2018
DOI: 10.4171/rmi/1003
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The Dirichlet boundary problem for second order parabolic operators satisfying a Carleson condition

Abstract: We establish L p , 2 ≤ p ≤ ∞ solvability of the Dirichlet boundary value problem for a parabolic equation ut − div(A∇u) − B · ∇u = 0 on time-varying domains with coefficient matrices A = [a ij ] and B = [b i ] that satisfy a small Carleson condition. The results are sharp in the following sense. For a given value of 1 < p < ∞ there exists operators that satisfy Carleson condition but fail to have L p solvability of the Dirichlet problem. Thus the assumption of smallness is sharp. Our results complements result… Show more

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Cited by 15 publications
(34 citation statements)
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“…We state a version of the maximum principle from [DH16] that is a modification of Lemma 3.38 from [HL01].…”
Section: Basic Results and Interior Estimatesmentioning
confidence: 99%
See 2 more Smart Citations
“…We state a version of the maximum principle from [DH16] that is a modification of Lemma 3.38 from [HL01].…”
Section: Basic Results and Interior Estimatesmentioning
confidence: 99%
“…In particular in this paper the authors has solved the L 2 Dirichlet problem for the heat equation in graph domains of Lewis-Murray type. A related class of localised domains in which parabolic boundary value problems are solvable was considered in [Riv14] as well as in [DH16,DPP16]. The paper [DH16] has established L p solvability for parabolic Dirichlet problem under assumption that the coefficients satisfy certain natural small Carleson condition which also appears for elliptic PDEs.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…As in [9], the results here are formulated for the class of admissible parabolic domains, which are, in effect, bounded time-varying domains that are "locally" of Lewis-Murray type. A related, but smaller, class of localized domains in which parabolic boundary value problems are solvable was considered in [31].…”
Section: Introductionmentioning
confidence: 99%
“…It is a fact that the parabolic PDE (2.12) with continuous boundary data is uniquely solvable (c.f. discussion under Definition 2.7 in [9]) and that there exists a a measure ω (X,t) such that (1.3) u(X, t) = ∂Ω f (y, s)dω (X,t) (y, s) for all continuous data, called the parabolic measure. Under the assumption of Definition 2.2, this measure is doubling (c.f.…”
Section: Introductionmentioning
confidence: 99%