Abstract

Under the well-known bilinear method of Hirota, the specific expression for N-soliton solutions of (2+1)-dimensional generalized Caudrey–Dodd–Gibbon–Kotera–Sawada(gCDGKS) equation in fluid mechanics is given. By defining a novel restrictive condition on N-soliton solutions, resonant Y-type and X-type soliton solutions are generated. Under the new proposed constraint, combined with the velocity resonance method and module resonant method, the mixed solutions of resonant Y-type solitons and line waves and breather solutions are found. Finally, with the support of long-wave limit method, the interaction between resonant Y-type solitons and higher-order lumps is shown, and the motion trajectory equation before and after the interaction between lumps and resonant Y-type solitons is derived. These new results greatly extend the exact solution of (2+1)-dimensional gCDGKS equation already available in the literature and provide new ideas for studying the dynamical behaviors of fluid mechanic, soliton and shallow water wave and so on.

Highlights

  • As a local nonlinear wave, solitons have many interesting properties [1]

  • By adding some constraints on the N-soliton solution obtained by Hirota bilinear method, one can obtain many types of bound molecules

  • Through the velocity resonance mechanism, the soliton molecular solution first observed in physical experiments is obtained [2,3,4,5,6]

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Summary

Introduction

As a local nonlinear wave, solitons have many interesting properties [1]. By adding some constraints on the N-soliton solution obtained by Hirota bilinear method, one can obtain many types of bound molecules. Chen and others constructed another constraint, which obtained the mixed solutions of resonant Y-type soliton and 1-order lump [22]. In order to obtain more interaction solutions between resonant Y-type solitons and other solutions, Li et al proposed a new constraint [24,25,26,27]. By this method, we can obtain the mixed solutions of resonant Y-shaped solitons and line waves, higher-order lumps, breather solutions and resonant Y-shaped solitons respectively.

N-soliton solution
Resonance Y-shape soliton
Interaction between resonant Y-shape soliton solution and lump solution
Conclusions
Data Availability Statements
Full Text
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