English

Maximum principles for boundary-degenerate linear parabolic differential operators

Analysis of PDEs 2013-07-23 v2 Probability

Abstract

We develop weak and strong maximum principles for boundary-degenerate, linear, parabolic, second-order partial differential operators, Lu:=ut\tr(aD2u)b,Du+cuLu := -u_t-\tr(aD^2u)-\langle b, Du\rangle + cu, with \emph{partial} Dirichlet boundary conditions. The coefficient, a(t,x)a(t,x), is assumed to vanish along a non-empty open subset, \mydirac0!\sQ\mydirac_0!\sQ, called the \emph{degenerate boundary portion}, of the parabolic boundary, \mydirac!\sQ\mydirac!\sQ, of the domain \sQ\RRd+1\sQ\subset\RR^{d+1}, while a(t,x)a(t,x) may be non-zero at points in the \emph{non-degenerate boundary portion}, \mydirac1!\sQ:=\mydirac!\sQ\less\mydirac0!\sQˉ\mydirac_1!\sQ := \mydirac!\sQ\less\bar{\mydirac_0!\sQ}. Points in \mydirac0!\sQ\mydirac_0!\sQ play the same role as those in the interior of the domain, \sQ\sQ, and only the non-degenerate boundary portion, \mydirac1!\sQ\mydirac_1!\sQ, is required for boundary comparisons. We also develop comparison principles and a priori maximum principle estimates for solutions to boundary value and obstacle problems defined by boundary-degenerate parabolic operators, again where only the non-degenerate boundary portion, \mydirac1!\sQ\mydirac_1!\sQ, is required for boundary comparisons. Our results complement those in our previous articles [arXiv1204.6613, arXiv:1305.5098].

Keywords

Cite

@article{arxiv.1306.5197,
  title  = {Maximum principles for boundary-degenerate linear parabolic differential operators},
  author = {Paul M. N. Feehan},
  journal= {arXiv preprint arXiv:1306.5197},
  year   = {2013}
}

Comments

34 pages, 2 figures. This article is the parabolic analogue of arXiv:1204.6613 and restates background material (definitions, notation, spaces) from arXiv:1305.5098

R2 v1 2026-06-22T00:38:15.873Z