2011
DOI: 10.1512/iumj.2011.60.4322
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Viscosity solutions for a polymer crystal growth model

Abstract: We prove existence of a solution for a polymer crystal growth model describing the movement of a front (Γ(t)) evolving with a nonlocal velocity. In this model the nonlocal velocity is linked to the solution of a heat equation with source δΓ. The proof relies on new regularity results for the eikonal equation, in which the velocity is positive but merely measurable in time and with Hölder bounds in space. From this result, we deduce a priori regularity for the front. On the other hand, under this regularity ass… Show more

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Cited by 2 publications
(3 citation statements)
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“…It improves the estimate for the length of trajectory from Su and Burger's l C O.l˛/ to its optimal l C O.l 1C2ˇ/ . Similar estimate has also been established in [8] with Hölder exponent2 under a different setting. The most significant application of this new estimate is that it allows us to construct efficiently comparison particle motion paths to show that .s/ near x .s/ is sandwiched between two C 1C˛=2 graphs touching at x .s/, for each s 2 .0; t/; technically, writing p D x .s/ and n D n .s/, we can prove the following inclusions: where C D C .n; c;˛/ is a constant depending only on n; c and˛.…”
Section: Introductionsupporting
confidence: 75%
See 1 more Smart Citation
“…It improves the estimate for the length of trajectory from Su and Burger's l C O.l˛/ to its optimal l C O.l 1C2ˇ/ . Similar estimate has also been established in [8] with Hölder exponent2 under a different setting. The most significant application of this new estimate is that it allows us to construct efficiently comparison particle motion paths to show that .s/ near x .s/ is sandwiched between two C 1C˛=2 graphs touching at x .s/, for each s 2 .0; t/; technically, writing p D x .s/ and n D n .s/, we can prove the following inclusions: where C D C .n; c;˛/ is a constant depending only on n; c and˛.…”
Section: Introductionsupporting
confidence: 75%
“…Their methods of proof, based on an interior sphere property of the attainable sets, are totally different from ours, and they also require somewhat stronger condition on expanding speed and initial shape. Recently, similar regularity results have also been obtained by Cardaliaguet, Ley and Mointeiliet [8] where in addition to the Hölder continuity of the expanding speed, they needed stronger condition jv.x; t/ v.y; t/j 6 C jy xj.1 C j ln jx yjj/:…”
Section: Introductionsupporting
confidence: 70%
“…An essential step of the analysis is the C 1,α -regularity of the extremal trajectories of (2), see Theorem 4.1. For time-dependent and isotropic Hamiltonians (H = a(t, x)|p|), such a regularity property-interesting in its own right-has already been observed in [2] for N = 2, and [6] for general N . However, the unexpected connection between Theorem 4.1 and the semiconcavity of the solution of ( 1) is, to our best knowledge, entirely new.…”
Section: Introductionmentioning
confidence: 83%