1 Introduction
Let H be a complex separable Hilbert space, and let \(B(H)\) denote the algebra of all bounded linear operators on H. For \(T\in B(H)\), we denote the approximate point spectrum of T by \(\sigma_{a}(T)\).
Let A and B be given operators in \(B(H)\). Recall the definition of the usual derivation operator \(\delta_{A,B}(X)\) given by \(\delta_{A,B}(X)= AX-XB\) for \(X\in B(H)\). For every positive integer k, we have \(\delta^{k}_{A,B}(X)= \delta_{A,B}(\delta^{k-1}_{A,B}(X))\) for \(X\in B(H)\). Let A and B be in \(B(H)\). An operator B is said to be in \(\mathrm{Helton}_{k}(A)\) if \(\delta^{k}_{A,B}(I)=0\).
In operator theory, one of the most important topics is local spectral theory. In the following we consider several properties in local spectral theory such as the single-valued extension property, property (β), property \((\beta )\epsilon\), and so on. Let \(D(\lambda,r)\) be the open disc centered at \(\lambda\in\mathbb {C}\) and with radius \(r > 0\). For an open set U in \(\mathbb {C}\), we denote by \(\mathcal{O}(U, H)\) and \(\mathcal{\xi}(U, H)\) the Fréchet space of all H-valued analytic functions on U and the Fréchet space of all H-valued \(C^{\infty}\)-functions on U, respectively.
An operator \(T\in B(H)\) is said to have the single-valued extension property (SVEP for short) at \(\lambda_{0}\in\mathbb {C}\) if, for every open neighborhood G of \(\lambda_{0}\), the only analytic function \(f: G\rightarrow H\) which satisfies the equation \((\lambda I-T)f(\lambda)=0\) for all \(\lambda\in G\) is the function \(f\equiv0\). An operator T is said to have SVEP if T has SVEP at every point \(\lambda\in\mathbb {C}\). An operator \(T\in B(H)\) is said to satisfy Bishop’s property (β) at \(\lambda_{0}\in\mathbb {C}\) (resp. \((\beta)\epsilon\)) if there exists \(r>0\) such that, for every open subset \(U\subset D(\lambda,r)\) and for any sequence \((f_{n})\) in \(\mathcal{O}(U, H)\) (resp. in \(\mathcal{\xi }(U, H)\)), whenever \((T - z)f_{n}(z)\rightarrow0\) in \(\mathcal{O}(U, H)\) (resp. in \(\mathcal{\xi}(U, H)\)), then \(f_{n}\rightarrow0\) in \(\mathcal{O}(U, H)\) (resp. in \(\mathcal{\xi}(U, H)\)). An operator T is said to have Bishop’s property (β) (resp. \((\beta )\epsilon\)) if T has Bishop’s property (β) (resp. \((\beta)\epsilon\)) at every point \(\lambda\in\mathbb {C}\).
Define
$$\begin{aligned} &\sigma_{\mathrm{SVEP}}(T)=\{\lambda\in\mathbb {C}:T-\lambda\mbox{ fails to SVEP at } \lambda\}; \\ &\sigma_{\beta}(T)= \bigl\{ \lambda\in\mathbb {C}:T-\lambda\mbox{ fails to property } (\beta) \mbox{ at } \lambda \bigr\} ; \\ &\sigma_{(\beta)_{\epsilon}}(T)= \bigl\{ \lambda\in\mathbb {C}:T-\lambda \mbox{ fails to property } (\beta)_{\epsilon} \mbox{ at } \lambda \bigr\} . \end{aligned}$$
An antilinear operator
C on
H is said to be conjugation if
C satisfies
\(C^{2} = I\) and
\((Cx,Cy)=(y,x)\) for all
\(x,y\in H\). An operator
\(T\in B(H)\) is said to be complex symmetric if
\(T^{*}=CTC\). Many standard operators such as normal operators, algebraic operators of order 2, Hankel matrices, finite Toeplitz matrices, all truncated Toeplitz operators, and Volterra integration operators are included in the class of complex symmetric operators. Several authors have studied the structure of a complex symmetric operator. We refer the reader to [
6‐
11] for further details. As a generalization of complex symmetric operators, in [
3], Chō et al. introduced
m-complex symmetric operators with conjugation
C as follows: For an operator
\(T\in B(H)\) and an integer
\(m\geq1\),
T is said to be an
m-complex symmetric operator if there exists some conjugation
C such that
$$\sum_{j=0}^{m}(-1)^{m-j} \begin{pmatrix}m\\j\end{pmatrix}T^{*j}.CT^{m-j}C=0. $$
In 1990s, Agler and Stankus [
1] intensively studied the following operator: For a fixed positive integer
m, an operator
\(T\in B(H)\) is said to be an
m-isometric operator if it satisfies the following equation:
$$\sum_{j=0}^{m}(-1)^{j} \begin{pmatrix}m\\j\end{pmatrix}T^{*m-j}T^{m-j}=0. $$
m-isometric operators are connected to Toeplitz operators, classical function theory, ordinary differential equations, distributions, classical conjugate point theory, Fejer–Riesz factorization, stochastic processes, and other topics.
In [
4], Chō et al. introduced (
\(m,C\))-isometric operators with conjugation
C as follows: For an operator
\(T\in B(H)\) and an integer
\(m\geq1\),
T is said to be an (
\(m,C\))-isometric operator if there exists some conjugation
C such that
$$\sum_{j=0}^{m}(-1)^{j} \begin{pmatrix}m\\j\end{pmatrix}T^{*m-j}.CT^{m-j}C=0. $$
In [
5], Chō et al. introduced [
\(m,C\)]-isometric operators with conjugation
C as follows: For an operator
\(T\in B(H)\) and an integer
\(m\geq1\),
T is said to be an [
\(m,C\)]-isometric operator if there exists some conjugation
C such that
$$\sum_{j=0}^{m}(-1)^{j} \begin{pmatrix}m\\j\end{pmatrix}CT^{m-j}C.T^{m-j}=0. $$
According to the definitions of complex symmetric,
m-complex symmetric,
m-isometric, (
\(m,C\))-isometry, and [
\(m,C\)]-isometry, we define [
m]-complex symmetric
T as follows: An operator
T is said to be an [
m]-complex symmetric operator if there exists some conjugation
C such that
$$\sum_{j=0}^{m}(-1)^{m-j} \begin{pmatrix}m\\j\end{pmatrix}CT^{j}C.T^{m-j}=0. $$
For an operator
\(T\in B(H)\) and a conjugation
C, we define the operator
\(w_{m}(T,C)\) by
$$w_{m}(T,C)=\sum_{j=0}^{m}(-1)^{m-j} \begin{pmatrix}m\\j\end{pmatrix}CT^{j}C.T^{m-j}. $$
Then
T is an [
m]-complex symmetric operator if and only if
\(w_{m}(T,C)= 0\). Moreover, it holds that
$$CTC.w_{m}(T,C)-w_{m}(T,C).T= w_{m+1}(T,C). $$
Hence if
T is an [
m]-complex symmetric operator, then
T is an [
n]-complex symmetric operator for every
\(n\geq m\).
The following example provides an operator which is a [3]-complex symmetric operator but not a [2]-complex symmetric operator.
2 [m]-complex symmetric operators
We investigate the power \(T^{n}\) and the inverse \(T^{-1}\) of an [m]-complex symmetric operator T and show that the class of [m]-complex symmetric operators is norm closed.
We examine the nilpotent perturbations of an [m]-complex symmetric operator.
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