Abstract
The aim of this paper is to construct Wronskian solutions to a generalized KdV equation in (\(2+1\))-dimensions, which possesses a trilinear form. On the basis of two useful properties associated with Hirota differential operators, a general Wronskian formulation is established and the involved functions for Wronskian entries satisfy a system of combined linear partial differential equations. The key technique is to apply the Wronskian identity of the bilinear KP equation while presenting those sufficient conditions. Other illustrative examples of sufficient conditions are also given for the cKP3-4 equation, the (\(2+1\))-dimensional DJKM equation, and the dissipative (\(2+1\))-dimensional AKNS equation. Finally, N-soliton solutions and soliton molecules are worked out through the presented Wronskian formation.
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Acknowledgements
The authors express their sincere thanks to the Referees and Editors for their valuable comments. This work is supported by Jinhua Polytechnic Key Laboratory of Crop Harvesting Equipment Technology of Zhejiang Province.
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The work was supported in part by NSFC under the grants 12271488, 11975145 and 11972291.
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Appendix
Appendix
The proof of Lemma 2.1 is as follows:
Proof
By applying the conditions (2.5) and differential rules for determinants as defined in [18], we have the following derivatives of the Wronskian determinant \(f=f_{N}=|\widehat{N-1}|\):
Let us next suppose that
where \(\delta _{nr}, r=1,2,\ldots ,\mathrm {C_{m+n-1}^{n}},\) are expansion coefficients. Using the definition of D-operators and the above conditions (A.1), we further get
It means that Lemma 2.1 holds.
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Cheng, L., Zhang, Y. & Ma, WX. Wronskian \(\pmb {N}\)-soliton solutions to a generalized KdV equation in (\(\pmb {2+1}\))-dimensions. Nonlinear Dyn 111, 1701–1714 (2023). https://doi.org/10.1007/s11071-022-07920-7
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DOI: https://doi.org/10.1007/s11071-022-07920-7