40 research outputs found
A simple example of the weak discontinuity of
In this short note I construct a sequence of conformal diffeomorphisms
from the -dimensional unit ball to itself that converges weakly to a
constant in . This is a simpler example than the ones that commonly
appear in the literature for the discontinuity of the functional in the weak -topology, and shows that this
discontinuity is not due to shear or failure of injectivity. It is also a
minimizing sequence of the norm among functions of a given volume of
the image
Cooperation under Incomplete Information on the Discount Factors
In the repeated Prisoner's Dilemma, when every player has a different
discount factor, the grim-trigger strategy is an equilibrium if and only if the
discount factor of each player is higher than some threshold. What happens if
the players have incomplete information regarding the discount factors? In this
work we look at repeated games in which each player has incomplete information
regarding the other player's discount factor, and ask when a pair of
grim-trigger strategies is an equilibrium. We provide necessary and sufficient
conditions for such strategies to be an equilibrium. We characterize the states
of the world in which the strategies are not triggered, i.e., the players
cooperate, in such equilibria (or -equilibria), and ask whether these
"cooperation events" are close to those in the complete information case, when
the information is "almost" complete, in several senses.Comment: Thesis submitted in partial fulfillment of requirements for the M.
Sc. degree in the School of Mathematical Sciences, Tel-Aviv University. The
research work for this thesis has been carried out at Tel-Aviv University
under the supervision of Prof. Eilon Sola
Limits of elastic models of converging Riemannian manifolds
In non-linear incompatible elasticity, the configurations are maps from a
non-Euclidean body manifold into the ambient Euclidean space, .
We prove the -convergence of elastic energies for configurations of a
converging sequence, , of body manifolds. This
convergence result has several implications: (i) It can be viewed as a general
structural stability property of the elastic model. (ii) It applies to certain
classes of bodies with defects, and in particular, to the limit of bodies with
increasingly dense edge-dislocations. (iii) It applies to approximation of
elastic bodies by piecewise-affine manifolds. In the context of
continuously-distributed dislocations, it reveals that the torsion field, which
has been used traditionally to quantify the density of dislocations, is
immaterial in the limiting elastic model
A Riemannian approach to the membrane limit in non-Euclidean elasticity
Non-Euclidean, or incompatible elasticity is an elastic theory for
pre-stressed materials, which is based on a modeling of the elastic body as a
Riemannian manifold. In this paper we derive a dimensionally-reduced model of
the so-called membrane limit of a thin incompatible body. By generalizing
classical dimension reduction techniques to the Riemannian setting, we are able
to prove a general theorem that applies to an elastic body of arbitrary
dimension, arbitrary slender dimension, and arbitrary metric. The limiting
model implies the minimization of an integral functional defined over
immersions of a limiting submanifold in Euclidean space. The limiting energy
only depends on the first derivative of the immersion, and for
frame-indifferent models, only on the resulting pullback metric induced on the
submanifold, i.e., there are no bending contributions
Cooperation under Incomplete Information on the Discount Factors
In repeated games, cooperation is possible in equilibrium only if players are
sufficiently patient, and long-term gains from cooperation outweigh short-term
gains from deviation. What happens if the players have incomplete information
regarding each other's discount factors? In this paper we look at repeated
games in which each player has incomplete information regarding the other
player's discount factor, and ask when full cooperation can arise in
equilibrium. We provide necessary and sufficient conditions that allow full
cooperation in equilibrium that is composed of grim trigger strategies, and
characterize the states of the world in which full cooperation occurs. We then
ask whether these "cooperation events" are close to those in the complete
information case, when the information on the other player's discount factor is
"almost" complete.Comment: appears in International Journal of Game Theory, 201
Variational Convergence of Discrete Geometrically-Incompatible Elastic Models
We derive a continuum model for incompatible elasticity as a variational
limit of a family of discrete nearest-neighbor elastic models. The discrete
models are based on discretizations of a smooth Riemannian manifold
, endowed with a flat, symmetric connection . The
metric determines local equilibrium distances between
neighboring points; the connection induces a lattice structure shared
by all the discrete models. The limit model satisfies a fundamental rigidity
property: there are no stress-free configurations, unless is
flat, i.e., has zero Riemann curvature. Our analysis focuses on two-dimensional
systems, however, all our results readily generalize to higher dimensions.Comment: v3: a more concise version (similar to the published version); proof
of Proposition 4.4 corrected, Lemma A.4 adde
Riemannian surfaces with torsion as homogenization limits of locally-Euclidean surfaces with dislocation-type singularities
We reconcile between two classical models of edge-dislocations in solids. The
first model, dating from the early 1900s models isolated edge-dislocations as
line singularities in locally-Euclidean manifolds. The second model, dating
from the 1950s, models continuously-distributed edge-dislocations as smooth
manifolds endowed with non-symmetric affine connections (equivalently, endowed
with torsion fields). In both models, the solid is modeled as a Weitzenb\"ock
manifold. We prove, using a weak notion of convergence [KM15], that the second
model can be obtained rigorously as a homogenization limit of the first model,
as the density of singular edge-dislocation tends to infinity
On the role of curvature in the elastic energy of non-Euclidean thin bodies
We prove a relation between the scaling of the elastic energies of
shrinking non-Euclidean bodies of thickness , and the curvature
along their mid-surface . This extends and generalizes similar results for
plates [BLS16, LRR] to any dimension and co-dimension. In particular, it proves
that the natural scaling for non-Euclidean rods with smooth metric is , as
claimed in [AAE+12] using a formal asymptotic expansion. The proof involves
calculating the -limit for the elastic energies of small balls
, scaled by , and showing that the limit infimum energy is given
by a square of a norm of the curvature at a point . This -limit
proves asymptotics calculated in [AKM+16]
The emergence of torsion in the continuum limit of distributed edge-dislocations
We present a rigorous homogenization theorem for distributed dislocations. We
construct a sequence of locally-flat Riemannian manifolds with dislocation-type
singularities. We show that this sequence converges, as the dislocations become
denser, to a flat non-singular Weitzenb\"ock manifold, i.e. a flat manifold
endowed with a metrically-consistent connection with zero curvature and
non-zero torsion. In the process, we introduce a new notion of convergence of
Weitzenb\"ock manifolds, which is relevant to this class of homogenization
problems.Comment: See an erratum regarding Definition 4.1 and Lemma 4.8 in
arxiv:1701.08903 (v3 is the same as v2 but for this comment
Vanishing geodesic distance for right-invariant Sobolev metrics on diffeomorphism groups
We study the geodesic distance induced by right-invariant metrics on the
group of compactly supported diffeomorphisms,
for various Sobolev norms . Our main result is that the geodesic
distance vanishes identically on every connected component whenever
, where is the dimension of . We also show that
previous results imply that whenever or , the geodesic
distance is always positive. In particular, when , the geodesic
distance vanishes if and only if in the Riemannian case , contrary
to a conjecture made in Bauer et al. [BBHM13].Comment: Version 2: some changes in presentation of the paper, no mathematical
changes. Now includes a link to some related videos in
http://www.math.toronto.edu/rjerrard/geo_dist_diffeo/vanishing.htm