*converges for a.e. .*

This results follows from the estimate on the Carleson’s maximal function. In the preprint with R. Bessonov, we studied the analog of Lusin’s conjecture for polynomials orthogonal on the unit circle.

Suppose is probability measure on . It belongs to Szego’s class if . This class plays crucial role in many branches of classical analysis and probability (see other posts). If is in Szego’s class, we can define Szego’s function by the formula

Denote the polynomials orthonormal with respect to by . The analog of Lusin’s conjecture says:

*For in Szego’s class, prove that for a.e. .*

We were not able to solve this problem but we proved a few results that reformulate pointwise convergence of polynomials in different terms. Each measure generates the sequence of Schur functions (analytic contractions on ), that we denote by . Given a parameter and a point , define the Stolz angle to be the convex hull of and . Our central result is the following theorem

**Theorem.**

*Let be Szego measure and . Take any and denote . Then, for almost every , the following assertions are equivalent:*

*(a) ,*

*(b) ,*

*(c) ,*

*(d) for every .*

The idea of the proof is based on the analysis of new entropy function which generalizes the standard Szego entropy. This quantity is well-behaved for a.e. boundary point and this gives uniform in control over the oscillation of in on the circle.

]]>

We define its logarithmic integral as

Existence of logarithmic integral, i.e., condition

plays a role in the theory of Gaussian stationary stochastic processes: it holds if and only if the future of the process with spectral measure can not be predicted by its past.

Every Poisson-finite measure gives rise to a function in Herglotz-Nevanlinna class, i.e., the class of functions analytic in with non-negative imaginary part, by a Herglotz formula

where . The de Branges theory of Hilbert spaces of functions of exponential type provides a bijection between Herglotz-Nevanlinna class and the class of all canonical Hamiltonian systems. Canonical Hamiltonian system can be written as the following Cauchy problem

where Hamiltonian is nonnegative locally summable matrix-function on . In short, the Weyl-Titchmarsh theory for canonical systems provides for each and the converse is true by de Branges theory. In the paper, we characterize all for which the logarithmic integral of exists. Consider for which . Then, define the grid of points by the formula

and consider the quantity

Our main theorem, which is stated below, is a natural generalization of the Szego theorem in the theory of polynomials orthogonal on the unit circle.

We quantify it by the sharp two-sided estimate. The sum in the definition of can be written in the form reminiscent of the matrix Muckenhoupt condition but we do not understand yet how the problem is connected to Muckenhoupt classes.

There are multiple applications of our theory to scattering problems for Dirac and wave equations.

]]>

We considered the problem on the infinite cylinder which is equivalent to -periodic initial data in one direction. If one takes as nonnegative bounded function with compact support, then the weak solution exists globally in time. If denotes the diameter of its support, then the trivial bound reads

In the paper, we improve it to

Our argument is based on controlling the sequence of specially chosen moments on the dyadic spatial scale. The crucial part of the argument was to exploit the uniform in time estimate on the first moment of vorticity. For the problem on the whole plain, similar results were obtained previously in the paper by Iftimie, Sideris, and Gamblin “On the evolution of compactly supported planar vorticity”. Our method is different from the one used previously in that it uses another conserved quantity and different set of moments.

The 2D Euler evolution in infinite cylinder is remarkable model because the kernel in the Biot-Savart law that expresses velocity in terms of has the exponentially decaying first component. That means two distant parts of vorticity are essentially decoupled. One would hope that this, along with conservation of horizontal center of mass, should yield much stronger bound on , for example, . This, however, seems difficult to achieve due to possible “diffusive dynamics” of .

One possible interesting direction is to study the evolution of patch of vorticity in the active scalar equation when no conserved quantities are known but the kernel in the Biot-Savart law is short-range and has some basic symmetries. One would think that this should be enough to prove strong confinement results.

]]>- The sequence of recurrence parameters (or Schur parameters) of polynomials orthogonal with respect to belongs to .

Given a measure on the real line that satisfies normalization

,

we can ask the question when the set of functions

is NOT dense in . The answer is given by the theorem of Kolmogorov-Krein-Wiener: it is iff

However, the spectral characterization of this condition has been missing. In the paper, we consider the Krein string, – the “mother of all non-negative self-adjoint operators with simple spectrum”. It is given by the formal differential operator

where is any non-decreasing function on . The corresponding self-adjoint operator can be defined and its spectral measure along with one additional real parameter determines completely. In the paper, we characterize all strings for which the logarithmic integral of converges. This is done by proving analogous statement for diagonal De Branges canonical systems. The existence of the entropy is important for the prediction theory of stationary Gaussian processes with continuous time. It is likely that the obtained characterization will allow one to quantify some statements in this theory.

]]>where oscillates and decays at infinity. More precisely, where and the norm is defined as

I also assume to make sure that is non-negative operator. The wave equation for is

The main result of the paper states that the following wave operators

exist for every and the limit is understood in norm. The condition on is optimal in some sense, i.e., the rate of decay is sharp and the oscillation is necessary if the potential is not short-range.

The proof is based on the analysis of the asymptotical behavior of the Green’s function where , is fixed, and . The result about asymptotics is similar to that for the orthogonal polynomials on the circle in the Szego case. The main difference with the one-dimensional situation is that the resulting “Szego” function belongs to the vector-valued Hardy space. The operator can be written through the resolvent by the contour integral and this is how the Green’s function enters the proof. The method is quite general and can be adapted to wave equations for the Schrodinger equation and other problems.

]]>

where is a stream function given by Then, we set up a variational problem with constraint

We proved that the global minimizer is and if is close to the minimum value for some patch , then is close to in a weak topology. This essentially gives the required stability.

]]>

If one considers the 2d Euler equation of incompressible inviscid fluids on the plane in the vorticity form and takes the initial data as the characteristic function of a certain domain, then the Yudovich theory guarantees that the solution will exist globally and will be equal to the characteristic function of a time-dependent domain which is homeomorphic to the original one for all times. The numerical experiments dating back to the works of P. Saffman and Zabusky et al. indicate the existence of the centrally-symmetric V-states, i.e. a symmetric pair of patches that rotates with constant angular velocity around the origin without changing shape. If the distance between the patches in the pair equals to and , then the boundary of the V-state seems to be smooth. However, when , the both patches form a 90 degrees angle at the point of contact. The analytical proof for the existence of these V-states has never been obtained and this is an interesting problem. In the recent preprint, I considered the analogous equation with the cut-off. Loosely speaking, this corresponds to looking at the window around the origin where the contact of the patches is supposed to happen. Mathematically, the model with cut-off is important as it possesses the explicit singular solution: . Then, I addressed the problem of existence of the curve of smooth solutions that converge to in the uniform metric when the parameter . Technically, this boils down to application of the implicit function theorem and is somewhat tedious. This technique might be important to better understand the mechanism of the merging and the sharp corner formation in the Euler dynamics. Another important problem is to prove that the merging in finite time is possible for the -model when and is close to .

]]>does have a transport effect (though without much specifics).

Perturb the Laplacian as follows where is potential and ask the question what is a minimal assumptions on to guarantee that the a.c. spectrum is preserved. Make it a perturbation theory question, assume that is in some weighted Lebesgue space . Then, what are the critical and ? In one-dimensional case, one answer is . This is a critical space. This result was proved for Schrodinger in a great paper by Deift and Killip but for Dirac it was known for at least half a century and dates back to the works by Mark Krein. Krein’s result on Dirac, however, is only a continuous analog of the classical results for polynomials orthogonal on the unit circle (Szego case).

For , the conjecture by Barry Simon is that

is sufficient for the preservation of a.c. spectrum. Very little is known so far. Only the case of Schrodinger on the Cayley tree is well-understood. Take a rooted Cayley tree with the origin at and assume that each vertex has exactly three neighbors while has only two. Consider the Laplacian on defined at each point as the sum over the neighbors and then a simple calculation shows that the spectrum of is and it is purely a.c. Then, perturb by . The multidimensional result reads as follows. Consider all paths that go from to infinity without self-intersections (rays). Put the probability measure on them by tossing a Bernoulli coin at each vertex. Then, the claim is that the a.c. spectrum contains the a.c. spectrum of unperturbed operator if with positive probability the potential where denotes the path from the origin. There is more quantitative version, of course, which implies Simon’s conjecture if the Jensen inequality is applied. The condition we have here is more general and more physically appealing: it says that we only need enough directions were the potential is small for the particle to propagate.

For , sparse or slowly decaying and oscillating potentials can be handled. If the potential does not oscillate, then the scattering process is quite complicated, it is governed by very intricate evolution equation (that captures semiclassical WKB correction as very special case). This evolution equation is poorly studied and much work is needed in this direction. Soft one-dimensional methods seem to be of little help.

In Euclidean case, what would be the analog of the probability space on the set of paths that escape to infinity? This question was addressed here. It turns out that there is a natural Ito’s stochastic equation that describes these paths. The statement we have is somewhat weak though. It says that the a.c. spectrum contains the positive half-line if with positive probability and we can not yet replace summability by the square summability over the path . Nevertheless, even this result gives rise to interesting questions like how one computes probabilities given by this Ito’s calculus? That conventionally can be reduced to the analysis of the corresponding potential theory and the modified harmonic measure. The potential theory one encounters in this case is somewhat in between elliptic and the parabolic one: on the large scale it is parabolic and on the small scale it is elliptic. The estimates on the harmonic measure in terms of the geometric properties of support can be found in my paper with Kupin.

___________________________________________________________________

**May 2012.** I recently finished writing a survey for the Nikolskii conference volume, it contains more details.