Szegő limit theorems explained
In mathematical analysis, the Szegő limit theorems describe the asymptotic behaviour of the determinants of large Toeplitz matrices.[1] [2] They were first proved by Gábor Szegő.
Notation
Let
be a
Fourier series with Fourier coefficients
, relating to each other as
w(\theta)=
ckei, \theta\in[0,2\pi],
ck=
w(\theta)e-ik\thetad\theta,
such that the
Toeplitz matrices
Tn(w)=\left(ck-l\right)0\leq
are
Hermitian, i.e., if
then
. Then both
and eigenvalues
are real-valued and the determinant of
is given by
.
Szegő theorem
Under suitable assumptions the Szegő theorem states that
\limn →
)=
F(w(\theta))d\theta
for any function
that is continuous on the range of
. In particular
such that the arithmetic mean of
converges to the integral of
.
[3] First Szegő theorem
The first Szegő theorem[1] [2] [4] states that, if right-hand side of holds and
, then
holds for
and
. The RHS of is the
geometric mean of
(well-defined by the
arithmetic-geometric mean inequality).
Second Szegő theorem
Let
be the Fourier coefficient of
, written as
\widehatck=
log(w(\theta))e-ik\thetad\theta
The second (or strong) Szegő theorem[1] [5] states that, if
, then
\limn
=\exp\left(
k\left|\widehat
\right).
See also
Notes and References
- Book: 1071374. Böttcher. Albrecht. Silbermann. Bernd. Analysis of Toeplitz operators. Springer-Verlag. Berlin. 1990. 3-540-52147-X. Toeplitz determinants. 525.
- Book: Simon. Barry. Szegő's Theorem and Its Descendants: Spectral Theory for L2 Perturbations of Orthogonal Polynomials. Princeton University Press. Princeton. 2011. 978-0-691-14704-8.
- Robert M.. Gray. Toeplitz and Circulant Matrices: A Review. Foundations and Trends in Signal Processing. 2006.
- G.. Szegő. Ein Grenzwertsatz über die Toeplitzschen Determinanten einer reellen positiven Funktion. Math. Ann.. 76. 1915. 490 - 503. 10.1007/BF01458220. 4. 123034653 .
- 0051961. Szegő. G.. On certain Hermitian forms associated with the Fourier series of a positive function. Comm. Sém. Math. Univ. Lund [Medd. Lunds Univ. Mat. Sem.]. 1952. 228 - 238.