Klein–Roudenko–Stoilov blow-up rate conjecture for the critical generalized Zakharov–Kuznetsov equation

Let QQ denote the unique positive radial solution on R2\mathbb{R}^2 of

ΔQ+QQ3=0.-\Delta Q+Q-Q^3=0.

Consider the critical two-dimensional Zakharov–Kuznetsov equation

ut+x1(Δu+u3)=0,u_t+\partial_{x_1}(\Delta u+u^3)=0,

with initial data u(0,x1,x2)=u0(x1,x2)H1(R2)u(0,x_1,x_2)=u_0(x_1,x_2)\in H^1(\mathbb{R}^2). For sufficiently localized u0S(R2)u_0\in\mathcal{S}(\mathbb{R}^2) satisfying u0L2>QL2\|u_0\|_{L^2}>\|Q\|_{L^2}, let λ(t)\lambda(t) and (x(t),y(t))(x(t),y(t)) be the blow-up scale and modulation parameters.

Klein–Roudenko–Stoilov conjecture. The solution blows up at a finite time TT, and, as tTt\to T,

u(x,y,t)1λ(t)Q(xx(t)λ(t),yy(t)λ(t))u~L2,u(x,y,t)-\frac{1}{\lambda(t)}Q\left(\frac{x-x(t)}{\lambda(t)},\frac{y-y(t)}{\lambda(t)}\right)\to\widetilde{u}\in L^2,

with

u(t)L21(Tt)1/2,λ(t)(Tt)1/2,\|\nabla u(t)\|_{L^2}\sim\frac{1}{(T-t)^{1/2}},\qquad \lambda(t)\sim(T-t)^{1/2},

and

x(t)1Tt,y(t)yR.x(t)\sim\frac{1}{T-t},\qquad y(t)\to y^*\in\mathbb{R}.

The paper states that its findings instead give an exponent approximately equal to 3/43/4, so the conjectured exponent 1/21/2 is contradicted by the paper's claimed result.

Sources & referencesView supporting material

Primary source

Francisc Bozgan, Tej-Eddine Ghoul, Nader Masmoudi and Kai Yang, “Blow-Up Dynamics for the L^2 critical case of the 2D Zakharov-Kuznetsov equation”, arXiv:2406.06568 (2024).

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