The talk will review some elementary, but amusing, results concerning
surface spectra for discrete Laplacians on half-planes with a boundary.In particular, interesting differences arise for square lattices with
straight boundaries between the case where the boundary has the same
direction of the lattice and the one where the boundary is slanted
at an angle of 45 degrees to the direction of the lattice. This
is joint work with Y. Kreimer.
Consider a quasi-periodic Schr\"odinger operator
$H_{\alpha,\theta}$ with analytic potential and Diophantine frequency
$\alpha$. Given any rational approximating $\alpha$, let $S_+$ and $S_-$
denote the union, respectively, the intersection of the spectra taken over
$\theta$. We show that up to sets of zero Lebesgue measure, the absolutely
continuous spectrum can be obtained asymptotically from $S_-$ of the
periodic operators associated with the continued fraction expansion of
$\alpha$. Similarly, from the asymptotics of $S_+$, one recovers the
spectrum of $H_{\alpha,\theta}$ (modulo a set of zero Lebesgue measure).
I will review recent work linking quantum dynamical estimates
and rates of mixing in fluid flow. The main result is a sharp classification
of stationary or time periodic flows that are particularly efficient mixers.
I will also formulate some open questions.
Since the discovery of quasicrystals by Schechtman et. al.
in 1984, quasi-periodic models in mathematical physics have formed an
active area of research. In particular, effects of quasi-periodicity
were investigated in a widely studied model of magnetism: the Ising
model (quantum and classical). Numerical and some analytic results
began to appear in the late '80s; however, most interesting
(numerical) results hitherto remained rigorously unconfirmed.Most of
the previous results relied on a connection with hyperbolic dynamical
systems.It is our aim to rigorously confirm previous numerical
observations, as well as to prove new results, by exploiting further
the aforementioned connection. In particular, we'll prove
multi-fractal structure of the energy spectrum of one-dimensional
quantum quasi-periodic Ising models. We'll also discuss its fractal
dimensions and measure.
The Ten Martini problem asked to show that the spectrum
of the Almost-Mathieu operator, that is, a Schroedinger operator with potential V (n) = 2 cos(2 pi alpha n), is a Cantor set. In particular, this means that the spectrum does not contain any intervals. The Ten Martini problem was solved in 2009 by Avila and Jitomirskaya. I will show that such a claim is false for the generalization to the potential V(n) =2 cos(2 pi alpha n^2), which is known as skew-shift Schroedinger operator. The proof relies on localization properties of this operator and that the phase space of the skew-shift is two dimensional, whereas it is one dimensional for the rotations underlying the Almost-Mathieu operator.