Numerical cusp-formation conjecture for Whitham and fractional KdV equations

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Let u0∈L2(R)u_0\in L_2(\mathbb{R}) be smooth initial data with a single negative hump. For −1<α<0-1<\alpha<0, solutions to the Whitham equation and to the fKdV equations with sufficiently small mass remain smooth for all tt and are radiated away. For α=−1/2\alpha=-1/2, solutions with negative initial data and sufficiently large mass develop, at t∗>tct^*>t_c, a cusp of the form ∣x−x∗∣1/3|x-x^*|^{1/3}, while the supremum norm remains bounded at the blow-up point. Solutions with positive initial data and sufficiently large norm mass develop, at t∗<tct^*<t_c, a cusp of the form ∣x−x∗∣1/2|x-x^*|^{1/2}. Numerical Whitham–fKdV cusp conjecture. The stated global-radiation and cusp-formation behavior holds for the indicated equations, parameters, and initial data. The claims are based on numerical observations of singularity formation and remain open in the supplied text.

References

Primary source

C. Klein and J. -C. Saut, “A numerical approach to Blow-up issues for dispersive perturbations of Burgers' equation”, arXiv:1401.1390 (2014).

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