1. Introduction
The concept of
m-isometry was introduced by Agler and Stankus in a series of seminal papers [
1,
2,
3]. Since then,
m-isometries have been the subject of active investigation. In fact, the case
, corresponding to standard isometries, had already been extensively studied due to its central role in the development of operator theory and its applications, particularly in modeling contractive operators through their isometric dilations [
4], its function-theoretic ties to the classical Hardy space [
5,
6], and its applications in
-control problems [
7]. For
, the theory connects to discrete-time nonstationary processes with stationary increments, a class that generalizes Brownian motion [
2,
3]. More broadly,
m-isometries with
appear naturally in the disconjugacy theory for Toeplitz operators with smooth symbols, as introduced by Boutet de Monvel and Guillemin [
8], as well as in the analysis of shift operators on Dirichlet-type spaces. For instance, multiplication by
z on the Dirichlet space over the unit disk is not an isometry but a 2-isometry ([
9], Proposition 9.3.1). Richter [
10,
11] established that every cyclic 2-isometry arises from multiplication by
z on certain Dirichlet-type spaces, creating a link with the study of shift-invariant subspaces; for recent progress on this topic, see [
12]. Other relevant contributions are [
13,
14,
15,
16,
17]. All these applications emphasize the significance of
m-isometries across analysis, probability, and mathematical physics, motivating the search for generalizations.
The original notion of
m-isometry has indeed been extended in numerous directions. Bayart [
18] introduced
-isometries in Banach spaces. Hoffman et al. [
19] explored the role of the second parameter,
p, in this definition, allowing
. Subsequently, other classes of operators encompassing or related to
m-isometries have been proposed, usually first in Hilbert spaces and later in the Banach or metric spaces setting. Without aiming for exhaustiveness, some of them are as follows: Chō et al. [
20,
21] introduced the so-called
- and
-isometric operators, where
C is some conjugation of the Hilbert space. Motivated by
m-isometries, Sid Ahmed generalized the notions of left and right inverses to
m-left and
m-right inverses, respectively, on Banach spaces [
22]. The notions of
m-left and
m-right generalized inverse operators—which extend both
m-left and
m-right inverses and generalized inverses—have been studied on Banach spaces by Ezzahraoui [
23]. Saddi et al. defined
m-partial isometries on Hilbert spaces [
24] and
-partial isometries in semi-Hilbertian spaces [
25], as an extension of the former. Aouichaoui [
26] introduced
-isometries. Further extensions include (but are not limited to)
-isometric mappings on Banach spaces, for
(see [
27] and references therein), along with
-isometric mappings on metric spaces [
28];
n-quasi-
-isometric operators [
29];
-isosymmetric operators [
30]; exponentially
m-isometric operators [
31]; and
q-partial-
-isometries [
32]. Another natural generalization of
m-isometries are (spherical)
m-isometric
d-tuples, as introduced by Gleason and Richter [
33]. Spherical
m-isometries have attracted additional interest due to their relation to a moment problem [
34]. The properties of this class have also been investigated in [
35], while interesting examples can be found in [
36]. In the last years, other single-variable operator families of
m-isometries have been extended to
d-tuples; see, e.g., [
37,
38,
39,
40].
Botelho et al. [
41,
42] characterized the elementary operators of length 1 acting on the Hilbert–Schmidt class of a separable Hilbert space that are 2-isometries and 3-isometries, and they conjectured the following: Given
, if there exists a nonzero scalar
such that
is a
p-isometry and
is a
q-isometry, then the elementary operator
is a
-isometry. Duggal [
43] and others subsequently confirmed this conjecture, cf. [
44] and references therein. Later on, Gu [
45] proved its converse—the elementary operator with symbols
, acting on the Hilbert–Schmidt class of a separable Hilbert space, is a strict
m-isometry if and only if there exists a constant
such that
is a strict
p-isometry and
is a strict
q-isometry, where
. Unlike the
if part, which can be established through algebraic and combinatorial methods, the proof for the
only if part uses analytical arguments relying on properties of the spectral radius and the approximate point spectrum of an operator, which can be traced back to Magajna [
46]. This fact might explain why, as compared to Duggal’s —which has been versioned in almost all generalizations of the notion of
m-isometry—Gu’s theorem has received less attention in the literature. Actually, to our knowledge, no analog of Gu’s necessary condition exists for the generalizations listed above.
The initial approach of Botelho and Jamison [
41], based on a result by Fong and Sourour [
47] (of wider applicability), does not seem to have been continued in later research on this topic. Aiming to provide a proof of the above results along the lines of [
41], in [
48], we introduced the concept of
m-null pairs of operators and established some properties and characterizations of
m-null elementary operators, which led to a generalization of Duggal’s theorem. Also, we raised the question of whether Gu’s necessity proof inherently required analytical techniques. In the present paper, we answer it in the negative by relying essentially on algebra and combinatorics to extend Gu’s theorem to
m-null elementary operators. Our procedure, which involves explicitly solving a difference equation in terms of binomial coefficients, is quite constructive, and we hope that it provides deeper insight into the role and scope of Fong and Sourour’s theorem.
Investigations on the aforementioned extensions of m-isometries have employed a wide range of techniques, comprising combinatorial arguments, arithmetic progressions, Lagrange interpolation, properties of operator roots of polynomials, tensor products, factorization into left and right multiplication operators, and the hereditary functional calculus. Despite this methodological diversity, a number of such extensions are special cases of -null pairs of operators (see Examples 1 to 10 below). Our approach provides a common framework for those generalizations, thereby enabling a unified treatment. In particular, a version of Gu’s theorem is immediately obtained for all those generalizations of m-isometries that can be expressed in terms of -null pairs. Furthermore, the use of combinatorial and algebraic arguments, as opposed to analytic ones, is particularly well suited to more general contexts where conventional tools from spectral theory may be unavailable, such as general metric spaces or Banach spaces with a limited operator structure, a fact that suggests new research directions. Finally, the constructive nature of our approach not only strengthens the understanding of the mechanisms governing m-null elementary operators but also opens new pathways for computational applications, where explicit representations are essential.
The paper is structured as follows: In
Section 2, we recall some previous material from [
48], along with the theorem from [
47] on which this research is based. The main result is achieved in
Section 3 (Theorem 3 and Corollary 4). The last
Section 4 briefly elaborates on the applications, versatility, limitations, and scope of our findings.
2. Preliminaries
Let
H be a Hilbert space, and let
denote the set of all bounded linear operators on
H. Given
, the elementary operator of length 1 with symbols
A and
B is the operator
, defined by
It can be easily checked that the adjoint
of
is
. For simplicity, the elementary operator
will be represented by
I, as this notation is unambiguous in context.
Definition 1. Let m be a positive integer and . A pair of symbols is said to be -null, provided thatIf this is true for all , then we shall just say that is m-null. The elementary operator is called -null, respectively m-null, when so is . Either one of these conditions will be termed strict if it holds for m, but not for . The flat condition in Definition 1 can be lifted from to , as follows:
Definition 2. Let m be a positive integer and . A pair of superoperators is said to be -null at , provided thatwhere and , respectively, denote the j-th iterates of A and B . Alternatively, we will abbreviate this condition by saying that is -null. The pair is m-null at if (
1)
holds for all . Again, either condition will be termed strict if it holds for m, but not for . When , we shall just refer to nullity at S, for short. Note that the
m-nullity of
does not mean
, as
, and their iterates differ from those of
. In particular, if
and
are elementary operators with symbols
, we have
and
, so that (
1) becomes the following:
The flat condition in Definition 1 can be recovered from the lifted one in Definition 2 by choosing the superoperators and as left and right multiplications, respectively, and setting .
Some examples illustrating the above are listed below.
Example 1 (Flat sense).
Recall from [1,2,3] that an operator is said to be an m-isometry iffor some . Thus, in the notation above, is an m-isometry, provided that . Also, the operator S is an m-isometry if the pair is -null, and a strict m-isometry if is -null, but not -null. Example 2 (Flat sense).
An operator is said to be -isometric [20] if there exists some conjugation C such thatfor some . If C is a conjugation and , then for every . Thus, S is -isometric if the pair is -null. Example 3 (Flat sense).
An operator is said to be -isometric [21] if there exists some conjugation C such thatfor some . Thus, S is -isometric if the pair is -null. Example 4 (Flat sense).
The notions of m-left and m-right invertible operators were introduced in [22]. Let . An operator is m-left invertible if there exists such thatSimilarly, is m-right invertible if there exists such that (2) holds. Thus, B is m-left invertible (and A is m-right invertible) if the pair is -null. Example 5 (Lifted sense).
The notions of m-left and m-right generalized inverses were introduced in [23]. Let and . We say that S is an m-left generalized inverse of R ifSimilarly, S is an m-right generalized inverse of R ifIntroducing the elementary operators and , we obtain that S is an m-left generalized inverse of R if the pair is -null at I, and an m-right generalized inverse of R if the pair is -null at I. Example 6 (Lifted sense).
An operator is an m-partial isometry [24] iffor some . Introducing the elementary operator , we obtain that S is an m-partial isometry if the pair is -null at I. Example 7 (Lifted sense).
Let be a positive operator and . An operator is an -partial isometry [25] ifIntroducing the elementary operator , we obtain that S is an -partial isometry if the pair is -null at . Example 8 (Lifted sense).
Let and . An operator is said to be an -isometry [26] ifIntroducing the elementary operator , we obtain that S is an -isometry if the pair is -null at I. Example 9 (Flat sense).
Let . An operator is said to be -isosymmetric [30] ifThus, S is -isosymmetric if the pair is -null, with Example 10 (Flat sense).
An operator is exponentially m-isometric [31] iffor some . Thus, S is exponentially m-isometric if the pair is -null. The next result is ([
48], Proposition 3). We include a (partially different) proof for the sake of completeness.
Proposition 1. Let and . The pair is -null if and only if Proof. Fix
and assume that
is
-null. Since
for
, we obtain:
By ([
49], Corollary 2.3):
Thus, (
3) follows.
For the converse, it suffices to particularize
in (
3). □
Proposition 1 shows that the sequence of powers
of an
-null operator
with symbols
belongs to the class of operator arithmetic progressions of order
, consisting of all those operator sequences
whose
-th differences are constant (and whose
m-th differences are therefore null). In fact, for
, the expression
where
defines a polynomial in
x of degree at most
with coefficients in
, such that
for all
(see, e.g., [
50]).
The following two results were also established in [
48]. The second one is essentially ([
43], Corollary 2.11), while the first one extends this result to
-null operators.
Theorem 1 ([
48], Theorem 1).
Let , let , and assume that the pairs and of operators in are -null and -null, respectively. Define the elementary operatorsThen, the pair is -null, that is, Corollary 1 ([
48], Corollary 1).
Let and . Assume that M is a p-isometry and is a q-isometry. Then, the operator is a -isometry. The theorem of Fong and Sourour on which our main results are based is stated next.
Lemma 1 ([
47], Theorem 1).
Let and be bounded operators on the Hilbert space H, and let Φ
be the operator given bywhere not all the ’s equal 0. If for all , then is linearly dependent. Furthermore, if is a maximal linearly independent subset of , and denote constants for whichthen for all if and only if(In case , identity (4) becomes vacuous and condition (5) should be interpreted as ). The following derivation of ([
48], Lemma 3) will be useful in the sequel.
Lemma 2. Let , and let . If is strictly -null, then the set of powers is linearly independent.
We end this section by recalling one of the main results from [
48]. Although it was fully proved there, we find it instructive to provide a new, explicit proof of the converse statement in Part
and highlight some if its consequences. The proof of the converse to Part
will be given as Proposition 2 below.
Theorem 2 ([
48], Theorem 2).
Notation is as in Theorem 1. Fix and . Let the elementary operator be given by the following:- (i)
Further, let be such that is a maximal linearly independent subset of the set , so thatfor some constants . Then, is m-null if and only if - (ii)
If q is as in Part , then is -null if and only if - (iii)
Let q be as in Part , let , and assume is m-null. If is (necessarily strictly) -null, then is -null. Conversely, if is strictly -null, then is -null.
It is worth noting that Theorem 2 can be particularized to m-isometries.
Corollary 2. Fix and .
- (i)
Let be such that is a maximal linearly independent subset of the set , so thatfor some constants . Then, is an m-isometry if and only if - (ii)
If q is as in Part , then is a q-isometry if and only if - (iii)
Let q be as in Part , let , and assume is an m-isometry. If is a (necessarily strict) q-isometry, then M is a p-isometry. Conversely, if M is a strict p-isometry, then is a q-isometry.
Proof. It is enough to apply Theorem 2, with , , and . □
The next corollary clarifies the role of the strictness conditions.
Corollary 3. Notation is as in Theorems 1 and 2. If is (strictly) -null, then is strictly m-null if and only if is strictly -null. Similarly, if is strictly -null, then is strictly m-null if and only if is (strictly) -null.
Proof. The property of being -null must be strict; otherwise, Proposition 1 would render as a linear combination of , contradicting the linear independence of . Since the proof of the second part can be reduced to that of the first part, we will concentrate on the latter. Thus, assume is -null. From Part of Theorem 2, we find that is -null.
If were -null for some then, by Theorem 1, would be n-null with , thereby preventing from being strictly m-null.
Conversely, let be n-null for some . As is a maximal linearly independent subset of , Lemma 1 yields , with , such that Part of Theorem 2 holds for n instead of m. But then, by Part of the same theorem, is -null with , so that is not strictly p-null. □
3. Main Results
In order to provide an explicit proof of the converse to Part of Theorem 2, in the following two lemmas, we analyze the recurrence relation satisfied by the coefficients appearing in Part of that theorem. For notational simplicity, the analysis will be performed in a more general context.
Lemma 3. Assume is such thatThen, the double sequence of coefficients satisfies the recurrence relationprovided that . Proof. Fix
. On the one hand,
On the other hand,
By linear independence, a comparison between (
9) and (
10) yields the following:
Setting
, we obtain (
8). □
Lemma 4. The solution to the recurrence relation (8) with initial conditionsis the sequence Proof. Write (
8) in the form:
Since
it is apparent that the proposed solution (
12) satisfies the initial conditions (
11) for all
and
. Let us verify by induction that (
12) also satisfies (
13) for any
and
. The base case
, along with the Pascal formula, leads to:
On the other hand, for the proposed solution, we obtain:
This disposes of this induction step. Assuming now that (
12) satisfies (
8) for all
and
, with
, let us prove the same for all
and
. Again, by the inductive hypothesis and the Pascal identity,
On the other hand, for the proposed solution, we obtain:
At this point, the induction process shows that
for all
and
. But then, by (8), equality holds for
as well, as shown by the following:
The proof is thus complete. □
We are now in a position to provide the announced explicit proof of the converse statement in Part of Theorem 2. The notation introduced will be retained.
Proposition 2. Assume is m-null, and let be as in Part of Theorem 2. If is strictly -null, then is -null.
Proof. Since the pair
is strictly
-null, the set of powers
is linearly independent (Lemma 2). Now,
being
m-null, Part
of Theorem 2 yields
for all
. Particularize
in (
14) to obtain
where
Specializing
in (
14) and shifting indices, we also obtain
or
As
R commutes with the operator in brackets, it follows that
On the other hand,
being
-null,
Therefore, writing
,
All the brackets in this expression must vanish, because the set
is linearly independent. Consequently,
and, for
,
To complete the proof, it suffices to invoke Lemma 4, along with Part
of Theorem 2. □
In ([
48],
Section 4), the question was raised whether a converse of Theorem 1—hence, the
m-isometric version of this converse ([
45], Theorem 7)—could be proven without resorting to analytic tools. Theorem 3 answers this question in the affirmative. A previous result is required.
Lemma 5. Notation is as in Theorem 2. If is strictly m-null, then and . Moreover, the set of powers is linearly independent.
Proof. To prove the first assertion, assume that
for some
with
. Let
. The
m-nullity of
yields:
Substitute the relation (
7),
into the first sum on the right-hand side of (
15), to obtain:
Inserting this one back into (
15) results in the following equation:
Since
(where
), and, by (
6),
we infer that
where
. If
, this conclusion prevents
from being linearly independent, which, in view of Lemma 2, contradicts our hypothesis that
is strictly
m-null. If
, then (
15) provides a zero linear combination of
with nonzero coefficients, violating again the linear independence of this set of powers. Consequently,
for all
. That
now follows from (
8) and the fact that
must be nonzero, to avoid a contradiction with the case
of Equation (
14).
To prove the second statement, assume that some
is such that
for suitable scalars
. Substituting this identity and (
6) in (
15) yields the following:
where
if
, and
if
,
. Since
is a maximal linearly independent subset of
, the Fong–Sourour theorem (Lemma 1 above) entails that
For
, combining this with (
7) allows us to obtain:
whence
A comparison with (
7) shows that either
, or
The second possibility can hold only if
or
and
m is even. This means that, unless
or
, we must have
whenever
. But this contradicts the strict
m-nullity of
and proves that
is linearly independent, as asserted.
If
, so that
, Equation (
6) yields the following:
In particular,
implies
for all
. As
is strictly
p-null,
Lemma 2 then renders
linearly independent, along with
. Indeed, assume that
for some scalars
, and, given any
, consider the rank-one operator
. Then,
The linear independence of
forces
. Since
, the desired conclusion follows.
If , so that , then is linearly independent. This completes the proof. □
Definition 3. Always in the notation of Theorem 2, we shall say that is (strictly) -null for some scalar μ and whenever is (strictly) -null (which implies that is (strictly) -null). An analogous convention applies for .
Theorem 3. Assume is strictly m-null, and let be as in Theorem 2. Then, there exists a constant such that is -null and is -null.
Proof. The argument in the proof of Proposition 2 leads us to the following:
Multiplying both sides of this identity by
, we find from (
8) that
where
, by Lemma 5. Now, from Equation (
16), we obtain:
On the other hand, rewriting (
16) as
or equivalently, after simplifying the binomial coefficients,
we see that the sequence given by
is an operator arithmetic progression of order
, and therefore
that is,
Again, Lemma 5 ensures that
, so that (
18) reduces to
In particular,
Also, writing
, we have
The linear independence of the set of powers
, guaranteed by Lemma 5, allows us to equate the coefficients for
in the two representations of
, namely
whence
This simplifies to
It follows that
At this point, we carry the previous identity, with
, over to (
17),
and obtain:
Now,
Therefore,
which shows that
is
-null, with
From the hypothesis, we may write:
Since
is (strictly)
-null, Proposition 2 shows that
is
-null and completes the proof. □
The announced generalization of ([
45], Theorem 7) can now be stated as follows.
Corollary 4. The operator is strictly m-null if and only if there exists a nonzero constant λ such that is strictly -null and is strictly -null, with .
Proof. The result is a straightforward consequence of Theorems 1 and 3, together with Corollary 3. □
We finish by deriving some consequences about the coefficients in Part
of Theorem 2 and their recurrence relation (
8).
Corollary 5. Assume is m-null, and let q and be as in Part of Theorem 2. Then, some constant is such that Proof. Corollary 4 provides a scalar
such that
is
-null. Hence (Proposition 1),
or
By linear independence, (
19) follows. □
Our last result is immediate from the preceding one, but a direct proof is provided for completeness.
Proposition 3. For any scalar λ, the sequence (19) is a solution to the recurrence relation (8), with initial conditions . Proof. We want to check that
Fix
. For
, this becomes
Now, for the proposed solution, we have
so that
Next, we consider
. On the one hand,
Thus,
On the other hand,
Thus,
So, we must prove that
In fact, two applications of the Pascal recurrence for binomial coefficients yield
as required. □
4. Discussion
This paper was motivated by an open question regarding the need for analytical tools (spectral radius and approximate point spectrum) in proving Gu’s result on the symbols of elementary operators that are strict
m-isometries [
45] (Theorem 7). Here, the question has been answered in the negative within the framework of
m-null operators, a generalization of
m-isometries introduced and studied by the author in [
48]. Specifically, we have demonstrated that algebraic and combinatorial methods suffice, thereby eliminating dependencies on spectral theory.
Our constructive approach, which involves explicitly solving a difference equation in terms of binomial coefficients, not only resolves this question but also revitalizes a line of research initiated by Botelho et al. [
41,
42], on the basis of a prior theorem by Fong and Sourour [
47] with broader implications. The findings are placed in the context of operator theory and functional analysis, where
m-isometries and related concepts have been intensively generalized and investigated through diverse methodologies. We show that a number of such generalizations can be expressed as
m-null operators, a unification that enables direct extensions of Gu’s result. Furthermore, by removing its apparent reliance on spectral theory, we pave the way for new extensions beyond the
m-null and Hilbert space settings.
The primary motivation for considering m-null and strictly m-null pairs of operators is twofold. First, as just recalled, they encompass m-isometries and strict m-isometries along with some of their generalizations and related classes, enriching operator theory and its applications by offering a framework that captures a wider range of operator behaviors. Second, they offer new insights into the algebraic and combinatorial nature of m-isometries, suggesting novel methods to handle similar polynomially defined families.
The algebraic character of our methods supports computational applications, such as numerical algorithms for operator decomposition or simulation of discrete-time processes in signal processing and control theory. Moreover, the m-null framework’s versatility suggests applicability to operator semigroups, noncommutative algebras, or graph-theoretic structures.
A primary limitation of the present work is its restriction to Hilbert space operators, raising the question of whether our methods can be effectively adapted to Banach spaces or general metric spaces with minimal structural assumptions, as could be expected. Additionally, due to the recursive nature of m-null conditions, the computational complexity of our algorithms may grow exponentially with the parameter m, potentially limiting scalability in numerical applications.
Thus, future research could focus on extending our results to non-Hilbert settings and enhancing the computational efficiency of our algorithms. A compelling question involves characterizing the structure of specific operator classes, such as weighted shifts, composition operators, or Toeplitz operators, within the m-null framework. Examining links with fields like combinatorics, representation theory, or quantum information theory, where operator-theoretic methods apply to quantum channel analysis, might uncover deeper structural properties and novel applications.