2015
DOI: 10.1007/s10231-015-0481-3
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The boundary Harnack inequality for variable exponent $$p$$ p -Laplacian, Carleson estimates, barrier functions and $${p(\cdot )}$$ p ( · ) -harmonic measures

Abstract: We investigate various boundary decay estimates for p(·)-harmonic functions. For domains in R n , n ≥ 2 satisfying the ball condition (C 1,1 -domains), we show the boundary Harnack inequality for p(·)-harmonic functions under the assumption that the variable exponent p is a bounded Lipschitz function. The proof involves barrier functions and chaining arguments. Moreover, we prove a Carleson-type estimate for p(·)-harmonic functions in NTA domains in R n and provide lower and upper growth estimates and a doubli… Show more

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Cited by 11 publications
(27 citation statements)
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“…Indeed, we conclude that solutions must vanish at the same rate as |x| k(v,p) as x approaches the apex (Corollary 5.1). Similar growth estimates where proved in the setting of C 1,1 -domains in [8] and for wider classes of equations and other geometric settings in [37,38,39,45,46,5,48]. An immediate consequence of Corollary 5.1 is the boundary Harnack inequality for p-harmonic functions in planar sectors, see (5.5).…”
Section: Introductionsupporting
confidence: 58%
“…Indeed, we conclude that solutions must vanish at the same rate as |x| k(v,p) as x approaches the apex (Corollary 5.1). Similar growth estimates where proved in the setting of C 1,1 -domains in [8] and for wider classes of equations and other geometric settings in [37,38,39,45,46,5,48]. An immediate consequence of Corollary 5.1 is the boundary Harnack inequality for p-harmonic functions in planar sectors, see (5.5).…”
Section: Introductionsupporting
confidence: 58%
“…More specifically, our boundary estimate consists of a lower estimate (Theorem 5.1) and an upper estimate (Theorem 5.3) generalizing the main results of Adamowicz-Lundström [1] to viscosity solutions of more general PDEs. To prove the lower estimate we need a sligthly stronger structural assumption than above in order to build a positive barrier function (Lemma 3.2) and to this end we assume…”
Section: Introductionmentioning
confidence: 99%
“…For infinity-harmonic functions, see e.g. Bhattacharya [13], Lundström-Nyström [46] and for solutions to the variable exponent p-Laplace equation in smooth domains, see Adamowicz-Lundström [2]. Only few papers considered local estimates of positive p-harmonic functions vanishing near boundaries having dimension less than n − 1.…”
Section: Introductionmentioning
confidence: 99%