2018
DOI: 10.1007/s12043-017-1512-y
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Rogue waves in the multicomponent Mel’nikov system and multicomponent Schrödinger–Boussinesq system

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Cited by 16 publications
(14 citation statements)
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“…Thus, they have attracted a lot of attention in the physics and nonlinear waves communities in recent years. Analytical expressions of rogue waves have been derived in a large number of integrable nonlinear wave equations, such as the nonlinear Schrödinger (NLS) equation [19][20][21][22][23][24][25][26][27][28], the derivative NLS equation [29,30], the three-wave interaction equation [31], the Davey-Stewartson equations [32,33], and many others [34][35][36][37][38][39][40][41][42][43][44][45][46][47][48][49][50][51][52][53]. Rogue waves have also been observed in water tanks [54,55] and optical fibers [56][57][58].…”
Section: Introductionmentioning
confidence: 99%
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“…Thus, they have attracted a lot of attention in the physics and nonlinear waves communities in recent years. Analytical expressions of rogue waves have been derived in a large number of integrable nonlinear wave equations, such as the nonlinear Schrödinger (NLS) equation [19][20][21][22][23][24][25][26][27][28], the derivative NLS equation [29,30], the three-wave interaction equation [31], the Davey-Stewartson equations [32,33], and many others [34][35][36][37][38][39][40][41][42][43][44][45][46][47][48][49][50][51][52][53]. Rogue waves have also been observed in water tanks [54,55] and optical fibers [56][57][58].…”
Section: Introductionmentioning
confidence: 99%
“…The technique we will use is the bilinear Kadomtsev-Petviashvili (KP) reduction method [62]. Although this technique has been applied to derive rogue waves in several other integrable equations before [26,32,33,42,[49][50][51]53], when it is applied to the Boussinesq equation, the previous choices of differential operators within this technique would cause considerable technical complications. Here, we propose a new judicious choice of those differential operators, which will drastically simplify the dimension reduction calculation as well as the analytical expressions of rogue wave solutions.…”
Section: Introductionmentioning
confidence: 99%
“…The stable and unstable parametric regimes of DAWs are organized by the sign of P and Q of Eq. (28) [14,15,16,17,18,19,20]. When P and Q have same sign (i.e., P/Q > 0), the evolution of the DAWs amplitude is modulationally unstable in presence of the external perturbations.…”
Section: Modulational Instability and Rogue Wavesmentioning
confidence: 99%
“…The plot of P/Q against k yields stable and unstable parametric regimes of the DAWs. The point, at which the transition of P/Q curve intersect with k-axis, is known as threshold or critical wave number k (= k c ) [18,19,20,21,22,23,24,25]. The governing equation for highly energetic DARWs in the modulationally unstable parametric regime (P/Q > 0) can be written as [26,27,28,29,30]…”
Section: Modulational Instability and Rogue Wavesmentioning
confidence: 99%
“…In the previous studies, high‐order rogue waves in the NLS equation have been discussed, which are also localized in both space and time and could exhibit higher main peaks in fundamental pattern. In addition to the NLS equation, families of nonlinear soliton equations have been verified possessing rogue wave solutions …”
Section: Introductionmentioning
confidence: 99%