- Aleksandrov–Clark measure
In
mathematics , Aleksandrov–Clark (AC) measures are specially constructed measures named after the twomathematician s,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.Construction of the measures
The original construction of Clark relates to one-dimensional perturbations of compressed shift operators on subspaces of the
Hardy space ::
By virtue of
Beurling's theorem , any shift-invariant subspace of this space is of the form:where is an
inner function . As such, any invariant subspace of the adjoint of the shift is of the form:
We now define to be the shift operator compressed to , that is
:
Clark noticed that all the one-dimensional perturbations of , which were also unitary maps, were of the form
:
and related each such map to a measure, on the unit circle, via the
Spectral theorem . This collection of measures, one for each on the unit circle , is then called the collection of AC measures associated with .An alternative construction
The collection of measures may also be constructed for any analytic function (that is, not necessarily an inner function). Given an analytic self map, , of the unit disc, , we can construct a collection of functions, , given by
:
one for each . Each of these functions is positive and harmonic, so by Herglotz' Theorem each is the Poisson integral of some positive measure on . This collection is the set of AC measures associated with . It can be shown that the two definitions coincide for inner functions.
References
* Douglas Clark, "One-dimensional perturbations of restricted shifts", J. Analyse Math., 1972, vol 25, pp 169–191.
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