TY - JOUR
T1 - A new integrable equation with no smooth solitons
AU - Qiao, Zhijun
AU - Liu, Liping
PY - 2009/7/30
Y1 - 2009/7/30
N2 - In this paper, we propose a new completely integrable equation:mt = frac(1, 2) fenced(frac(1, m2))xxx - frac(1, 2) fenced(frac(1, m2))x,which has no smooth solitons. This equation is shown to have bi-Hamiltonian structure and Lax pair, which imply integrability of the equation. Studying this new equation, we develop two new kinds of soliton solutions under the inhomogeneous boundary condition lim| x | → ∞ m = B where B is nonzero constant. One is continuous and piecewise smooth "W/M"-shape-peaks solitary solution and the other one-single-peak soliton. The two new kinds of peaked solitons can not be written as the regular type peakon: c e- | x - ct |, where c is a constant. We will provide graphs to show those new kinds of peaked solitons. © 2008 Elsevier Ltd. All rights reserved.
AB - In this paper, we propose a new completely integrable equation:mt = frac(1, 2) fenced(frac(1, m2))xxx - frac(1, 2) fenced(frac(1, m2))x,which has no smooth solitons. This equation is shown to have bi-Hamiltonian structure and Lax pair, which imply integrability of the equation. Studying this new equation, we develop two new kinds of soliton solutions under the inhomogeneous boundary condition lim| x | → ∞ m = B where B is nonzero constant. One is continuous and piecewise smooth "W/M"-shape-peaks solitary solution and the other one-single-peak soliton. The two new kinds of peaked solitons can not be written as the regular type peakon: c e- | x - ct |, where c is a constant. We will provide graphs to show those new kinds of peaked solitons. © 2008 Elsevier Ltd. All rights reserved.
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U2 - 10.1016/j.chaos.2007.11.034
DO - 10.1016/j.chaos.2007.11.034
M3 - Article
SN - 0960-0779
VL - 41
SP - 587
EP - 593
JO - Chaos, Solitons and Fractals
JF - Chaos, Solitons and Fractals
IS - 2
ER -