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Transactions of the American Mathematical Society

Published by the American Mathematical Society since 1900, Transactions of the American Mathematical Society is devoted to longer research articles in all areas of pure and applied mathematics.

ISSN 1088-6850 (online) ISSN 0002-9947 (print)

The 2020 MCQ for Transactions of the American Mathematical Society is 1.48.

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Geometric Sobolev-like embedding using high-dimensional Menger-like curvature
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by Sławomir Kolasiński PDF
Trans. Amer. Math. Soc. 367 (2015), 775-811 Request permission

Abstract:

We study a modified version of Lerman-Whitehouse Menger-like curvature defined for $(m+2)$ points in an $n$-dimensional Euclidean space. For $1 \le l \le m+2$ and an $m$-dimensional set $\Sigma \subset R^n$, we also introduce global versions of this discrete curvature by taking the supremum with respect to $(m+2-l)$ points on $\Sigma$. We then define geometric curvature energies by integrating one of the global Menger-like curvatures, raised to a certain power $p$, over all $l$-tuples of points on $\Sigma$. Next, we prove that if $\Sigma$ is compact and $m$-Ahlfors regular and if $p$ is greater than the dimension of the set of all $l$-tuples of points on $\Sigma$ (i.e. $p > ml$), then the P. Jones’ $\beta$-numbers of $\Sigma$ must decay as $r^{\tau }$ with $r \to 0$ for some $\tau \in (0,1)$. If $\Sigma$ is an immersed $C^1$ manifold or a bilipschitz image of such a set then, it follows that it is Reifenberg flat with vanishing constant; hence (by a theorem of David, Kenig and Toro) an embedded $C^{1,\tau }$ manifold. We also define a wide class of other sets for which this assertion is true. After that, we bootstrap the exponent $\tau$ to $\alpha = 1 - ml/p$, which is optimal due to our theorem with S. Blatt [Adv. Math., 2012]. This gives an analogue of the Morrey-Sobolev embedding theorem $W^{2,p}(\mathbb {R}^{ml}) \subseteq C^{1,\alpha }(\mathbb {R}^{ml})$ but, more importantly, we also obtain a qualitative control over the local graph representations of $\Sigma$ only in terms of the energy.
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Additional Information
  • Sławomir Kolasiński
  • Affiliation: Institute of Mathematics, University of Warsaw, Banacha 2, 02-097 Warsaw, Poland
  • Address at time of publication: Max Planck Institute for Gravitational Physics, Albert Einstein Institute, Am Mühlenberg 1, D-14476 Golm, Germany
  • Email: s.kolasinski@mimuw.edu.pl
  • Received by editor(s): May 24, 2012
  • Published electronically: July 24, 2014
  • Additional Notes: The major part of this work was accomplished while the author was working at the University of Warsaw and was supported by the Polish Ministry of Science grant no. N N201 611140. The work was put in its final form at the AEI Golm, AEI publication number AEI-2013-165
  • © Copyright 2014 American Mathematical Society
    The copyright for this article reverts to public domain 28 years after publication.
  • Journal: Trans. Amer. Math. Soc. 367 (2015), 775-811
  • MSC (2010): Primary 49Q10; Secondary 28A75, 49Q20, 49Q15
  • DOI: https://doi.org/10.1090/S0002-9947-2014-05989-8
  • MathSciNet review: 3280027