98 research outputs found
The Spectrum of an Adelic Markov Operator
With the help of the representation of SL(2,Z) on the rank two free module
over the integer adeles, we define the transition operator of a Markov chain.
The real component of its spectrum exhibits a gap, whereas the non-real
component forms a circle of radius 1/\sqrt{2}.Comment: 38 pages, 5 figure
Elastic Scattering of Point Particles With Nearly Equal Masses
We show that for n billiard particles on the line there exist three open sets
in the product of phase space and the space of their masses, such that these
particles exhibit exactly n-1, n over 2 respectively n+1 over 3 collisions.
These open sets intersect any neighborhood of the diagonal in mass space.Comment: 9 pages, 1 figur
Quantum Transport on KAM Tori
Although quantum tunneling between phase space tori occurs, it is suppressed
in the semiclassical limit for the Schr\"{o}dinger equation
of a particle in \bR^d under the influence of a smooth periodic potential.
In particular this implies that the distribution of quantum group velocities
near energy converges to the distribution of the classical asymptotic
velocities near , up to a term of the order \cO(1/\sqrt{E}).Comment: 21 page
Symbolic Dynamics of Magnetic Bumps
For n convex magnetic bumps in the plane, whose boundary has a curvature
somewhat smaller than the absolute value of the constant magnetic field inside
the bump, we construct a complete symbolic dynamics of a classical particle
moving with speed one.Comment: 11 pages, 4 figure
On the integrability of the n-centre problem
It is known that for centres and positive energies the -centre
problem of celestial mechanics leads to a flow with a strange repellor and
positive topological entropy.
Here we consider the energies above some threshold and show: Whereas for
arbitrary independent integrals of Gevrey class exist, no
real-analytic (that is, Gevrey class 1) independent integral exists.Comment: 22 pages, a short announcement see in math.DS/031242
Semiclassical resolvent estimates for Schroedinger operators with Coulomb singularities
Consider the Schroedinger operator with semiclassical parameter h, in the
limit where h goes to zero. When the involved long-range potential is smooth,
it is well known that the boundary values of the operator's resolvent at a
positive energy E are bounded by O(1/h) if and only if the associated Hamilton
flow is non-trapping at energy E. In the present paper, we extend this result
to the case where the potential may possess Coulomb singularities. Since the
Hamilton flow then is not complete in general, our analysis requires the use of
an appropriate regularization.Comment: 39 pages, no figures, corrected versio
Stochastically Stable Quenched Measures
We analyze a class of stochastically stable quenched measures. We prove that
stochastic stability is fully characterized by an infinite family of zero
average polynomials in the covariance matrix entries.Comment: 13 page
Lagrangian Relations and Linear Point Billiards
Motivated by the high-energy limit of the -body problem we construct
non-deterministic billiard process. The billiard table is the complement of a
finite collection of linear subspaces within a Euclidean vector space. A
trajectory is a constant speed polygonal curve with vertices on the subspaces
and change of direction upon hitting a subspace governed by `conservation of
momentum' (mirror reflection). The itinerary of a trajectory is the list of
subspaces it hits, in order. Two basic questions are: (A) Are itineraries
finite? (B) What is the structure of the space of all trajectories having a
fixed itinerary? In a beautiful series of papers Burago-Ferleger-Kononenko
[BFK] answered (A) affirmatively by using non-smooth metric geometry ideas and
the notion of a Hadamard space. We answer (B) by proving that this space of
trajectories is diffeomorphic to a Lagrangian relation on the space of lines in
the Euclidean space. Our methods combine those of BFK with the notion of a
generating family for a Lagrangian relation.Comment: 29 pages, 4 figure
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