Abstract
In this paper, the Sasa-Satsuma equation in fluid dynamics and nonlinear optics is investigated. Starting from the first-order Darboux transformation, we construct an N-fold generalized Darboux transformation (GDT), where N is a positive integer. Through the obtained N-fold GDT, we derive three kinds of the semirational solutions, which describe the second-order degenerate solitons, third-order degenerate solitons and interaction between the second-order degenerate solitons and one soliton, respectively. We graphically illustrate the above three kinds of semirational solutions and investigate them through the asymptotic analysis, from which we find that the characteristic lines of the semirational solutions are composed of the straight lines and curves. Expressions of the characteristic lines, positions, amplitudes, slopes, positions and phase shifts of the asymptotic solitons are presented through the asymptotic analysis. The above discussions might be extended to the higher-order solitons, and to the relevant analysis on the degenerate breathers.
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Acknowledgements
This work was supported by the National Natural Science Foundation of China under Grant No. 11772017 and by the Fundamental Research Funds for the Central Universities.
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Appendix
Appendix
When considering the linear pulses in an optical transmission system, dispersion character of the fiber material has been considered to limit the maximum value of the bit rate of transmission (i.e., channel capacity of an optical fiber) [35]. To overcome this limitation, the nonlinear change of dielectric (the so-called Kerr effect) of the fiber has been used to compensate for the dispersion effect [35]. Afterward, the researchers have analyzed an optical pulse propagating through a cylindrical fiber with the Kerr effect [35, 36]. Starting from the three-dimensional vector Maxwell equation for the electric field in a fiber with an inhomogeneous dielectric constant, the researchers have derived the one-dimensional scalar perturbation nonlinear Schrödinger in an appropriate asymptotic sense, i.e.,
where the meanings of the variables are offered in Refs. [35, 36]. In fact, the derivation process details in Refs. [35, 36] have been shown to be really complicated. On the basis of Eq. (28), the feasibility of a long-distance-high-bit-rate optical transmission system by the use of solitons has been discussed [35].
Actually, when \(\alpha _1=\alpha _2=\alpha _3=0\), Eq. (28) has been reduced to the NLS equation [1]. That is to say, Eq. (28) has been considered as the result of adding higher-order terms to the NLS equation [17]. As the real parameters \(\alpha _1,~\alpha _2\) and \(\alpha _3\) satisfy certain conditions, e.g., \(\alpha _1:\alpha _2:\alpha _3=0:1:1\), \(\alpha _1:\alpha _2:\alpha _3=0:1:0\) and \(\alpha _1:\alpha _2:\alpha _3=1:6:0\), Eq. (28) has been shown to be integrable and solvable through the inverse scattering transform scheme [6].
Later, under the condition \(\alpha _1:\alpha _2:\alpha _3=1:6:3\), the Sasa–Satsuma equation has been derived [6]. With the higher-order nonlinear terms concluded, the Sasa–Satsuma equation has been considered to have the applications as follows:
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Amplitude modulations of the fundamental harmonic of Stokes waves on the surface of a medium- and large-depth (compared to the wavelength) fluid layer [37].
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Gravity surface waves in the finite-depth water by assuming small wave steepness, narrow-band spectrum, and small depth as compared to the modulation length [38].
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A train of the femtosecond pulses with repetition rates of a few terahertz in the nonlinear optical fibers [39, 40].
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Propagation of the short optical pulses through a dispersive media with a cubic self-focusing nonlinear polarization, which incorporates the self-steepening and self-frequency shifting [41].
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Other relevant symbolic-computation studies have been reported, e.g., in Refs. [42,43,44,45,46,47,48,49,50,51,52].
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Wu, XH., Gao, YT., Yu, X. et al. N-fold generalized Darboux transformation and asymptotic analysis of the degenerate solitons for the Sasa-Satsuma equation in fluid dynamics and nonlinear optics. Nonlinear Dyn 111, 16339–16352 (2023). https://doi.org/10.1007/s11071-023-08533-4
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DOI: https://doi.org/10.1007/s11071-023-08533-4