Abstract
The interaction of two lump solitons described by the Kadomtsev–Petviashvili I (KPI) equation is analysed using both exact and numerical methods. The numerical method is based on a third order Runge–Kutta method, and a Crank–Nicholson scheme. The main characteristic of a direct interaction when the two lumps are initially aligned along the x-axis is that they may separate in the y-direction, but then come back to the x-axis after collision; the dependence of the maximum separation in the y-direction on the relative velocity difference is described. Two lumps may also experience an abrupt phase change in the case of an oblique interaction.
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