×
Well done. You've clicked the tower. This would actually achieve something if you had logged in first. Use the key for that. The name takes you home. This is where all the applicables sit. And you can't apply any changes to my site unless you are logged in.

Our policy is best summarized as "we don't care about _you_, we care about _them_", no emails, so no forgetting your password. You have no rights. It's like you don't even exist. If you publish material, I reserve the right to remove it, or use it myself.

Don't impersonate. Don't name someone involuntarily. You can lose everything if you cross the line, and no, I won't cancel your automatic payments first, so you'll have to do it the hard way. See how serious this sounds? That's how serious you're meant to take these.

×
Register


Required. 150 characters or fewer. Letters, digits and @/./+/-/_ only.
  • Your password can’t be too similar to your other personal information.
  • Your password must contain at least 8 characters.
  • Your password can’t be a commonly used password.
  • Your password can’t be entirely numeric.

Enter the same password as before, for verification.
Login

Grow A Dic
Define A Word
Make Space
Set Task
Mark Post
Apply Votestyle
Create Votes
(From: saved spaces)
Exclude Votes
Apply Dic
Exclude Dic

Click here to flash read.

This paper studies the Dirichlet-type space and the generalized
Dirichlet-type space whose defect operators are of finite ranks.


The Dirichlet-type space $D(\mu)$ is defined by a nonnegative Borel measure
$\mu$ on the closed unit disc. When $\mu$ is a finitely atomic measure, we
characterize the conditions for the de Branges-Rovnyak space $\mathcal{H}(B)$
and the $D(\mu)$ space to be the same.


The generalized Dirichlet-type space $\mathcal{D}_{\vec{\mu}}$ is determined
by a tuple $\vec{\mu}$ of distributions on the unit circle. If $\vec{\mu} =
(\frac{|dz|}{2\pi}, \mu_1, \ldots, \mu_{n-1})$ is an allowable $n$-tuple such
that $(M_z, \mathcal{D}_{\vec{\mu}})$ is expansive and the defect operator of
$(M_z, \mathcal{D}_{\vec{\mu}})$ has finite rank, then we show that $n$ is
even, $\mu_{n-1}$ is a positive measure, the distributions $\mu_i$ $(i = 1,
\ldots, n-1)$ are supported on a finite set contained in the unit circle, and
the order of each $\mu_i$ doesn't exceed $\frac{n}{2}-1$. We show that the
converse of this is true when $n=2$, but when $n \geq 3$, the converse is not
true. To achieve this, we use the characterization of the higher order
isometric $(M_z,\mathcal{H}(B))$ that are finite rank perturbations of
isometric operators obtained in \cite{LGR}. Our investigation also provides
many interesting examples of normalized allowable $2m$-tuples $\vec{\mu}$.

Click here to read this post out
ID: 512837; Unique Viewers: 0
Unique Voters: 0
Total Votes: 0
Votes:
Latest Change: Oct. 31, 2023, 7:34 a.m. Changes:
Dictionaries:
Words:
Spaces:
Views: 8
CC:
No creative common's license
Comments: