English

Counterexamples to the comparison principle in the special Lagrangian potential equation

Analysis of PDEs 2022-10-19 v2

Abstract

For each k=0,,nk = 0,\dots,n we construct a continuous phase fkf_k, with fk(0)=(n2k)π2f_k(0) = (n-2k)\frac{\pi}{2}, and viscosity sub- and supersolutions vkv_k, uku_k, of the elliptic PDE i=1narctan(λi(D2w))=fk(x)\sum_{i=1}^n \arctan(\lambda_i(D^2 w)) = f_k(x) such that vkukv_k-u_k has an isolated maximum at the origin. It has been an open question whether the comparison principle would hold in this second order equation for arbitrary continuous phases f ⁣:Ω(nπ/2,nπ/2)f\colon\Omega\to (-n\pi/2,n\pi/2). Our examples show it does not.

Keywords

Cite

@article{arxiv.2206.09373,
  title  = {Counterexamples to the comparison principle in the special Lagrangian potential equation},
  author = {Karl K. Brustad},
  journal= {arXiv preprint arXiv:2206.09373},
  year   = {2022}
}