133 research outputs found
Analyticity of extremisers to the Airy Strichartz inequality
We prove that there exists an extremal function to the Airy Strichartz
inequality, by
using the linear profile decomposition. Furthermore we show that, if is an
extremiser, then is extremely fast decaying in Fourier space and so can
be extended to be an entire function on the whole complex domain. The rapid
decay of the Fourier transform of extremisers is established with a bootstrap
argument which relies on a refined bilinear Airy Strichartz estimate and a
weighted Strichartz inequality.Comment: 18 page
Exponential decay of eigenfunctions and generalized eigenfunctions of a non self-adjoint matrix Schr\"odinger operator related to NLS
We study the decay of eigenfunctions of the non self-adjoint matrix operator
\calH = (\begin{smallmatrix} -\Delta +\mu+U & W \W & \Delta -\mu -U
\end{smallmatrix}), for , corresponding to eigenvalues in the strip
-\mu<\re E <\mu.Comment: 16 page
Classical magnetic Lifshits tails in three space dimensions: impurity potentials with slow anisotropic decay
We determine the leading low-energy fall-off of the integrated density of
states of a magnetic Schroedinger operator with repulsive Poissonian random
potential in case its single impurity potential has a slow anisotropic decay at
infinity. This so-called magnetic Lifshits tail is shown to coincide with the
one of the corresponding classical integrated density of states
The Fate of Lifshitz Tails in Magnetic Fields
We investigate the integrated density of states of the Schr\"odinger operator
in the Euclidean plane with a perpendicular constant magnetic field and a
random potential. For a Poisson random potential with a non-negative
algebraically decaying single-impurity potential we prove that the leading
asymptotic behaviour for small energies is always given by the corresponding
classical result in contrast to the case of vanishing magnetic field. We also
show that the integrated density of states of the operator restricted to the
eigenspace of any Landau level exhibits the same behaviour. For the lowest
Landau level, this is in sharp contrast to the case of a Poisson random
potential with a delta-function impurity potential.Comment: 19 pages LaTe
Variational Estimates for Discrete Schr\"odinger Operators with Potentials of Indefinite Sign
Let be a one-dimensional discrete Schr\"odinger operator. We prove that
if \sigma_{\ess} (H)\subset [-2,2], then is compact and
\sigma_{\ess}(H)=[-2,2]. We also prove that if has at
least one bound state, then the same is true for . Further, if has infinitely many bound states, then so does .
Consequences include the fact that for decaying potential with
, has infinitely many bound
states; the signs of are irrelevant. Higher-dimensional analogues are also
discussed.Comment: 17 page
Cwikel's bound reloaded
There are a couple of proofs by now for the famous Cwikel--Lieb--Rozenblum
(CLR) bound, which is a semiclassical bound on the number of bound states for a
Schr\"odinger operator, proven in the 1970s. Of the rather distinct proofs by
Cwikel, Lieb, and Rozenblum, the one by Lieb gives the best constant, the one
by Rozenblum does not seem to yield any reasonable estimate for the constants,
and Cwikel's proof is said to give a constant which is at least about 2 orders
of magnitude off the truth. This situation did not change much during the last
40+ years.
It turns out that this common belief, i.e, Cwikel's approach yields bad
constants, is not set in stone: We give a drastic simplification of Cwikel's
original approach which leads to an astonishingly good bound for the constant
in the CLR inequality. Our proof is also quite flexible and leads to rather
precise bounds for a large class of Schr\"odinger-type operators with
generalized kinetic energies. Moreover, it highlights a natural but overlooked
connection of the CLR bound with bounds for maximal Fourier multipliers from
harmonic analysis.Comment: 30 page
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