Abstract
Motivated by Botelho and Jamison’s seminal 2010 study on elementary operators that are m-isometries, in this paper, we introduce the concept of m-null pairs of operators and establish some structural properties and characterizations of the class of elementary operators whose symbols are m-null (so-called m-null elementary operators). It is shown that if the symbols of an elementary operator L are, in turn, a p-null elementary operator and a q-null elementary operator, then L is a -null elementary operator. Some extant results on elementary m-isometries can be recovered from this renewed perspective, often providing added value.
Keywords:
elementary operator; m-isometry; m-null operators; (m, T)-null operators; Stirling numbers MSC:
47B02; 47B47; 47B49; 11B73
1. Introduction
Let denote the set of all bounded linear operators on a Hilbert space H, and let m be a fixed positive integer. An operator is said to be an m-isometry if
where, as usual, is the adjoint of T. Note that a 1-isometry is an isometry. The notion of m-isometry was developed by Agler and Stankus in the trilogy [1,2,3]. Since then, a number of authors have explored the properties of this class of operators, and multiple generalizations have been proposed in different contexts. The arguments employed in those investigations encompass a wide variety of methods, including combinatorics, arithmetic progressions, Lagrange interpolation, properties of operator roots of polynomials, tensor products, factorization into left and right multiplication operators, and the hereditary functional calculus. For a rather complete account, the interested reader is referred to [4] and references therein.
Fix . An operator is said to be an elementary operator if there exist finite sequences and of operators in such that , where the number d is called the length of the operator. The special cases (of length 1) and (of length 2) have been amply studied in several contexts. Botelho et al. [5,6] 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. They also gave sufficient conditions for such elementary operators to be m-isometries for higher m, and formulated the following conjecture: given , if there is a nonzero scalar such that is a p-isometry and is a q-isometry, then the elementary operator is a -isometry. This conjecture was subsequently confirmed by Duggal [7] and other authors from different viewpoints and generalizations, cf. [8] and references therein. To our best knowledge, the initial approach of Botelho and Jamison [5], based on a result by Fong and Sourour [9], has not been pursued in later investigations on the subject. In this paper, we provide a proof that combines the ideas in [5] with basic operator algebra and some combinatorics. With this purpose, we introduce the concept of m-null pairs of operators and establish some structural properties and characterizations of the class of elementary operators whose symbols are m-null, which we call m-null elementary operators. This is performed in Section 2. Then, in Section 3, it is shown that if the symbols of an elementary operator L are, in turn, a p-null elementary operator and a q-null elementary operator, then L is a -null elementary operator (Theorem 1). As a consequence, the aforementioned result of Botelho–Jamison–Duggal is retrieved (Corollary 1), as are other improved versions of extant results on elementary m-isometries. In view of the techniques employed in achieving this result, in the last Section 4, we raise the natural question whether its reciprocal, as established by Gu ([10], Theorem 7), could be obtained without resorting to analytic tools.
2. (m, T)-Null Pairs
Let us introduce some notation. To any pair of operators , we associate the elementary operator of length 1 , which maps each to
The operators A and B are called the symbols of . It can be easily checked that the adjoint of is given by . Further, for and , we write
Here, as usual, is the identity operator. Clearly,
Definition 1.
Let and . A pair of symbols is said to be -null provided that (or, equivalently, ). If this is true of all , then we shall just say that is m-null. The elementary operator is called -null, respectively m-null, whenever so is . Either one of these conditions will be termed strict if it holds for m, but not for .
Remark 1.
In the notation above, is an m-isometry if
or, equivalently,
Additionally, the operator S is an m-isometry if the pair is -null, and a strict m-isometry if is -null but not -null.
The following simple recurrence relation, valid for all , will be useful:
Remark 2.
Proposition 1.
Proof.
Finally, when is -null, we must have (3). Indeed, if , this derives from the fact that is -null for all , while if , then implies , whence . □
Proposition 2.
Let and . Assume that is -null and for sufficiently large . Then, .
Proof.
From Proposition 1,
Now
implies
Upon assuming for large k, the result follows. □
Given , the next proposition characterizes those pairs that are -null.
Proposition 3.
Let and . The pair is -null if, and only if,
Proof.
Assume that is -null, and fix . Then, from Proposition 1,
Since
we have
The last identity is obtained by appropriately redefining and shifting the indices in the horizontal recurrence relation for the binomial coefficients ([11], Corollary 2.3). This yields (4). Equations (4) and (5) are seen to be equivalent on account of ([11], Equation (3.12)).
Conversely, if (4) holds then, particularizing there, gives
so that is -null. □
We close this section with a second characterization of m-null pairs of operators, this time involving Stirling numbers.
Let , . The Stirling number of the first kind is defined such that the number of permutations of n elements that contain exactly k permutation cycles is the non-negative number . The Stirling number of the second kind is the number of ways of partitioning a set of n elements into k disjoint non-empty subsets. The Stirling numbers of the first and second kind turn out to be the coefficients of the expansions of the falling factorials into powers, and of the powers into falling factorials, respectively. They arise frequently in combinatorial, probabilistic, and statistical applications, and have been generalized in several directions, one of them being the so-called non-central Stirling numbers. For further insight on Stirling and non-central Stirling numbers of the first and second kind, the interested reader is referred to ([11], Chapter 8).
Given , consider the falling factorial operator
Falling factorial operators can be expanded into a sum of operator powers whose coefficients are the Stirling numbers of the first kind. In fact, as commutes with itself, in analogy with [11] (Equation (8.2)), we have
for each . Since , the identity
actually holds true for all .
The following well-known lemma will be useful in the sequel. We include a proof for the sake of completeness.
Lemma 1.
Let , and let be a polynomial of degree r. Then
for all .
Proof.
This can be easily proved using the calculus of finite differences. In fact, let be the forward difference operator, where denotes the translation operator, given by , and is the identity operator, acting on the space of all polynomials g. On the one hand,
so that
On the other hand, an induction process gives
whence
This establishes the result. □
Proposition 4.
Assume and . Then,
- (i)
- There holdswhereare non-central Stirling numbers of the second kind with parameter ([11], Equation (8.62)).
- (ii)
- is -null if, and only if,
- (iii)
- is strictly -null if, and only if,whereare Stirling numbers of the second kind ([11], Theorem 8.4).
Proof.
Let . By induction on , we will show that
Since
the identity (7) holds trivially for and . Assuming (7) is true for r, we shall prove it for . Indeed, using the induction hypothesis and the triangular recurrence formula for the Stirling numbers of the second kind ([11], Theorem 8.7), we obtain
Now we may write
To get (6), it suffices to observe that for each , , Lemma 1, with , implies
so that
(cf. [11], p. 316); this gives Part (i). Part (ii) is a straightforward consequence. Lastly, the same argument as above, applied to instead of , shows that
Therefore,
Bearing in mind Definition 1, Equations (1) and (6) complete the proof. □
3. Elementary Operators with Elementary Symbols
Theorem 1.
Let , let , and assume that the pairs and of operators in are -null and -null, respectively. Define the elementary operators
Then, the pair is -null, that is,
Proof.
Fix an arbitrary , and set
We want to show that
Without loss of generality, we may assume . Since is -null, Proposition 3 yields
Similarly, being -null, also
Inserting (10) and (11) into (9), we obtain
To complete the proof, it suffices to establish that
for every with and . This amounts to showing that
Since
is a polynomial in x of degree less than , Lemma 1, with , yields the desired conclusion. □
Corollary 1.
Let and . Assume M is a p-isometry and is a q-isometry. Then, the operator is a -isometry.
Proof.
In fact, is -null, and is -null (Remark 1). Apply Theorem 1, with , , and , to obtain
as required. □
The following result by Fong and Sourour ([9], Theorem 1) will allow us to give a final property of m-null elementary operators.
Lemma 2.
Let and be bounded operators on the Hilbert space H, and let Φ be the operator given by
with not all the ’s equal to 0. If for all , then is linearly dependent. Furthermore, if is a maximal linearly independent subset of , and denote constants for which
then for all if, and only if,
(In case , identity (12) becomes vacuous and condition (13) should be interpreted as ).
We shall also make use of the following basic facts.
Lemma 3.
Let and .
- (i)
- If the family of powers is linearly independent, then so is .
- (ii)
- If , but , then is linearly independent.
Proof.
First, let be scalars such that ; we want to show that . Since
we obtain
The linear independence of the family yields the following homogeneous system of linear equations in the unknowns :
The matrix of coefficients of this system is upper triangular, so its determinant can be computed as the product of the entries in the main diagonal, namely,
This means that the only solution to this system is the trivial one. Consequently, is linearly independent.
Second, to prove that the family is linearly independent, let the scalars be such that
Again, we want to show that . As , but ,
necessarily implies that . Proceeding by induction, assume for some . Then,
and
which entails that and completes the induction. □
Theorem 2.
Notation is as in Theorem 1. Fix and . Let the elementary operator be given by (8).
- (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 (i), then is -null if, and only if,
- (iii)
- Let q be as in Part (i), let , and assume is m-null. If is (necessarily strictly) -null, then is -null. Conversely, if is strictly -null, then is -null.
Proof.
Part (i) follows immediately from (9) and Lemma 2, while the first identity in Part (ii) is a straightforward consequence of Proposition 3 and the linear independence of . Regarding the second, it is easy to check that
To establish the direct implication in Part (iii), first, observe that if is -null, then this property must be strict; otherwise, Proposition 3 would render as a linear combination of , contradicting the linear independence of . Next, fix . Since is m-null, Part (i) gives
Furthermore, being -null, we may apply Part (ii) and substitute to obtain
or
Shifting the summation index and recalling that , we finally arrive at the identity
valid for all . The particularization of in (16) gives
where
On the other hand, particularizing in (16) and shifting indices, we obtain
whence
Since R commutes with the operator in brackets,
Thus,
so that is -null.
To prove the converse implication in Part (iii), assume that is m-null and is strictly -null. Then, by Part (ii) of Lemma 3 along with Proposition 3, the family is linearly independent maximal. The desired conclusion follows from the direct implication, by symmetry. □
Remark 3.
Again, Remark 1 provides a particular version of Theorem 2 for m-isometries.
4. An Open Question
The nature of the solutions to the problems discussed in this paper is primarily algebraic and combinatorial rather than analytic, as it is often the case in the literature on similar problems arising in other contexts, such as m-invertible, m-isometric, m-self-adjoint, and related classes of operators. In ([10], Theorem 7), the following result is established:
Theorem 3.
Assume . Then, 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 is a constant λ such that is a strict p-isometry and is a strict q-isometry, where .
Unlike the proof for the if part, that 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 [12]. The question arises whether a similar converse to Theorem 1, and hence a proof for Theorem 3, can be found that avoids analytic tools.
Funding
This research received no external funding.
Data Availability Statement
The original contributions presented in the study are included in the article. Further inquiries can be directed to the author.
Acknowledgments
The author wishes to thank the anonymous referees for the insightful comments that helped improve the presentation of this paper.
Conflicts of Interest
There are no conflicts of interest to disclose.
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