Dynamical interactions between higher-order rogue waves and various forms of n-soliton solutions (n → ∞) of the (2+1)-dimensional ANNV equation
Md Fazlul Hoque1, †, Harun-Or-Roshid1,, ‡, and Fahad Sameer Alshammari2
1 Department of Mathematics, Pabna University of Science and Technology, Pabna 6600, Bangladesh 2 Department of Mathematics, College of Science at Alkharj, Prince Sattam bin Abdulaziz University, Alkharj, Saudi Arabia
We present new lemmas, theorem and corollaries to construct interactions among higher-order rogue waves, n-periodic waves and n-solitons solutions (n → ∞) to the (2+1)-dimensional asymmetric Nizhnik–Novikov–Veselov (ANNV) equation. Several examples for theories are given by choosing definite interactions of the wave solutions for the model. In particular, we exhibit dynamical interactions between a rogue and a cross bright-dark bell wave, a rogue and a cross-bright bell wave, a rogue and a one-, two-, three-, four-periodic wave. In addition, we also present multi-types interactions between a rogue and a periodic cross-bright bell wave, a rogue and a periodic cross-bright-bark bell wave. Finally, we physically explain such interaction solutions of the model in the 3D and density plots.
Md Fazlul Hoque, Harun-Or-Roshid, and Fahad Sameer Alshammari Dynamical interactions between higher-order rogue waves and various forms of n-soliton solutions (n → ∞) of the (2+1)-dimensional ANNV equation 2020 Chin. Phys. B 29 114701
Fig. 1.
The 3D (upper) and density (lower) profiles of Eq. (8) for : interaction between (a) a rogue and a bright bell wave, (b) a rogue and a two-bell (one bright and one dark) wave, and (c) a rogue and a four-bell (double bright and double dark) wave.
Fig. 2.
The 3D (upper) and density (lower) profiles of Eq. (8) for : interaction between (a) a rogue and a bright bell wave, (b) a rogue and a two-cross-bright-bell wave, and (c) a rogue and a four-cross-bright-bell wave.
Fig. 3.
The 3D (upper) and density (lower) profiles of Eq. (17) for : (a) a single rogue wave; and interaction between (b) a rogue and a bright bell wave, and (c) a rogue and a three-bell (double bright and single dark) wave.
Fig. 4.
The 3D (upper) and density (lower) profiles of Eq. (17) for : (a) a single rogue wave; and interaction between (b) a rogue and a cross-bright bell wave, and (c) a rogue and a triple cross-bright bell wave.
Fig. 5.
The 3D (upper) and density (lower) profiles of Eq. (18) for : interaction between (a) a rogue and a periodic wave, (b) a rogue and a double periodic wave, and (c) a rogue and a triple periodic wave.
Fig. 6.
The 3D (upper) and density (lower) profiles of Eq. (18) for : interaction between (a) a rogue and a periodic wave, (b) a rogue and a double periodic wave, and (c) a rogue and a triple periodic wave.
Fig. 7.
The 3D (upper) and density (lower) profiles of Eq. (19) for : interaction between (a) a rogue and a periodic wave, (b) a rogue and a double periodic wave, and (c) a rogue and a four-periodic-bell wave.
Fig. 8.
The 3D (upper) and density (lower) profiles of Eq. (19) for : interaction between (a) a rogue and a periodic wave, (b) a rogue and a double-periodic-bell wave, and (c) a rogue and a four-periodic-bell wave.
Fig. 9.
The 3D (upper) and density (lower) profiles of Eq. (20) for : multi-interaction among a rogue periodic wave and bright-bark bell soliton waves.
Fig. 10.
The 3D (upper) and density (lower) profiles of Eq. (20) for : multi-interaction among a rogue periodic wave and bright-bark bell soliton waves.
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