2020
DOI: 10.1007/s11071-020-05611-9
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M-lump, high-order breather solutions and interaction dynamics of a generalized $$(2 + 1)$$-dimensional nonlinear wave equation

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Cited by 65 publications
(15 citation statements)
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“…The single lump wave travels black line y = − 1 2 x (black line in Fig. (7)) before the interaction. Then the trajectory of the lump wave changes into line y = − 1 2 x + 294 293 (red line in Fig.…”
Section: N -Soliton Solutionsmentioning
confidence: 99%
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“…The single lump wave travels black line y = − 1 2 x (black line in Fig. (7)) before the interaction. Then the trajectory of the lump wave changes into line y = − 1 2 x + 294 293 (red line in Fig.…”
Section: N -Soliton Solutionsmentioning
confidence: 99%
“…Then the trajectory of the lump wave changes into line y = − 1 2 x + 294 293 (red line in Fig. (7)) after the interaction. It is notable that the center of the lump wave is located at the bifurcation point of the resonance solitary wave as t = 0.…”
Section: N -Soliton Solutionsmentioning
confidence: 99%
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“…e4k 2 +e5l 2 )(ω 2 +e1k 2 ) .Therefore, from Eqs (32). and(33), we can getu(x, y, t) = 12b tanh[b(kx + ly − ωt)] [b(kx + ly − ωt)].…”
mentioning
confidence: 98%