9 research outputs found
Cascade of minimizers for a nonlocal isoperimetric problem in thin domains
For \Omega_\e=(0,\e)\times (0,1) a thin rectangle, we consider minimization
of the two-dimensional nonlocal isoperimetric problem given by \inf_u
E^{\gamma}_{\Omega_\e}(u) where E^{\gamma}_{\Omega_\e}(u):=
P_{\Omega_\e}(\{u(x)=1\})+\gamma\int_{\Omega_\e}\abs{\nabla{v}}^2\,dx and
the minimization is taken over competitors u\in BV(\Omega_\e;\{\pm 1\})
satisfying a mass constraint \fint_{\Omega_\e}u=m for some .
Here P_{\Omega_\e}(\{u(x)=1\}) denotes the perimeter of the set
in \Omega_\e, \fint denotes the integral average and denotes the
solution to the Poisson problem -\Delta
v=u-m\;\mbox{in}\;\Omega_\e,\quad\nabla v\cdot
n_{\partial\Omega_\e}=0\;\mbox{on}\;\partial\Omega_\e,\quad\int_{\Omega_\e}v=0.
We show that a striped pattern is the minimizer for \e\ll 1 with the number
of stripes growing like as We then present
generalizations of this result to higher dimensions.Comment: 20 pages, 2 figure
Axisymmetric critical points of a nonlocal isoperimetric problem on the two-sphere
On the two dimensional sphere, we consider axisymmetric critical points of an
isoperimetric problem perturbed by a long-range interaction term. When the
parameter controlling the nonlocal term is sufficiently large, we prove the
existence of a local minimizer with arbitrary many interfaces in the
axisymmetric class of admissible functions. These local minimizers in this
restricted class are shown to be critical points in the broader sense (i.e.,
with respect to all perturbations). We then explore the rigidity, due to
curvature effects, in the criticality condition via several quantitative
results regarding the axisymmetric critical points.Comment: 26 pages, 6 figures. This version is to appear in ESAIM: Control,
Optimisation and Calculus of Variation
Sharp interface limit of an energy modelling nanoparticle-polymer blends
We identify the -limit of a nanoparticle-polymer model as the number
of particles goes to infinity and as the size of the particles and the phase
transition thickness of the polymer phases approach zero. The limiting energy
consists of two terms: the perimeter of the interface separating the phases and
a penalization term related to the density distribution of the infinitely many
small nanoparticles. We prove that local minimizers of the limiting energy
admit regular phase boundaries and derive necessary conditions of local
minimality via the first variation. Finally we discuss possible critical and
minimizing patterns in two dimensions and how these patterns vary from global
minimizers of the purely local isoperimetric problem.Comment: Minor changes. Rephrased introduction. This version is to appear in
Interfaces and Free Boundarie