Benjamin-Ono Soliton Dynamics in a slowly varying potential revisited

preprint2022arXivOpen access

Abstract

The Benjamin Ono equation with a slowly varying potential is (pBO)ut+(Hux−Vu+12u2)x=0 \text{(pBO)} \qquad u_t + (Hu_x-Vu + \tfrac12 u^2)_x=0 with V(x)=W(hx)V(x)=W(hx), 0<h≪10< h \ll 1, and W∈Cc∞(R)W\in C_c^\infty(\mathbb{R}), and HH denotes the Hilbert transform. The soliton profile is Qa,c(x)=cQ(c(x−a)) , where Q(x)=41+x2Q_{a,c}(x) = cQ(c(x-a)) \,, \text{ where } Q(x) = \frac{4}{1+x^2} and a∈Ra\in \mathbb{R}, c>0c>0 are parameters. For initial condition u0(x)u_0(x) to (pBO) close to Q0,1(x)Q_{0,1}(x), it was shown in a previous work by Z. Zhang that the solution u(x,t)u(x,t) to (pBO) remains close to Qa(t),c(t)(x)Q_{a(t),c(t)}(x) and approximate parameter dynamics for (a,c)(a,c) were provided, on a dynamically relevant time scale. In this paper, we prove exact (a,c)(a,c) parameter dynamics. This is achieved using the basic framework of the previous work by Z. Zhang but adding a local virial estimate for the linearization of (pBO) around the soliton. This is a local-in-space estimate averaged in time, often called a local smoothing estimate, showing that effectively the remainder function in the perturbation analysis is smaller near the soliton than globally in space. A weaker version of this estimate is proved in a paper by Kenig & Martel as part of a "linear Liouville" result, and we have adapted and extended their proof for our application.

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