1. Introduction and Preliminaries
The study of operators acting on spaces endowed with a semi-inner product induced by a positive operator arises naturally in the framework of pseudo-Hermitian quantum mechanics. This setting provides a natural framework for extending classical notions of operator theory, leading to the introduction and systematic study of generalized classes of operators. In particular,
-normal operators offer a meaningful generalization of normal operators and allow for the investigation of their structural properties in spaces equipped with such semi-inner products [
1,
2,
3]).
Let denote the -algebra of all bounded linear operators on a complex infinite-dimensional Hilbert space .
Let
be the set of all positive operators in
, defined by
For any operator , we use the notations , , and to denote its range, null space, and adjoint, respectively. Moreover, stands for the closure of the range, and denotes the orthogonal projection onto .
Given
, we define a semi-inner product on
by
with the induced seminorm
An operator
is called
-bounded if there exists
, such that
The set of all
-bounded operators is denoted by
. For
, the
-operator seminorm is defined by [
4] as
Definition 1 ([
4])
. Let . We say that is an -adjoint
of if, for all , the relationholds. Equivalently, this condition can be expressed in operator form asAn operator is called -selfadjoint
if it coincides with its -adjoint, that is, Following Douglas theorem, as presented in [
5,
6], an operator
admits an
-adjoint if and only if
The set of all operators that admit an
-adjoint is denoted by
. As is standard in the literature, for each
, there exists a distinguished
-adjoint operator of
, called the reduced solution of the equation
which is denoted by
or
(see [
4]). In this paper, we adopt the notation
.
The
-adjoint operator
satisfies the following properties:
Some properties of the map
are summarized in the following theorem.
Theorem 1 ([
4,
7,
8])
. The operator satisfies the following properties:- 1.
.
- 2.
.
- 3.
If , then and
- 4.
Recall that an operator
is said to be
-isometric ([
4]), if
and
-unitary if
that is, both
and
are
-isometries ([
4]).
Several broader notions of normality have emerged in recent developments, extending the classical framework of normal operators. Notable examples include
n-normal,
-normal, polynomially normal, and doubly polynomially normal operators on Hilbert spaces ([
9,
10,
11,
12]). Let
. The operator
is said to belong to one of the following generalized normal classes:
- 1.
n-normal if
for some positive integer
n ([
12]).
- 2.
-normal if
for some positive integers
n and
m ([
11]).
- 3.
Polynomially normal if
for some polynomial
([
13]).
- 4.
Doubly polynomially normal if
for some polynomials
([
14]).
These classes of generalized normal operators satisfy the chain of inclusions
The classical concepts of normality in Hilbert spaces have been naturally extended to semi-Hilbertian spaces, giving rise to the notion of
-normal operators and their various generalizations. A number of authors have contributed significantly to the formulation and analysis of these
-extensions. For a comprehensive treatment, the reader may consult [
4,
7,
8,
15,
16]. Let
. The operator
is said to belong to one of the following classes of
-normal operators:
- 1.
- 2.
--normal ([
15]) if
for
.
- 3.
--normal ([
17]) if
- 4.
Polynomially -normal ([
18]) if
for some polynomial
.
- 5.
--normal ([
19]) if
for some polynomial
and a positive integer
m.
For recent developments in the theory of Hilbert space operators, the reader may consult [
20,
21,
22,
23,
24].
In this paper, we introduce and systematically study the class of -normal operators in semi-Hilbertian spaces, where P and Q are nonconstant complex polynomials. These spaces are endowed with a semi-inner product induced by a positive operator, providing a natural generalization of classical Hilbert spaces and a suitable framework for extending traditional operator theory. Building on the recently developed notions of operator normality in semi-Hilbertian spaces, we define -normality as a natural extension of polynomially normal operators and investigate the fundamental algebraic and spectral properties of these operators. In particular, we examine their behavior under common operator constructions, study conditions for their -adjoints, and explore their relationships with other generalized classes of operators such as --normal and --normal operators. Several results are provided to highlight the structural and spectral characteristics of -normal operators, showing how this class not only generalizes classical polynomially normal operators but also provides new insights into the interplay between operator polynomials and semi-Hilbertian structures.
2. --Normal Operators in Semi-Hilbertian Spaces
In this section, we introduce a new notion of operator normality, termed --normal operators, where P and Q are nonconstant complex polynomials in a single variable. We explore several fundamental properties of this class, building on earlier results established for related concepts of -normality.
Definition 2. Let . The operator is called a -
-normal operator
if there exist two nonconstant complex polynomialssuch thator equivalently, In particular, if , then reduces to a polynomially -normal operator.
Remark 1. The above definition of --normal operators includes several important special cases:
- 1.
A --normal operator coincides with a standard -normal operator.
- 2.
A --normal operator coincides with an n--normal operator.
- 3.
A --normal operator coincides with an --normal operator.
- 4.
A --normal operator coincides with a polynomially -normal (or P--normal) operator, where .
These observations highlight that the concept of --normal operators provides a unified framework encompassing several previously studied classes of -normal operators. In particular, by choosing specific forms of the polynomials P and Q, one can recover familiar operator classes such as -normal, n--normal, --normal, and polynomially -normal operators. This demonstrates the versatility of the --normality notion and its potential to facilitate the study of algebraic and spectral properties across a wide spectrum of semi-Hilbertian operators.
To illustrate the distinctive features of --normal operators and to show that this class genuinely extends previously studied notions of -normality, we present the following concrete example.
Example 1. It can be easily verified thatwhich implies that . A straightforward computation yields the -adjoint We then observe thatfor . However, if we take and , a direct calculation shows Hence, is a --normal operator, while it is neither -normal nor P--normal.
This example illustrates that the class of --normal operators is strictly broader than both the -normal and P--normal classes. Even though does not satisfy these stronger notions of normality, it satisfies the defining condition of --normality for appropriate choices of the polynomials P and Q.
For convenience, we adopt the following abbreviations:
Remark 2. The hierarchy of -normal operator classes can be summarized as follows: This diagram shows the inclusion relations between the different classes of -normal operators.
Remark 3. Let Then, the operator polynomial is given by and its -adjoint satisfies We now provide a theorem that gives a characterization of --normal operators.
Theorem 2. Let and let . Then, is --, if and only if the following conditions hold: Proof. Assume first that
is
-
-
, that is,
Since
it follows that
which proves condition (
24).
Moreover, for any
, we have
which establishes condition (
25).
Conversely, suppose that conditions (
24) and (
25) are satisfied. From (
24) and the inclusion
we obtain
Next, using condition (
25), for all
,
This implies
and, hence,
Finally, for all
, we have
which yields
Therefore,
is
-
-
, completing the proof. □
Remark 4. In this remark, we present several specific instances of Theorem 2 that have appeared in previous studies. These examples show that the general --normal framework not only encompasses well-known classes of -normal operators such as -, n--, --, and polynomially - operators, but also unifies these diverse notions under a single, more general concept. By choosing suitable polynomials P and Q, each classical case can be recovered as a particular instance of the -- condition.
(i) If , then conditions (24) and (25)) of Theorem 2 reduce toThis recovers the notion of - operators. In this case, Theorem 2 coincides with [16] (Theorem 2.1). (ii) If and , the conditions becomeThis corresponds to the class of -- operators, and Theorem 2 reduces to [17] (Theorem 2.1). It illustrates how powers of the operator and its -adjoint characterize generalized normality. (iii) If and , then the conditions areThis recovers the notion of polynomially - operators (or P--normal operators), and Theorem 2 coincides with [18] (Theorem 2.1).
The following proposition examines the relationship between the --normality of an operator and that of its -adjoint , thus extending the classical properties of normal operators to the broader --normal framework.
Proposition 1. Let , P and Q are in . The following are true.
(1) If is an --, then is an -- operator.
(2) If is an -- and is invariant subspace for , then is an -- operator.
Proof. (1) Since
is a
-
-
, we have
If we put
and
we obtain
This means that
is a
-
-
.
(2) Let
. Since
, we have
By our additional assumption,
Thus, both
and
are invariant subspaces for
, and so
is a reducing subspace for
.
The block form of
in the decomposition
is
Step 1: Show .
The operator
maps
into
. Let
. Then,
, so
By assumption,
. Hence
so
Step 2: Show .
Similarly, for
,
since
. Therefore,
Step 3: Deduce .
The block matrix of
becomes diagonal:
so
Assume that
is
-
-normal, then
Using
a direct calculation gives
We deduce
Since
is reducing for
, we have
Hence
so
Thus,
is a
-
-normal operator. □
Proposition 2. Let and let . DefineThe following provides several algebraic characterizations of the --normality of . The operator is --, if and only if i.e., the operators and commute.
If is --, then the mixed operator commutes with both and : The operator is --, if and only if one of the following equivalent commutation relations is satisfied: Thus, either relation alone provides an alternative characterization of --normality.
Proof. Set
so that
Recall that
is
-
-
, if and only if
(1) Compute
Hence,
, if and only if
, which is exactly the
-
-normality of
.
(2) Assume
. Then
and similarly,
(3) Observe
Hence, either
or
is equivalent to
, which by part (1) is equivalent to the
-
-normality of
. □
Lemma 1 ([
25] (Lemma 3.1)).
Let , where for all . Then, Furthermore, The following theorem provides a structural criterion ensuring that an upper triangular block operator
inherits
-
-normality from its diagonal entries
and
.
Theorem 3. Letand let . Assume that and are -
-normal and that . If, moreover, , then is -
-normal, where .
Proof. Write
By a routine computation, one obtains, for
and for
,
Since
, all off-diagonal sums vanish, and thus
Since and are --normal, each diagonal block is zero. Hence, the whole matrix is zero, and so is --normal. □
The following proposition shows that the class of --normal operators is stable under conjugation by -isometries. That is, if an operator is --normal, then any operator of the form , where is an -isometry, remains --normal.
Proposition 3. Let and let be operators reducing . If is an -isometry and is --, then is also --.
Proof. Let
and
. We have
, which satisfies
Moreover, because
and
reduce
,
and
Step 1: Computing powers of
. By induction,
Step 2: Computing
.
Step 3: Computing
. Using
,
Step 4: Verifying
-
-normality.
Since
is
-
-
,
thus
Therefore, is --. □
Remark 5. In the classical Hilbert space setting, normality is invariant under unitary equivalence. Proposition 3 shows that an analogous phenomenon holds in the semi-Hilbertian context, where unitary operators are replaced by -isometries and the usual adjoint is replaced by the -adjoint.
The following proposition shows that --normality is inherited by reducing subspaces. Specifically, if a closed subspace reduces both the operator and is compatible with , then the restriction remains --normal.
Proposition 4. Let and , such that is --normal. Let be a closed subspace of , which reduces . Assume, moreover, that reduces (equivalently and ). Then, the restriction is --.
Proof. Since
reduces both
and
, we may view
and
as block diagonal with respect to the orthogonal decomposition
, namely
where each block acts on the indicated subspace. Under these block decompositions, the
-adjoint also decomposes blockwise; more precisely
Now the polynomial functional calculus respects this block decomposition. For every polynomial
, we have
Because
is
-
-normal, we have
Restricting this equality to the
-block (i.e., looking at the
-entry of the block matrix equality) yields
This shows that
is
-
-
. □
The following result links classical polynomial normality with the semi-Hilbertian setting.
Proposition 5. Let and be such that . If is a P- operator, then is --.
Proof. Let
and
satisfy
. Assume that
is
P-
, i.e.,
Step 1: Commutation implies equality of
-adjoint and usual adjoint. Since
, the
-adjoint of
coincides with the usual adjoint:
Using
, we obtain
for all
, showing
Step 2:
-
-normality. By definition,
is
-
-normal if
Using Step 1, this becomes
Since
is
P-normal, this equality holds. Hence,
is
-
-
. □
It is well known that every - operator is -- for all polynomials . However, the converse does not hold in general; that is, an operator can be -- for certain polynomials P and Q without being - (see Example 1). This naturally leads to the question: under what conditions does --normality imply -normality? The following theorem provides sufficient conditions on the operator and its -adjoint.
Theorem 4. Let such that:
LetIf for all , the operator is --normal, i.e.,then, is -: Proof. Step 1: Reduce to .
Since
is invariant under
, it is a reducing subspace. Hence,
Step 2: Expand
-normality.
By assumption, for all
,
Expanding
P and
Q gives
Step 3: Collect powers of
.
Using the binomial theorem:
Thus, the commutator becomes a polynomial in
, whose leading term is
Step 4: Let
.
Dividing by
and taking the limit, we obtain
so for all
,
Step 5: Use the image condition.
Since
, we have
Combining these inclusions, we conclude
so
is
-
. □
2.1. Tensor Products on Semi-Hilbertian Spaces
Let
and
be semi-Hilbertian spaces, i.e., Hilbert spaces equipped with positive operators
and
inducing the semi-inner products
2.1.1. Tensor Product Space and Semi-Inner Product
The tensor product space
is equipped with the tensor product semi-inner product
extended by linearity and continuity to all elements of
.
2.1.2. Tensor Product of Operators
Let
and
. Their tensor product operator
is defined on pure tensors by
Its
-adjoint satisfies
(see [
26] (Lemma 3.1))
2.1.3. Normality in Tensor Products
If
is
-
and
is
-
, i.e.,
then their tensor product is
-
([
27] (Theorem 3.3)):
The semi-inner product factorizes over the tensor product: acts independently on each factor.
Normality is preserved because the commutator factorizes:
This property underlies the validity of Theorem 5.
Theorem 5. Let be such that
is invariant under each , and
for .
LetIf, for all and all , the operators are --normal, then the tensor productis -. Proof. We proceed by induction on d.
Step 1: Base case .
For , the result reduces to Theorem 4, which ensures that if is --normal for all and is invariant under with , then is -normal.
Step 2: Induction hypothesis.
Assume that for some
, if
satisfy the assumptions of the theorem, then
is
-
.
Step 3: Induction step.
Considerthe
d-fold tensor product
By the induction hypothesis,
is
-normal, and by Theorem 4,
is
-
.
Step 4: Tensor product of -normal operators.
If
X is
-
and
Y is
-
, then
is
-
from [
27] (Theorem 3.3). Applying this to
, we conclude that
is
-
.
Step 5: Conclusion.
By induction, the result holds for all . □
Theorem 5 generalizes the result of Theorem 4 from a single operator to a tuple of operators acting on a tensor-product space. It shows that under certain structural conditions, the property of --normality for each individual operator is preserved in the tensor product.
Theorem 6. Let be semi-Hilbertian spaces induced by positive operators for . For each i, let and let be polynomials. Assume each is invariant under , so that and the polynomial functional calculus are well-defined. Assume further that each satisfies the --normality condition:Define the tensor product operator and polynomials byso thatThen, satisfies the --normality condition: Proof. By the invariance assumption, the tensor-product
-adjoint decomposes as
The polynomial functional calculus respects the tensor structure:
Hence,
By the
-
-normality of each
, each factor commutes:
Therefore,
which proves the theorem. □