2016
DOI: 10.1016/j.na.2016.02.027
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Extension properties and boundary estimates for a fractional heat operator

Abstract: Abstract. The square root of the heat operator √ ∂ t − ∆, can be realized as the Dirichlet to Neumann map of the heat extension of data on R n+1 to R n+2 + . In this note we obtain similar characterizations for general fractional powers of the heat operator, (∂ t − ∆) s , s ∈ (0, 1). Using the characterizations we derive properties and boundary estimates for parabolic integro-differential equations from purely local arguments in the extension problem.2000 Mathematics Subject Classification.

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Cited by 54 publications
(55 citation statements)
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“…This is the so-called extension operator for the fractional powers (∂ t − x ) s , 0 < s < 1, of the heat operator. It was recently introduced independently by Nyström-Sande in [24], and Stinga-Torrea in [27]. These authors proved that, if for a given u ∈ S (R n+1 ), the function U solves the problem…”
Section: Notations and Preliminariesmentioning
confidence: 99%
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“…This is the so-called extension operator for the fractional powers (∂ t − x ) s , 0 < s < 1, of the heat operator. It was recently introduced independently by Nyström-Sande in [24], and Stinga-Torrea in [27]. These authors proved that, if for a given u ∈ S (R n+1 ), the function U solves the problem…”
Section: Notations and Preliminariesmentioning
confidence: 99%
“…The passage from (1.2) to (1.1) rests on the extension procedure for the operator (∂ t − x ) s , developed independently by Nyström and Sande in [24] and by Stinga and Torrea in [27]. Such result represents the parabolic counterpart of the famous Caffarelli and Silvestre's extension work [9].…”
Section: Introductionmentioning
confidence: 99%
“…It was recently introduced independently by Nyström-Sande in [46], and Stinga-Torrea in [57]. These authors proved that if for a given ϕ ∈ S (R n+1 ), the function u solves the problem…”
Section: A Sharp Harnack Inequality For the Parabolic Extension Problemmentioning
confidence: 99%
“…In more recent years Stinga and Torrea have generalized the extension procedure to different classes of operators, including uniformly elliptic operators in divergence form L = div(A(x)∇), see [57], or the heat operator H = ∂ ∂t − ∆ x , see [58]. This latter result was also established simultaneously and independently by Nyström and Sande in [46].…”
mentioning
confidence: 91%
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