For p=2,3,4, the coefficient beta_1^{(p)}(h) controlling the exponentially small width of the p-th Stokes-wave isolas has explicit deep-water asymptotics, namely (3*sqrt(3)/64)e^{-h/2}, (2*sqrt(2)/3)e^{-2h}, and -(5*sqrt(5)/(8*sqrt(3)))e^{-2h}.
Full description of Benjamin-Feir instability for generalized Korteweg-de Vries equations
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abstract
In this paper we consider a family of generalized Korteweg-de Vries equations and study the linear modulational instability of small amplitude traveling waves solutions. Under explicit non-degeneracy conditions on the dispersion relation, we completely describe the spectrum near the origin of the linearized operator at such solutions and prove that the unstable spectrum (when present) is composed by branches depicting always a closed figure ''8''. We apply our abstract theorem to several equations such as the Whitham, the gravity-capillary Whitham and the Kawahara equations, confirming that the unstable spectrum of the corresponding linearized operators exhibits a figure ''8'' instability, as it was observed before only numerically. Our method of proof uses a symplectic version of Kato's theory of similarity transformation to reduce the problem to determine the eigenvalues of a $3 \times 3$ complex Hamiltonian and reversible matrix. Then, via a block-diagonalization procedure, we conjugate such matrix into a block-diagonal one composed by a $2\times 2$ Hamiltonian and reversible matrix, describing the unstable spectrum, and a single purely imaginary element describing the stable eigenvalue.
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On higher order isolas of unstable Stokes waves
For p=2,3,4, the coefficient beta_1^{(p)}(h) controlling the exponentially small width of the p-th Stokes-wave isolas has explicit deep-water asymptotics, namely (3*sqrt(3)/64)e^{-h/2}, (2*sqrt(2)/3)e^{-2h}, and -(5*sqrt(5)/(8*sqrt(3)))e^{-2h}.