The weak null condition and global existence using the p-weighted energy method

TL;DR

This paper proves global existence for small data solutions to a broad class of quasilinear wave equations satisfying the weak null condition, using a robust p-weighted energy method that handles degenerate energies and geometric complexities.

Contribution

It extends the class of equations known to have global solutions under the weak null condition, including Einstein and Einstein-Maxwell equations, with new techniques for degenerate energies and shock formation.

Findings

Proved global existence for equations satisfying the weak null condition.

Established a connection between the weak null condition and shock formation at infinity.

Developed a generalized p-weighted energy method adaptable to dynamic geometries.

Abstract

We prove global existence for solutions arising from small initial data for a large class of quasilinear wave equations satisfying the `weak null condition' of Lindblad and Rodnianski, significantly enlarging upon the class of equations for which global existence is known. In addition to the usual weak null condition, we require a certain hierarchical structure in the semilinear terms. Included in this class are the Einstein equations in harmonic coordinates, so a special case of our results is a new proof of the stability of Minkowski space. Our proof also applies to the coupled Einstein-Maxwell system in harmonic coordinates and Lorenz gauge, as well as to various model scalar wave equations which do not satisfy the null condition. Our proof also applies to the Einstein(-Maxwell) equations if, after writing the equations as a set of nonlinear wave equations, we then `forget' about the gauge conditions. The methods we use allow us to treat initial data which only has a small `degenerate energy', involving a weight that degenerates at null infinity, so the usual (unweighted) energy might be unbounded. We also demonstrate a connection between the weak null condition and geometric shock formation, showing that equations satisfying the weak null condition can exhibit `shock formation at infinity', of which we provide an explicit example. The methods that we use are very robust, including a generalisation of the p-weighted energy method of Dafermos and Rodnianski, adapted to the dynamic geometry. This means that our proof applies in a wide range of situations, including those in which the metric remains close to, but never approaches the flat metric in some spatially bounded domain, and those in which the `geometric' null infinity and the `background' null infinity differ dramatically, for example, when the solution exhibits shock formation at null infinity.