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There has been considerable interest in the Kadomtsev-Petviashvili (KP) equation, which arises in many physical applications including shallow water waves and plasma physics.
This feature of our approach may be important in many physical applications because the locations of the zeros and poles have physically meaningful consequences, including the resonant frequencies and linewidths of the effective trapped cavity modes resulting in the network due to feedback.
The constant impulse is a class of common impulsive perturbations appearing in many physical applications.
However, in many physical applications, we need to consider geometries that are more sophisticated.
This equation appears in many physical applications and is used as a model for nonlinear dispersive waves.
In many physical applications, large scales numerical simulation is no longer possible because of a lack of computing resources.
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Many physical application problems are axis-symmetric.
Spectral problems of differential operators arise in many different physical applications.
In many real physical applications, performing high-order and efficient numerical methods for solving the partial differential equations is essential.
For example, this equation has many direct physical applications to solids, liquids, gases, plasma, the FPU problem, rotating flow in tube [2, 5], and so on.
It is one of the most important nonlinear PDEs arising in the study of water waves and is used in the analysis of many other physical applications such as the percolation of water in the porous subsurface of a horizontal layer of material [7].
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