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Finite-time blow-up for the real-valued defocusing energy-supercritical quintic NLW

Published 5 Oct 2026 in math.AP | (2610.06678v1)

Abstract: We consider the defocusing quintic wave equation ∂t<sup>2u−Δu+u<sup>5=0\partial_t<sup>2u-Δu+u<sup>5=0 for real-valued functions on R<sup>1+10\mathbb{R}<sup>{1+10}, which is energy-supercritical. We construct a discretely self-similar solution in a backward light cone, of the form u(t,x)=(T−t)<sup>−1/2W<sup><em>(ω</em>log⁡1T−t,∣x∣T−t),u(t,x)=(T-t)<sup>{-1/2}W<sup><em>\big(ω^</em>\log\frac1{T-t},\frac{|x|}{T-t}\big), where the nonzero profile W<sup>∗W<sup>* is $2π$-periodic in its first variable and real-analytic up to and across the light cone. Cutting off its initial data gives smooth, compactly supported, radial data whose solution coincides with the discretely self-similar solution in the backward light cone, is smooth on [0,T]×R<sup>10[0,T]\times\mathbb{R}<sup>{10} except at the vertex (T,0)(T,0) of the cone, and blows up there at the self-similar rate. The solutions we construct here appear to be the first real-valued blow-up solutions of defocusing energy-supercritical NLW. Existence of the real profile is proved by a computer-assisted Newton--Kantorovich argument in a Banach algebra of Fourier--Chebyshev coefficients, with rigorous error control. We find the approximate profile by numerically continuing rotating self-similar profiles of the complex-valued equation. This step is not essential for the blow-up proof, so it is left as non-rigorous numerics. The main analytic ingredients are an exact description of the mode operators for the linear part, which are hypergeometric and upper triangular in the Chebyshev basis, and a bound for their inverses that is uniform at high frequencies. All computer-assisted proofs, including the requisite codes and the approximate objects, are accessible on GitHub at \cite{code}.

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