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本文研究了四阶色散非线性薛定谔方程的明暗孤立波和怪波的形成机制, 该模型既可以模拟高速光纤传输系统中超短脉冲的非线性传输和相互作用, 又可以描述具有八极与偶极相互作用的一维海森堡铁磁链的非线性自旋激发现象. 本文首先通过对四阶色散非线性薛定谔方程的相平面分析, 发现由其约化得到的二维平面自治系统具有同宿轨道和异宿轨道, 并在相应条件下求得了方程的明孤立波解和暗孤立波解, 从而揭示了同异宿轨道和孤立波解的对应关系; 其次, 基于非零背景平面上的精确一阶呼吸子解, 给出了呼吸子的群速度和相速度的显式表达式, 进而分析得出呼吸子的速度存在跳跃现象. 最后, 为了验证在跳跃点处呼吸子可以转化为怪波, 将呼吸子解在速度跳跃条件下取极限获得了一阶怪波解, 从而证实怪波的产生与呼吸子速度的不连续性有关.In this paper, we study the generation mechanism of bright and dark solitary waves and rogue wave for the fourth-order dispersive nonlinear Schrödinger (FODNLS) equation, which can not only model the nonlinear propagation and interaction of ultrashort pulses in the high-speed optical fiber transmission system, but also govern the nonlinear spin excitations in the onedimensional isotropic biquadratic Heisenberg ferromagnetic spin with the octupole-dipole interaction. Firstly, via the phase plane analysis, we obtain both the homoclinic and heteroclinic orbits for the two-dimensional plane autonomous system reduced from the FODNLS equation. Further, we derive the bright and dark solitary wave solutions under the corresponding conditions, which reveals the relationship between the homoclinic (heteroclinic) orbit and solitary wave. Secondly, based on the exact first-order breather solution of the FODNLS equation over a nonvanishing background, we give the explicit expressions of group and phase velocities, and reveal that there exists a jump in both the velocities. Finally, in order to verify that the breather becomes a rogue wave at the jumping point, we obtain the first-order rogue wave solution by taking the limit of the breather solution at such point, which confirms the relationship of the generation of rogue wave with the velocity discontinuity.
[1] He J S, Xu S W, Porsezian 2012 Phys. Rev. E 86 066603Google Scholar
[2] Bludov Y V, Konotop V V, Akhmediev N 2009 Phys. Rev. A 80 033610Google Scholar
[3] Stenflo L, Marklund M 2010 J. Plasma Phys. 76 293Google Scholar
[4] Li M, Shui J J, Xu T 2018 Appl. Math. Lett. 83 110Google Scholar
[5] Li M, Shui J J, Huang Y H, Wang L, Li H J 2018 Phys. Scr. 93 115203Google Scholar
[6] Li M, Xu T, Meng D X 2016 J. Phys. Soc. Jpn. 85 124001Google Scholar
[7] Xu T, Lan S, Li M, Li L L, Zhang G W 2019 Physica D 390 47Google Scholar
[8] Xu T, Pelinovsky D E 2019 Phys. Lett. A 383 125948 ; Xu T, Chen Y, Li M, Meng D X 2019 Chaos 29 123124
[9] Agrawal G P 2012 Nonlinear Fiber Optics (5th ed.) (San Diego: Academic Press) pp120–150
[10] Ma Y C 1979 Stud. Appl. Math. 60 43Google Scholar
[11] Akhmediev N N, Korneev V I 1986 Theor. Math. Phys. 69 1089Google Scholar
[12] Calini A, Schober C M 2002 Phys. Lett. A 298 335Google Scholar
[13] Wang L, Zhang J H, Wang Z Q, Liu C, Li M, Qi F H, Guo R 2016 Phys. Rev. E 93 012214Google Scholar
[14] Akhmediev N N, Soto-Crespo J M, Ankiewica A 2009 Phys. Lett. A 373 2137Google Scholar
[15] Zuo D W, Gao Y T, Xue L, Feng Y J 2014 Chaos, Solitons Fractals 69 217227
[16] Solli D R, Ropers C, Koonath P, Jalali B 2007 Nature 450 1054Google Scholar
[17] Chabchoub A, Hoffmann N P, Akhmediev N 2011 Phys. Rev. E 106 204502
[18] Peregrine D H 1983 J. Austral. Math. Soc. Ser. B 25 16Google Scholar
[19] Akhmediev N N, Soto-Crespo J M, Ankiewica A 2009 Phys. Rev. A 80 043818Google Scholar
[20] Benjamin T B, Feir J E 1967 J. Fluid. Mech. 27 417Google Scholar
[21] Toffoli T, Fernandez L, Monbaliu J, Benoit M, Gagnaire-Renou E, Lefèvre J M, Cavaleri L, Proment D, Pakozdi C, Stansberg C T, Waseda T, Onorato M 2013 Phys. Fluids 25 091701Google Scholar
[22] Mussot A, Kudlinski A, Kolobov M, Louvergneaux E, Douay M, Taki M 2009 Opt. Express 17 17010Google Scholar
[23] Genty G, de Sterke C M, Bang O, Dias F, Akhmediev N, Dudley J M 2010 Phys. Lett. A 374 989Google Scholar
[24] He J S, Xu S W, Porsezian K, Cheng Y, Dinda P T 2016 Phys. Rev. E 93 062201Google Scholar
[25] He J S, Xu S W, Porsezian K, Dinda P T, Mihalache D, Malomed B A, Ding E 2017 Rom. J. Phys. 62 203
[26] Liu S D, Liu S K 1994 Soliton Wave and Turbulence (Chinese version) (1st ed.) (Shanghai: Shanghai Scientific and Technological Education Press) pp90–97
[27] Infeld E, Rowlands G 2000 Nonlinear Waves, Solitons and Chaos (2th ed.) (Cambridge: Cambridge University Press) pp144–156
[28] Choudhuri A, Porsezian K 2013 Phys. Rev. A 88 033808Google Scholar
[29] Porsezian K, Daniel M, Lakshmanan M 1992 J. Math. Phys. 33 1807Google Scholar
[30] Wang L H, Porsezian K, He J S 2013 Phys. Rev. E 87 053202Google Scholar
[31] Azzouzi F, Triki H, Mezghiche K, Akrmi A E 2009 Chaos, Solitons Fractals 39 1304Google Scholar
[32] Daniel M, Latha M M 2001 Physica A 298 351Google Scholar
[33] Zhang H Q, Tian B, Meng X H, Lü X, Liu W J 2009 Eur. Phys. J. B 72 233Google Scholar
[34] Liu R X, Tian B, Liu L C, Qin B, Lü X 2013 Physica B 413 120Google Scholar
[35] Peregrine D H 1983 The ANZIAM Journal 25 16
[36] Chen S H, Mihalache D 2015 J. Phys.A: Math. Theor. 48 215202Google Scholar
[37] Liu B Y, Fokas A S, Mihalache D, He J S 2016 Rom. Rep. Phys. 68 1425
[38] Zakharov V E, Gelash A A 2013 Phys. Rev. Lett. 111 054101Google Scholar
[39] Whitham G B 1999 Linear and Nonlinear Waves (2nd ed.) (New York: A Wiley-Interscience Publication) pp363-374
[40] Ruban V, Kodama Y, Ruderman M, et al. 2010 Eur. Phys. J. Special Topics 185 5Google Scholar
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图 2 (a)由明孤立波解(22)式描述的明孤立波传输图形, 其中参数选取为 α1 = 1, α2 = 2, α3 = 1, α4 = 8, α5 = 2,α6 = 6, α7 = 4, α8 = 6, c = 1, K = 1,
$\varOmega $ = 51/16, ε = 1, a = 1; (b) 由暗孤立波解(25)式描述的暗孤立波传输图形, 其中参数选取为α1 = –1, α2 = 2, α3 = 1, α4 = –8, α5 = –2, α6 = –6, α 7 = –4, α8 = 6, c = –7, K = 1,$\varOmega $ = –123/32, ε = 1, a = 1Fig. 2. (a) Propagation of bright solitary wave via Solution (22) with the parameters chosen as α1 = 1, α2 = 2, α3 = 1, α4 = 8, α5 = 2, α6 = 6, α7 = 4, α8 = 6, c = 1, K = 1,
$\varOmega $ = 51/16, ε = 1, a = 1; (b) propagation of dark solitary wave via Solution (25) with the parameters chosen as α1 = –1, α2 = 2, α3 = 1, α4 = –8, α5 = –2, α6 = –6, α7 = –4, α8 = 6, c = –7, K = 1,$\varOmega $ = –123/32, ε = 1, a = 1.图 6 (a) 群速度
$V_{\rm g}$ 随振幅参数c的变化(红实线)和(b)相速度$V_{\rm p}$ 随振幅参数c的变化(蓝点线), 其中参数选取为$\xi={1}/{2}(\sqrt{-4 c^2}-a)$ ,$\eta=0$ 和$a=1$ Fig. 6. Variation of the group velocity
$V_{\rm g}$ (red-solid line) and phase velocity$V_{\rm p}$ (blue-dot line) about the amplitude parameter c with the parameters chosen as$\xi={1}/{2}(\sqrt{-4 c^2}-a)$ ,$\eta=0$ and$a=1$ . -
[1] He J S, Xu S W, Porsezian 2012 Phys. Rev. E 86 066603Google Scholar
[2] Bludov Y V, Konotop V V, Akhmediev N 2009 Phys. Rev. A 80 033610Google Scholar
[3] Stenflo L, Marklund M 2010 J. Plasma Phys. 76 293Google Scholar
[4] Li M, Shui J J, Xu T 2018 Appl. Math. Lett. 83 110Google Scholar
[5] Li M, Shui J J, Huang Y H, Wang L, Li H J 2018 Phys. Scr. 93 115203Google Scholar
[6] Li M, Xu T, Meng D X 2016 J. Phys. Soc. Jpn. 85 124001Google Scholar
[7] Xu T, Lan S, Li M, Li L L, Zhang G W 2019 Physica D 390 47Google Scholar
[8] Xu T, Pelinovsky D E 2019 Phys. Lett. A 383 125948 ; Xu T, Chen Y, Li M, Meng D X 2019 Chaos 29 123124
[9] Agrawal G P 2012 Nonlinear Fiber Optics (5th ed.) (San Diego: Academic Press) pp120–150
[10] Ma Y C 1979 Stud. Appl. Math. 60 43Google Scholar
[11] Akhmediev N N, Korneev V I 1986 Theor. Math. Phys. 69 1089Google Scholar
[12] Calini A, Schober C M 2002 Phys. Lett. A 298 335Google Scholar
[13] Wang L, Zhang J H, Wang Z Q, Liu C, Li M, Qi F H, Guo R 2016 Phys. Rev. E 93 012214Google Scholar
[14] Akhmediev N N, Soto-Crespo J M, Ankiewica A 2009 Phys. Lett. A 373 2137Google Scholar
[15] Zuo D W, Gao Y T, Xue L, Feng Y J 2014 Chaos, Solitons Fractals 69 217227
[16] Solli D R, Ropers C, Koonath P, Jalali B 2007 Nature 450 1054Google Scholar
[17] Chabchoub A, Hoffmann N P, Akhmediev N 2011 Phys. Rev. E 106 204502
[18] Peregrine D H 1983 J. Austral. Math. Soc. Ser. B 25 16Google Scholar
[19] Akhmediev N N, Soto-Crespo J M, Ankiewica A 2009 Phys. Rev. A 80 043818Google Scholar
[20] Benjamin T B, Feir J E 1967 J. Fluid. Mech. 27 417Google Scholar
[21] Toffoli T, Fernandez L, Monbaliu J, Benoit M, Gagnaire-Renou E, Lefèvre J M, Cavaleri L, Proment D, Pakozdi C, Stansberg C T, Waseda T, Onorato M 2013 Phys. Fluids 25 091701Google Scholar
[22] Mussot A, Kudlinski A, Kolobov M, Louvergneaux E, Douay M, Taki M 2009 Opt. Express 17 17010Google Scholar
[23] Genty G, de Sterke C M, Bang O, Dias F, Akhmediev N, Dudley J M 2010 Phys. Lett. A 374 989Google Scholar
[24] He J S, Xu S W, Porsezian K, Cheng Y, Dinda P T 2016 Phys. Rev. E 93 062201Google Scholar
[25] He J S, Xu S W, Porsezian K, Dinda P T, Mihalache D, Malomed B A, Ding E 2017 Rom. J. Phys. 62 203
[26] Liu S D, Liu S K 1994 Soliton Wave and Turbulence (Chinese version) (1st ed.) (Shanghai: Shanghai Scientific and Technological Education Press) pp90–97
[27] Infeld E, Rowlands G 2000 Nonlinear Waves, Solitons and Chaos (2th ed.) (Cambridge: Cambridge University Press) pp144–156
[28] Choudhuri A, Porsezian K 2013 Phys. Rev. A 88 033808Google Scholar
[29] Porsezian K, Daniel M, Lakshmanan M 1992 J. Math. Phys. 33 1807Google Scholar
[30] Wang L H, Porsezian K, He J S 2013 Phys. Rev. E 87 053202Google Scholar
[31] Azzouzi F, Triki H, Mezghiche K, Akrmi A E 2009 Chaos, Solitons Fractals 39 1304Google Scholar
[32] Daniel M, Latha M M 2001 Physica A 298 351Google Scholar
[33] Zhang H Q, Tian B, Meng X H, Lü X, Liu W J 2009 Eur. Phys. J. B 72 233Google Scholar
[34] Liu R X, Tian B, Liu L C, Qin B, Lü X 2013 Physica B 413 120Google Scholar
[35] Peregrine D H 1983 The ANZIAM Journal 25 16
[36] Chen S H, Mihalache D 2015 J. Phys.A: Math. Theor. 48 215202Google Scholar
[37] Liu B Y, Fokas A S, Mihalache D, He J S 2016 Rom. Rep. Phys. 68 1425
[38] Zakharov V E, Gelash A A 2013 Phys. Rev. Lett. 111 054101Google Scholar
[39] Whitham G B 1999 Linear and Nonlinear Waves (2nd ed.) (New York: A Wiley-Interscience Publication) pp363-374
[40] Ruban V, Kodama Y, Ruderman M, et al. 2010 Eur. Phys. J. Special Topics 185 5Google Scholar
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