1998
DOI: 10.1007/bf02498215
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Balls and quasi-metrics: A space of homogeneous type modeling the real analysis related to the Monge-Ampère equation

Abstract: We prove that having a quasi-metric on a given set X is essentially equivalent to have a family of subsets S(x, r) of X for which y ~ S(x, r) implies both ,..q(y, r) C S(x, Kr) and S(x, r) C S(y, Kr) for some constant K. As an application, starting from the Monge-Ampbre setting introduced in [3], we get a space of homogeneous type modeling the real analysis for such an equation.

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Cited by 39 publications
(44 citation statements)
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“…The properties (A) and (B) of the sections imply the following engulfing property proved in [1]: there exists a constant θ > 1, depending only on K 1 and 1 , such that for y ∈ S(x, r) we have (D) S(y, r) ⊂ S(x, θr) and S(x, r) ⊂ S(y, θr).…”
Section: Preliminary Resultsmentioning
confidence: 82%
“…The properties (A) and (B) of the sections imply the following engulfing property proved in [1]: there exists a constant θ > 1, depending only on K 1 and 1 , such that for y ∈ S(x, r) we have (D) S(y, r) ⊂ S(x, θr) and S(x, r) ⊂ S(y, θr).…”
Section: Preliminary Resultsmentioning
confidence: 82%
“…This result was proved by H. Aimar, L. Forzani, and R. Toledano in [1] under the assumption of several geometric conditions on the sections of ϕ, which, later on, turned out to be equivalent to the (DC)-doubling condition, (see Theorem 8 in [12]). Conversely, if Eq.…”
Section: Real Analysis Associated To the Monge-ampère Equationmentioning
confidence: 82%
“…To prove that the distributional Hessian D 2 D u of an Alexandrov solution is a L 1 function, it is enough to prove an a priori equi-integrability estimate on smooth solutions. 5 To do this, a key observation is that any domain Ω endowed with the Lebesgue measure and the family of "balls" given by the sections {S(x, p, t)} x∈Ω, t∈R of solutions of (2.6) as defined in (2.22) is a space homogenous type in the sense of Coifman and Weiss, see [25,68,1]. In particular Stein's Theorem implies that if…”
Section: 4mentioning
confidence: 99%
“…It says that if we take the function ψx ,y 0 ,y 1 = max −c(·, y 0 ) + c(x, y 0 ), −c(·, y 1 ) + c(x, y 1 ) , then we are able to touch the graph of this function from below atx with the family of functions {−c(·, y t ) + c(x, y t )} t∈ [0,1] . This suggests that we could use this family to regularize the cusp of ψx ,y 0 ,y 1 at the pointx, by slightly moving above the graphs of the functions −c(·, y t ) + c(x, y t ).…”
Section: 1mentioning
confidence: 99%