Perturbations of local maxima and comparison principles for boundary-degenerate linear differential equations

preprint2020arXivOpen access

Abstract

We develop strong and weak maximum principles for boundary-degenerate elliptic and parabolic linear second-order partial differential operators, Au:=−tr(aD2u)−<b,Du>+cuAu := -\mathrm{tr}(aD^2u)-<b, Du> + cu, with partial Dirichlet boundary conditions. The coefficient, a(x)a(x), is assumed to vanish along a non-empty open subset, ∂0O\partial_0\mathscr{O}, called the \emph{degenerate boundary portion}, of the boundary, ∂O\partial\mathscr{O}, of the domain O⊂Rd\mathscr{O}\subset\mathbb{R}^d, while a(x)a(x) is non-zero at any point of the \emph{non-degenerate boundary portion}, ∂1O:=∂O∖∂0O‾\partial_1\mathscr{O} := \partial\mathscr{O}\setminus\overline{\partial_0\mathscr{O}}. If an AA-subharmonic function, uu in C2(O)C^2(\mathscr{O}) or Wloc2,d(O)W^{2,d}_{\mathrm{loc}}(\mathscr{O}), is C1C^1 up to ∂0O\partial_0\mathscr{O} and has a strict local maximum at a point in ∂0O\partial_0\mathscr{O}, we show that uu can be perturbed, by the addition of a suitable function w∈C2(O)∩C1(Rd)w\in C^2(\mathscr{O})\cap C^1(\mathbb{R}^d), to a strictly AA-subharmonic function v=u+wv=u+w having a local maximum in the interior of O\mathscr{O}. Consequently, we obtain strong and weak maximum principles for AA-subharmonic functions in C2(O)C^2(\mathscr{O}) and Wloc2,d(O)W^{2,d}_{\mathrm{loc}}(\mathscr{O}) which are C1C^1 up to ∂0O\partial_0\mathscr{O}. Only the non-degenerate boundary portion, ∂1O\partial_1\mathscr{O}, is required for boundary comparisons. Our results extend those in Daskalopoulos and Hamilton (1998), Epstein and Mazzeo [arXiv:1110.0032], and the author [arXiv:1204.6613, 1306.5197], where tr(aD2u)\mathrm{tr}(aD^2u) is in addition assumed to be continuous up to and vanish along ∂0O\partial_0\mathscr{O} in order to yield comparable maximum principles for AA-subharmonic functions in C2(O)C^2(\mathscr{O}), while the results developed here for AA-subharmonic functions in Wloc2,d(O)W^{2,d}_{\mathrm{loc}}(\mathscr{O}) are entirely new.

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