2015
DOI: 10.1016/j.aop.2015.06.017
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Darboux transformation of the Drinfeld–Sokolov–Satsuma–Hirota system and exact solutions

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Cited by 17 publications
(6 citation statements)
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“…Choose a constant 1 = 11 + 2 . Let Ω( 1 ) be the solution to Lax pair (6) and (16) when = 1 , and let Ω ′ ( 1 ) = Ω (1) ( 1 ) be defined by (25). Choose…”
Section: F I G U R E 3 a First-order Rogue Wavementioning
confidence: 99%
See 1 more Smart Citation
“…Choose a constant 1 = 11 + 2 . Let Ω( 1 ) be the solution to Lax pair (6) and (16) when = 1 , and let Ω ′ ( 1 ) = Ω (1) ( 1 ) be defined by (25). Choose…”
Section: F I G U R E 3 a First-order Rogue Wavementioning
confidence: 99%
“…Choose a constant 1 = 11 + 2 . Let Ω( 1 ) be the solution to Lax pair (6) and (16) when = 1 , and let Ω ′ ( 1 ) = Ω (1) ( 1 ), Ω ′′ ( 1 ) = Ω (2) ( 1 ) be defined by (25). Choose By using (20) and its derivatives with respect to , we can obtain ( 1 ), ( 1 ), ′ ( 1 ), ′ ( 1 ), ′′ ( 1 ), and ′′ ( 1 ).…”
Section: F I G U R E 3 a First-order Rogue Wavementioning
confidence: 99%
“…It should be pointed out that the two-component mYOLS Equation (10) is different from the long-wave-short-wave resonance Equation (1), and the two-component mYOLS Equation (10) is equivalent to the long-wave-short-wave model (2) under some transformation [21]. Then, with the help of Riccati equations for the Lax pair associated with the vmYOLS Equation (8) [22][23][24], Bäcklund transformation [25,26], Darboux transformation [27][28][29][30][31][32][33][34][35][36][37][38][39], and others [40][41][42][43][44][45][46][47][48][49][50][51]. Some interesting explicit solutions have been found, the most important among which are pure-soliton solutions, quasi-periodic solutions, and rogue waves solutions.…”
Section: Introductionmentioning
confidence: 99%
“…where the solution is defined. Example 2: As the next example, we consider the time-fractional coupled Drinfeld--Sokolov-Satsuma-Hirota (DSSH) as [23]:…”
Section: Application Of the Methodsmentioning
confidence: 99%