In mathematics, Aleksandrov–Clark (AC) measures are specially constructed measures named after the two mathematicians, A. B. Aleksandrov and Douglas Clark, who discovered some of their deepest properties. The measures are also called either Aleksandrov measures, Clark measures, or occasionally spectral measures.
AC measures are used to extract information about self-maps of the unit disc, and have applications in a number of areas of complex analysis, most notably those related to operator theory. Systems of AC measures have also been constructed for higher dimensions, and for the half-plane.
The original construction of Clark relates to one-dimensional perturbations of compressed shift operators on subspaces of the Hardy space:
H2(D,C).
By virtue of Beurling's theorem, any shift-invariant subspace of this space is of the form
\thetaH2(D,C),
where
\theta
K\theta=\left(\thetaH2(D,C)\right)\perp.
We now define
S\theta
K\theta
S\theta=
P | |
K\theta |
S| | |
K\theta |
.
Clark noticed that all the one-dimensional perturbations of
S\theta
U\alpha(f)=S\theta(f)+\alpha\left\langlef,
\theta | |
z |
\right\rangle,
and related each such map to a measure,
\sigma\alpha
\alpha
T
\theta
The collection of measures may also be constructed for any analytic function (that is, not necessarily an inner function). Given an analytic self map,
\phi
D
u\alpha
u\alpha(z)=\Re\left(
\alpha+\varphi(z) | |
\alpha-\varphi(z) |
\right),
one for each
\alpha\inT
\mu\alpha
T
\varphi