2011
DOI: 10.1016/j.nonrwa.2010.11.002
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Bifurcation of peakons and periodic cusp waves for the generalization of the Camassa–Holm equation

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Cited by 20 publications
(14 citation statements)
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References 20 publications
(49 reference statements)
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“…Han et al [9] studied the solitary waves and wave-breaking phenomena for GDGH2 system (2). In this paper, we study the bifurcations and nonlinear wave solutions for the GDGH2 system (2) by employing the bifurcation method and qualitative theory of dynamical systems [6,7,12,[14][15][16][17][18][19][20][22][23][24]. Through the bifurcations of phase portraits corresponding to system (2), we not only show the existence of several types of nonlinear wave solutions, including solitary waves, peakons, periodic cusp waves, periodic waves, compacton-like waves and kink-like waves, but also obtain their implicit expressions.…”
Section: Introductionmentioning
confidence: 99%
“…Han et al [9] studied the solitary waves and wave-breaking phenomena for GDGH2 system (2). In this paper, we study the bifurcations and nonlinear wave solutions for the GDGH2 system (2) by employing the bifurcation method and qualitative theory of dynamical systems [6,7,12,[14][15][16][17][18][19][20][22][23][24]. Through the bifurcations of phase portraits corresponding to system (2), we not only show the existence of several types of nonlinear wave solutions, including solitary waves, peakons, periodic cusp waves, periodic waves, compacton-like waves and kink-like waves, but also obtain their implicit expressions.…”
Section: Introductionmentioning
confidence: 99%
“…In our previous work , we studied the peakons and periodic cusp wave solutions of Eq. when n = 1, m ≥2 and n ≥2, m = n + 1, by exploiting the bifurcation method and qualitative theory of dynamical systems , and setting the integral constant to be zero. The results of are summarized as follows: When n = 1, m = 2, Eq.…”
Section: Introductionmentioning
confidence: 99%
“…when n = 1, m ≥2 and n ≥2, m = n + 1, by exploiting the bifurcation method and qualitative theory of dynamical systems , and setting the integral constant to be zero. The results of are summarized as follows: When n = 1, m = 2, Eq. has peakons falseu¯1(x,t,c)=cnormale|xct|,and periodic cusp wave solutions falseu¯2(ξ,K,c)=falseu¯0()ξ21emnormalifalseT¯0,K,c,where i=0,±1,±2,0.3em,ξ=xct[](21emnormali1)falseT¯0,(2normali+1)falseT¯0, and falseu¯0(ξ,K,c)=3(2K+1)(32K)16K2falseα¯normale2K3|ξ|+falseα¯4normale2K3|ξ|+32K4K<...>…”
Section: Introductionmentioning
confidence: 99%
“…In this paper, we employ the bifurcation method and qualitative theory of dynamical systems [11][12][13][14][15][16][17][18][19][20][21] to investigate the nonlinear wave solutions for (1), and we obtain many exact explicit expressions of nonlinear wave solutions for (1). These nonlinear wave solutions contain solitary wave solutions, singular solutions, periodic singular solutions, and kink-shaped solutions, most of which, to our knowledge, are newly obtained.…”
Section: Introductionmentioning
confidence: 99%