Skip to Main Content

Journal of the American Mathematical Society

Published by the American Mathematical Society, the Journal of the American Mathematical Society (JAMS) is devoted to research articles of the highest quality in all areas of pure and applied mathematics.

ISSN 1088-6834 (online) ISSN 0894-0347 (print)

The 2020 MCQ for Journal of the American Mathematical Society is 4.79.

What is MCQ? The Mathematical Citation Quotient (MCQ) measures journal impact by looking at citations over a five-year period. Subscribers to MathSciNet may click through for more detailed information.

 

Uniform energy distribution for an isoperimetric problem with long-range interactions
HTML articles powered by AMS MathViewer

by Giovanni Alberti, Rustum Choksi and Felix Otto PDF
J. Amer. Math. Soc. 22 (2009), 569-605 Request permission

Abstract:

We study minimizers of a nonlocal variational problem. The problem is a mathematical paradigm for the ubiquitous phenomenon of energy-driven pattern formation induced by competing short- and long-range interactions. The short-range interaction is attractive and comes from an interfacial energy, and the long-range interaction is repulsive and comes from a nonlocal energy contribution. In particular, the problem is the sharp interface version of a problem used to model microphase separation of diblock copolymers. A natural conjecture is that in all space dimensions, minimizers are essentially periodic on an intrinsic scale. However, proving any periodicity result turns out to be a formidable task in dimensions larger than one.

In this paper, we address a weaker statement concerning the distribution of energy for minimizers. We prove in any space dimension that each component of the energy (interfacial and nonlocal) of any minimizer is uniformly distributed on cubes which are sufficiently large with respect to the intrinsic length scale. Moreover, we also prove an $L^\infty$ bound on the optimal potential associated with the long-range interactions. This bound allows for an interesting interpretation: Note that the average volume fraction of the optimal pattern in a subsystem of size $R$ fluctuates around the system average $m$. The bound on the potential yields a rate of decay of these fluctuations as $R$ tends to $+\infty$. This rate of decay is stronger than the one for a random checkerboard pattern. In this sense, the optimal pattern has less large-scale variations of the average volume fraction than a pattern with a finite correlation length.

References
Similar Articles
Additional Information
  • Giovanni Alberti
  • Affiliation: Dipartimento di Matematica, Università di Pisa, largo Pontecorvo 5, 56127 Pisa, Italy
  • Email: galberti1@dm.unipi.it
  • Rustum Choksi
  • Affiliation: Department of Mathematics, Simon Fraser University, 8888 University Drive, Burnaby, BC V5A 1S6 Canada
  • MR Author ID: 604242
  • Email: choksi@math.sfu.ca
  • Felix Otto
  • Affiliation: Institute for Applied Mathematics, Universität Bonn, Wegelerstr 10, D-53115 Bonn, Germany
  • Email: otto@iam.uni-bonn.de
  • Received by editor(s): October 16, 2007
  • Published electronically: November 6, 2008
  • © Copyright 2008 American Mathematical Society
    The copyright for this article reverts to public domain 28 years after publication.
  • Journal: J. Amer. Math. Soc. 22 (2009), 569-605
  • MSC (2000): Primary 49Q10, 49N60, 49S05, 35B10
  • DOI: https://doi.org/10.1090/S0894-0347-08-00622-X
  • MathSciNet review: 2476783