2022
DOI: 10.1007/s00021-022-00685-4
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The Shallow-Water Models with Cubic Nonlinearity

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Cited by 19 publications
(6 citation statements)
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“…Proof. Proving ( 7) is done by applying 𝐿 given in (6), on 𝜙 and 𝜙 ′ and using the facts that 𝜙 ′2 = 𝜙 2 , 𝜙 ′′ = 𝜙 − 2𝛿 0 , and (1 − 𝜙 2 )𝛿 0 = 0, with 𝛿 0 being the Dirac delta distribution centered at 𝜉 = 0. □…”
Section: Lemmamentioning
confidence: 99%
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“…Proof. Proving ( 7) is done by applying 𝐿 given in (6), on 𝜙 and 𝜙 ′ and using the facts that 𝜙 ′2 = 𝜙 2 , 𝜙 ′′ = 𝜙 − 2𝛿 0 , and (1 − 𝜙 2 )𝛿 0 = 0, with 𝛿 0 being the Dirac delta distribution centered at 𝜉 = 0. □…”
Section: Lemmamentioning
confidence: 99%
“…We multiply both sides of the resolvent equation ( 16) by v and integrate over ℝ. Using the definition of 𝐿 given in (6), one finds…”
Section: Spectral and Linear Instability On 𝑳 𝟐 (ℝ)mentioning
confidence: 99%
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“…The equation (1.1) is known to be completely integrable via the Inverse Scattering Transform, has infinitely many symmetries and conserved quantities, and is bi-Hamiltonian [26,40]. Further, the Novikov equation has been shown to model the propagation of shallow water waves of moderately large amplitude [11]. In this regard, (1.1) can be regarded as generalization of the Camassa-Holm equation [8,9] (1.2)…”
Section: Introductionmentioning
confidence: 99%