xiao-Xia (张晓霞), Cheng Ke (程科), Xiang An-Ping (向安平). Ultrashort pulse breaking in optical fiber with third-order dispersion and quintic nonlinearity[J]. Chin. Phys. B, 2014, 23(6): 64207-064207.

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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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