Advances in Pure Mathematics
Vol.05 No.06(2015), Article ID:56137,4 pages
10.4236/apm.2015.56032
On Eigenvalues and Boundary Curvature of the Numerical Rang of Composition Operators on Hardy Space
Mohammad Taghi Heydari
Department of Mathematics, College of Sciences, Yasouj University, Yasouj, Iran
Email: heydari@yu.ac.ir
Copyright © 2015 by author and Scientific Research Publishing Inc.
This work is licensed under the Creative Commons Attribution International License (CC BY).
http://creativecommons.org/licenses/by/4.0/
Received 9 November 2014; accepted 30 April 2015; published 6 May 2015
ABSTRACT
For a bounded linear operator A on a Hilbert space, let
be the smallest possible cons- tant in the inequality
. Here, p is a point on the smooth portion of the boundary
of the numerical range of A.
is the radius of curvature of
at this point and
is the distance from p to the spectrum of A. In this paper, we compute the
for composition operators on Hardy space
.
Keywords:
Composition Operator, Numerical Range, Eigenvalues, Curvature
1. Introduction
For a bounded linear operator A on a Hilbert space, the numerical range
is the image of the unit sphere of
under the quadratic form
associated with the operator. More precisely,
Thus the numerical range of an operator, like the spectrum, is a subset of the complex plane whose geometrical properties should say something about the operator.
One of the most fundamental properties of the numerical range is its convexity, stated by the famous Toeplitz-Hausdorff Theorem. Other important property of is that its closure contains the spectrum of the operator,
is a connected set with a piecewise analytic boundary
[1] .
Hence, for all but finitely many points, the radius of curvature
of
at p is well defined. By convention,
if p is a corner point of
, and
if p lies inside a flat portion of
.
Let denote the distance from p to
, we define
the smallest constant such that
(1)
for all with finite non-zero curvature.
By Donoghue’s theorem whenever
. Therefore,
for all convexoid element A. Recall that convexoid element is an element such that its numerical range coincides with the convex hull of its spectrum. For non-convexoid A,
(2)
where the supremum in the right-hand side is taken along all points with finite non-zero curvature.
The computation of for arbitrary
matrix A is an interesting open problem. For
, we do not have an exact value of
. The question whether there exists a universal constant
, posed by Mathias [2] . Caston, et al. [3] prove the following inequalities:
(3)
Mirman a sequence of Toeplitz nilpotent matrices
with
algrowing asymptotically as
is also found [3] . Hence, the answer to Mathias question is negative. However, the lower bound in (3) is still of some interest, at least for small values of n. The question of the exact rate of growth of
(it is
, or n, or something in between) remains open.
2. Composition Operator on Hardy Space
Let denote the open unit disc in the complex plane, and the Hardy space H2 the functions
holomorphic in such that
, with
denoting the n-th Taylor coefficient of f. The
inner product inducing the norm of is given by
. The inner product of two functions f and g in
may also be computed by integration:
where is positively oriented and f and g are defined a.e. on
via radial limits.
For each holomorphic self map of
induces on
a composition operator
defined by the equation
. A consequence of a famous theorem of J. E. Littlewood [4] asserts that
is a bounded operator. (see also [5] [6] ).
In fact (see [6] )
In the case, Joel H. Shapiro has been shown that the second inequality changes to equality if and only if
is an inner function.
A conformal automorphism is a univalent holomorphic mapping of onto itself. Each such map is linear fractional, and can be represented as a product
, where
for some fixed and
(See [7] ).
The map interchanges the point p and the origin and it is a self-inverse automorphism of
.
Each conformal automorphism is a bijection map from the sphere to itself with two fixed points (counting multiplicity). An automorphism is called:
elliptic if it has one fixed point in the disc and one outside the closed disc;
hyperbolic if it has two distinct fixed point on the boundary, and
parabolic if there is one fixed point of multiplicity 2 on the boundary.
For, an r-dilation is a map of the form
. We call r the dilation parameter of
and in the case that
,
is called positive dilation. A conformal r-dilation is a map that is conformally conjugate to an
-dilation, i.e., a map
, where
and
is a conformal automorphism of
.
For, an w-rotation is a map of the form
. We call w the rotation parameter of
. A straightforward calculation shows that every elliptic automorphism
of
must have the form
for some and some
.
3. Main Results
In [8] , the shapes of the numerical range for composition operators induced on by some conformal automorphisms of the unit disc specially parabolic and hyperbolic are investigated.
In [9] , V. Matache determined the shapes in the case when the symbol of the composition operator the inducing functions are monomials or inner functions fixing 0. The numerical ranges of some compact composition operators are also presented.
Also, in [10] the spectrum of composition operators are investigated.
This facts will help in discussing and proving many of the results below.
Remark 3.1 If,
, then
and
is a closed ellipticall disc whose boun-
dary is the ellipse of foci 0 and 1, having major/minor axis of length and
. There- fore
.
Remark 3.2 If,
, then
the closure of
. If w is the n-th root
of unity then is the convex hull of all the n-th roots of unity and so
. If w is not a root of
unity the is the union of
and the set
. In this case also
.
Remark 3.3 If is hyperbolic with fixed point a,
, then
and is a disc center at the origin. Therefore
where
is the numerical radius of
.
Remark 3.4 If is parabolic, then
and
is a disc center at the origin. Therefore
.
Remark 3.5 If is elliptic with rotation parameter w, and w is not a root of unity, then
and
is a disc center at the origin. Therefore
.
Therefore we have the following table for.
Completing the Table
An elliptic automorphism of
that does not fix the origin must have the form
, where
for some fixed and
If we wish to show this dependence of
on p and w, we will denote the elliptic automorphism
by
.
If is periodic then, surprisingly, the situation seems even murkier: For period 2 has been shown the closure of
is an elliptical disc with foci at
(Corollary 4.4. of [8] ). It is easy to see that
is open, also in [11] , the author completely determined
for period 2.
Theorem 3.6 If is an elliptic automorphism with order 2 and P it’s only fixed point in open unit disc, then there is
such that
Proof. Let the operator A be self-inverse, i.e., but
, so
is an ellipse with foci at ±1 [12] . If
with
. Then
If is an elliptic automorphism with order 2 and p it’s only fixed point in open unit disc, then
where. Since
is a nontrivial self-inverse operator on Hardy space
and
is an inner
function, then
and so there is such that:
But for period then all we can say is that the numerical range of
has k-fold symmetry and we strongly suspect that in this case the closure is not a disc. Because the numerical range in this case is an open problem, so the completing of
is also open problem.
Acknowledgements
I thank the editor and the referee for their comments. Also, when the author is the responsible of establishing Center for Higher Education in Eghlid he is trying to write this paper, so I appreciate that center because of supporting me in conducting research.
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