• Acta Physica Sinica
  • Vol. 69, Issue 1, 010502-1 (2020)
Min Li1、*, Bo-Ting Wang1, Tao Xu2、*, and Juan-Juan Shui1
Author Affiliations
  • 1Department of Mathematics and Physics, North China Electric Power University, Beijing 102206, China
  • 2College of Science, China University of Petroleum, Beijing 102249, China
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    DOI: 10.7498/aps.69.20191384 Cite this Article
    Min Li, Bo-Ting Wang, Tao Xu, Juan-Juan Shui. Study on the generation mechanism of bright and dark solitary waves and rogue wave for a fourth-order dispersive nonlinear Schrödinger equation[J]. Acta Physica Sinica, 2020, 69(1): 010502-1 Copy Citation Text show less
    Phase portraits of System (15): (a) Homoclinic orbits (β1 = –1/10, β2 = 1/18); (b) heteroclinic orbits (β1 = 1, β2 = –5/9).系统(15)的相位图 (a)同宿轨道(β1 = –1/10, β2 = 1/18); (b) 异宿轨道(β1 = 1, β2 = –5/9)
    Fig. 1. Phase portraits of System (15): (a) Homoclinic orbits (β1 = –1/10, β2 = 1/18); (b) heteroclinic orbits (β1 = 1, β2 = –5/9). 系统(15)的相位图 (a)同宿轨道(β1 = –1/10, β2 = 1/18); (b) 异宿轨道(β1 = 1, β2 = –5/9)
    (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, = 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, = –123/32, ε = 1, a = 1.(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, = 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, α7 = –4, α8 = 6, c = –7, K = 1, = –123/32, ε = 1, a = 1
    Fig. 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, = 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, = –123/32, ε = 1, a = 1. (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, = 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, α7 = –4, α8 = 6, c = –7, K = 1, = –123/32, ε = 1, a = 1
    The propagation of one breather via Solution (32) with the parameters chosen as , , and .解(32)式描述的一阶呼吸子的动力学演化, 其中参数选取为, , 和
    Fig. 3. The propagation of one breather via Solution (32) with the parameters chosen as , , and . 解(32)式描述的一阶呼吸子的动力学演化, 其中参数选取为 , , 和
    Group velocity (red-solid line) and phase velocity (blue-dot line) of the breather呼吸子的群速度(红实线)和相速度(蓝虚线)随参数a的变化关系
    Fig. 4. Group velocity (red-solid line) and phase velocity (blue-dot line) of the breather 呼吸子的群速度 (红实线)和相速度 (蓝虚线)随参数a的变化关系
    The propagation of first-order rogue wave via Solution (42) with the parameters chosen as , , , , and .解(42)式描述的一阶怪波的动力学演化, 其中参数选取为, , , , 和
    Fig. 5. The propagation of first-order rogue wave via Solution (42) with the parameters chosen as , , , , and . 解(42)式描述的一阶怪波的动力学演化, 其中参数选取为 , , , , 和
    Variation of the group velocity (red-solid line) and phase velocity (blue-dot line) about the amplitude parameter c with the parameters chosen as , and .(a) 群速度随振幅参数c的变化(红实线)和(b)相速度随振幅参数c的变化(蓝点线), 其中参数选取为, 和
    Fig. 6. Variation of the group velocity (red-solid line) and phase velocity (blue-dot line) about the amplitude parameter c with the parameters chosen as , and . (a) 群速度 随振幅参数c的变化(红实线)和(b)相速度 随振幅参数c的变化(蓝点线), 其中参数选取为 , 和
    Min Li, Bo-Ting Wang, Tao Xu, Juan-Juan Shui. Study on the generation mechanism of bright and dark solitary waves and rogue wave for a fourth-order dispersive nonlinear Schrödinger equation[J]. Acta Physica Sinica, 2020, 69(1): 010502-1
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