2003
DOI: 10.14321/realanalexch.28.1.0235
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A Taylor Series Condition for Harmonic Extension

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Cited by 7 publications
(8 citation statements)
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“…Combining ( 12) and ( 13), provided h ≤ (2c) −1 we establish (9) with α = 1/3. Now let u H ∈ H 1 (Ω) be the solution of the Laplace equation ∆u H = 0 in Ω fulfilling u H = g on Γ.…”
Section: The Approximate Problemmentioning
confidence: 65%
See 1 more Smart Citation
“…Combining ( 12) and ( 13), provided h ≤ (2c) −1 we establish (9) with α = 1/3. Now let u H ∈ H 1 (Ω) be the solution of the Laplace equation ∆u H = 0 in Ω fulfilling u H = g on Γ.…”
Section: The Approximate Problemmentioning
confidence: 65%
“…Akin to problem (8) and thanks to (9), problem (92) has a unique solution. This fact allows us to claim the following preliminary result:…”
Section: The Case Of Non-convex Domainsmentioning
confidence: 99%
“…Even if we go the other around by prescribing a regular f in trueΩ, the existence of an associated trueu fulfilling the assumptions of Theorem 4.5 can be questioned. However using results in [9] combined with standard ones (cf. [13]) it is possible to identify cases where such an extension trueu does exist.…”
Section: Error Estimatesmentioning
confidence: 99%
“…Let r 0 be the radius of the largest (open) ball B contained in Ω and O = (x 0 , y 0 ) be its center. Assuming that the extension of f is not too wild in Ω so that the Taylor series of u H (x, y 0 ) and [∂u H /∂y](x, y 0 ) centered at O converge in the segment of the line y = y 0 centered at O with length equal to r 0 √ 2r 0 + 2δ for a certain δ > 0, according to [9] there exists a harmonic extension u H of u H to the ball B 0 centered at O with radius r 0 + δ √ 2. Clearly in this case, as long as δ is large enough for B to contain Ω, we can define ũ := u 0 − u H as a function in H k+1 ( Ω) that vanishes on Γ, and thus satisfies all the required properties.…”
Section: Error Estimatesmentioning
confidence: 99%