2012
DOI: 10.1090/s0033-569x-2012-01316-9
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On global minimizers for a variational problem with long-range interactions

Abstract: Abstract. Energy-driven pattern formation induced by competing short and longrange interactions is common in many physical systems. In these proceedings we report on certain rigorous asymptotic results concerning global minimizers of a nonlocal perturbation to the well-known Ginzburg-Landau/Cahn-Hilliard free energy. We also discuss two hybrid numerical methods for accessing the ground states of these functionals.

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Cited by 14 publications
(10 citation statements)
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“…Importantly, the model in (1.1) is a paradigm for the energy-driven pattern forming systems in which spatial patterns (global or local energy minimizers) form as a result of the competition of short-range attractive and long-range repulsive forces. This is why this model and its generalizations attracted considerable attention of mathematicians in recent years (see, e.g., [31][32][33][34][35][36][37][38][39][40][41][42][43][44][45][46][47][48][49], this list is certainly not exhaustive). In particular, the volume-constrained global minimization problem for (1.1) in the whole space with no neutralizing background, which we will also refer to as the "self-energy problem", has been investigated in [34,37,45,49].…”
Section: -3mentioning
confidence: 99%
See 1 more Smart Citation
“…Importantly, the model in (1.1) is a paradigm for the energy-driven pattern forming systems in which spatial patterns (global or local energy minimizers) form as a result of the competition of short-range attractive and long-range repulsive forces. This is why this model and its generalizations attracted considerable attention of mathematicians in recent years (see, e.g., [31][32][33][34][35][36][37][38][39][40][41][42][43][44][45][46][47][48][49], this list is certainly not exhaustive). In particular, the volume-constrained global minimization problem for (1.1) in the whole space with no neutralizing background, which we will also refer to as the "self-energy problem", has been investigated in [34,37,45,49].…”
Section: -3mentioning
confidence: 99%
“…From (5.42), (5.44) and (5.45) we then get 46) for ε small enough. Letting nowû ε (x) :=ũ ε (ε 1/3 x) be the rescaled function which satisfies 47) for every fixed ρ 0 > 0 and ε sufficiently small, we get 48) where Γ ρ 0 is defined via (5.21). Recalling Corollary 4.6 and choosing ρ 0 ≥ R 1 , we obtain 49) which gives (5.40) by first letting ρ → 0 and then δ → δ.…”
Section: Equidistribution Of Energymentioning
confidence: 99%
“…The sharp interface functional (1.3) has recently received attention from many authors; see, for example, [1,4,5,7,8,12,23,30]. It is a natural extension of the isoperimetric problem.…”
Section: Introductionmentioning
confidence: 99%
“…It to be pointed out is that the two fields in this description do not stand for cell types themselves, but any cell type can be described as a suitable linear combination of the two fields. The phase field literature is replete with formulations that model more complex structures (Choksi, 2012), including lipid bilayers (Dai and Promislow, 2013) and tubular structures (Kraitzman and Promislow, 2015). Rather than review those works this perspective has chosen to dwell on a few broader observations.…”
Section: Discussionmentioning
confidence: 99%