Abstract

We develop a method to study the structure of the common part of the boundaries of disjoint and possibly non-complementary time-varying domains in Rn+1, n≥2, at the points of mutual absolute continuity of their respective caloric measures. Our set of techniques, which is based on parabolic tangent measures, allows us to tackle the following problems:1.Let Ω1 and Ω2 be disjoint domains in Rn+1, n≥2, which are quasi-regular for the heat equation and regular for the adjoint heat equation, and their complements satisfy a mild non-degeneracy hypothesis on the set E⊂∂Ω1∩∂Ω2 of mutual absolute continuity of the associated caloric measures ωi with poles at p¯i=(pi,ti)∈Ωi, i=1,2. Then, we obtain a parabolic analogue of the results of Kenig, Preiss, and Toro, i.e., we show that the parabolic Hausdorff dimension of ω1|E is n+1 and the tangent measures of ω1 at ω1-a.e. point of E are equal to a constant multiple of the parabolic (n+1)-Hausdorff measure restricted to hyperplanes containing a line parallel to the time-axis.2.If, additionally, ω1|E and ω2|E are doubling, log⁡dω2|Edω1|E∈VMO(ω1|E), and E is relatively open in the support of ω1, then their tangent measures at every point of E are caloric measures associated with adjoint caloric polynomials. As a corollary we obtain that if Ω1 is a δ-Reifenberg flat domain for δ small enough and Ω2=Rn+1∖Ω‾1, and log⁡dω2dω1∈VMO(ω1), then Ω1∩{t<t2} is vanishing Reifenberg flat. This generalizes results of Kenig and Toro for the Laplacian.3.Finally, we establish a parabolic version of a theorem of Tsirelson about triple-points for harmonic measure. Assuming that Ωi, 1≤i≤3, are quasi-regular domains for both the heat and the adjoint heat equations, the set of points on ∩i=13∂Ωi, where the three caloric measures are mutually absolutely continuous has null caloric measure. In the course of proving our main theorems, we obtain new results on heat potential theory, parabolic geometric measure theory, nodal sets of caloric functions, and Optimal Transport, that may be of independent interest.

Highlights

  • In this paper, we study two-phase problems for harmonic measure associated with the heat equation, which is traditionally called caloric measure

  • I.e., we show that the parabolic Hausdorff dimension of ω1|E is n + 1 and the tangent measures of ω1 at ω1-a.e. point of E are equal to a constant multiple of the parabolic (n + 1)-Hausdorff measure restricted to hyperplanes containing a line parallel to the time-axis

  • We study two-phase problems for harmonic measure associated with the heat equation, which is traditionally called caloric measure

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Summary

INTRODUCTION

We study two-phase problems for harmonic measure associated with the heat equation, which is traditionally called caloric measure. In the case of harmonic and elliptic measures, it has been proved in [AMTV19, Lemma 5.3] and [AM19, Lemma 4.13] that mutual absolute continuity of the interior and the exterior measures implies an even stronger version of (1.3) in terms of the (n + 1)dimensional Lebesgue measure of euclidean balls This method, is based on a dichotomy argument and cannot be generalized directly to the caloric measure because it is not enough to obtain that the exterior of the domain is “large” in a sequence of parabolic balls; we need to know that this is true in a sequence of time-backwards cylinders, which complicates things significantly. We prove that at sufficiently small scales, the support of ω+ resembles the zero set of an adjoint caloric polynomial uniformly on compact subsets of the set of mutual absolute continuity This assertion can be formulated both in terms of Θ∂PΩΣ±(d) and the functional d1(·, P(d)), which is essentially a distance between measures and the set P(d) (see (4.4) for the exact definition).

PRELIMINARIES AND NOTATION
HEAT POTENTIAL THEORY AND PDE ESTIMATES
HAUSDORFF AND TANGENT MEASURES
NODAL SET OF CALORIC FUNCTIONS
CALORIC MEASURE ASSOCIATED WITH A CALORIC FUNCTION
CALORIC POLYNOMIAL MEASURES
ELEMENTS OF THE THEORY OF OPTIMAL TRANSPORT
BLOW-UPS IN TIME VARYING DOMAINS
10. PROOFS OF THE MAIN THEOREMS
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