Higher order differentiability of operator functions in Schatten norms
Christian Le Merdy, Anna Skripka

TL;DR
This paper characterizes the higher order differentiability of operator functions in Schatten norms, linking smoothness of scalar functions to operator differentiability, and extends previous results to unbounded operators and broader function classes.
Contribution
It provides new necessary and sufficient conditions for higher order Schatten differentiability of operator functions, extending existing theories to unbounded operators and wider function classes.
Findings
Characterizes when scalar functions induce higher order Schatten differentiable operator functions.
Extends differentiability results to unbounded operators and broader function classes.
Provides explicit formulas for Fréchet and Gâteaux derivatives.
Abstract
We establish the following results on higher order -differentiability, , of the operator function arising from a continuous scalar function and self-adjoint operators defined on a fixed separable Hilbert space: (i) is times continuously Fr\'{e}chet -differentiable at every bounded self-adjoint operator if and only if ; (ii) if and , then is times continuously Fr\'{e}chet -differentiable at every self-adjoint operator; (iii) if , then is times continuously Fr\'{e}chet -differentiable and times G\^{a}teaux -differentiable at every self-adjoint operator. We also prove that if , then…
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Higher order differentiability
of operator functions in Schatten norms
Christian Le Merdy*∗*
and
Anna Skripka*∗∗*
Abstract.
We establish the following results on higher order -differentiability, , of the operator function arising from a continuous scalar function and self-adjoint operators defined on a fixed separable Hilbert space:
- (i)
is times continuously Fréchet -differentiable at every bounded self-adjoint operator if and only if ; 2. (ii)
if and , then is times continuously Fréchet -differentiable at every self-adjoint operator; 3. (iii)
if , then is times continuously Fréchet -differen-tiable and times Gâteaux -differentiable at every self-adjoint operator;
We also prove that if , then is times continuously Fréchet -differentiable, , at every self-adjoint operator. These results generalize and extend analogous results of [10] to arbitrary and unbounded operators as well as substantially extend the results of [2, 4, 19] on higher order -differentiability of in a certain Wiener class, Gâteaux -differentiability of with , and Gâteaux -differentiability of in the intersection of the Besov classes . As an application, we extend -estimates for operator Taylor remainders to a broad set of symbols. Finally, we establish explicit formulas for Fréchet differentials and Gâteaux derivatives.
Key words and phrases:
Differentiation of operator functions, Schatten-von Neumann classes
2010 Mathematics Subject Classification:
47B49, 47B10, 46L52
*∗*Research supported by the French “Investissements d’Avenir” program, project ISITE-BFC (contract ANR-15-IDEX-03)
*∗∗*Research supported in part by NSF grants DMS-1500704 and DMS-1554456
1. Introduction
Differentiability is one of natural properties studied in theory of functions, in particular, operator functions. Pioneering results on differentiability of operator functions were obtained in [6] under restrictive assumptions on functions and operators. These results were substantially refined and extended in [3, 29, 17, 18, 1, 11, 16, 12, 7, 19, 2, 10, 22] in response to development of perturbation theory, but some problems remained open. In this paper we answer several questions on higher order differentiability of operator functions in Schatten -norms, . The exponent in this paper is reserved for a number in the interval .
Initially derivatives of operator functions were studied in the operator norm, but the same results hold in the -norm, . It was proved in [18, Theorem 2] that if is an element of the Besov space , then is Gâteaux differentiable with respect to the -norm and the operator norm at every self-adjoint operator, yet a stronger sufficient condition was derived in [1] in terms of complex analysis. It follows from [3] and properties of Besov spaces, that is Fréchet -differentiable, , at every self-adjoint operator (see Theorem 4.1) and Fréchet differentiable with respect to the operator norm at every bounded self-adjoint operator. The necessary condition for differentiability of in the -norm was obtained in [18, Theorem 3] via nuclearity criterion for Hankel operators. In particular, the condition is not sufficient for Gâteaux -differentiability of [17, Theorem 8] (see also [8]). It was established in [19, Theorem 5.6] that if is in the intersection of Besov classes , then is times Gâteaux differentiable with respect to the -norm and the operator norm. Notes on higher order Fréchet -differentiability follow below.
The set of Fréchet differentiable functions with respect to the -norm is larger than the set of -differentiable functions. It was established in [10, Theorem 7.17] that is Fréchet -differentiable at every bounded self-adjoint operator if and only if , while it was demonstrated in [10, Example 7.20] that the assumption “ and is bounded” is not sufficient for Fréchet differentiability of at an arbitrary unbounded operator. It was proved in [2, Theorem 5.5] that a function is times Fréchet -differentiable (in fact, differentiable with respect to any symmetric operator ideal norm with so called property (F)) at every self-adjoint operator if is in the Wiener class , which consists of with the Fourier transform of a finite measure on , . It was proved in [4, Theorem 4.1] that a function in is times Gâteaux -differentiable at every bounded self-adjoint operator and, under the additional assumption “ is bounded, ”, at every self-adjoint operator.
We prove (see Theorem 3.6) that is times continuously Fréchet -differentiable at every bounded self-adjoint operator if and only if , generalizing the differentiability result of [10] for to an arbitrary natural and establishing a new property of continuous dependence of the differential on the point of differentiation. We obtain new sufficient conditions for an arbitrary order continuous Fréchet differentiability at an unbounded self-adjoint operator that significantly extend analogous results of [2, 10]. Namely, we prove that is times continuously Fréchet -differentiable at every self-adjoint operator if , all derivatives are bounded, and (see Theorem 3.4) as well as that is times continuously Fréchet -differentiable at every self-adjoint operator if and all derivatives are bounded (see Theorem 3.3). We also prove (see Theorem 3.7(ii)) that is times Gâteaux -differentiable under the relaxed assumption “ and all derivatives are bounded” (the latter property is a necessary condition for times Gâteaux -differentiability, see Proposition 3.9), extending the result of [4] from to the general and the consequence of [19] from to with bounded derivatives. Finally, we prove (see Theorem 4.1) that every is times continuously Fréchet -differentiable, , substantially strengthening Gâteaux -differentiability that follows from [19].
Study of operator derivatives has been mainly motivated by development of perturbation theory. Initially operator derivatives were calculated in the operator norm and appeared in Taylor-like approximations of operator functions (see, for instance, [26] for details and references). It was necessary to involve higher order derivatives to produce approximations with respective remainders in symmetrically normed ideals. Replacing the first and second order derivatives of operator functions with respect to the operator norm by the -norm derivatives allowed to extend the fundamental results of [14, 13] on Taylor approximations to much broader sets of functions in [20, 4]. In Theorem 3.8 we apply our main results to extend the estimate of [23, Theorem 4.1] for the th order Taylor approximation with bounded initial self-adjoint operator and to an unbounded initial operator and with bounded .
Advancement in the study of operator smoothness and differentiability has been based on techniques known under the name “multiple operator integration” and developing since [6]. There are two principal approaches to multiple operator integration on Schatten classes (see, e.g., [28] for details and references). The approach in [5, 19] depends on separation of variables of a symbol and applies to the entire set of symbols treated in this paper only when ; the approach in [22] builds on harmonic analysis of UMD spaces. To establish higher order Fréchet differentiability and include unbounded operators we combine advantages of both approaches and perform multi-stage approximations on symbols, perturbations, and generating operators. Our method differs from the methods of [5, 19] for Gâteaux differentiability resting on the former approach, which was sufficient due to the weaker type of differentiability and either restriction to a smaller set of functions or to perturbations in , as well as the method of [10] for the first order Fréchet differentiability resting on the latter approach, which was sufficient due to a stronger technical machinery available in the first order case and restriction to bounded operators.
We fix the following notations and conventions to be used throughout the paper. Let denote the space of bounded -linear operators mapping the Cartesian product of Banach spaces to a Banach space , let denote a separable Hilbert space, the th Schatten-von Neumann class of compact operators on , , the subset of self-adjoint elements of , and the canonical trace on the ideal . For basic properties of Schatten ideals see, e.g., [25]. When the domain of a self-adjoint operator is not specified, it is assumed to be defined either on or on a dense subspace of . For any , let denote the linear space of times continuously differentiable functions on . Let denote the space of continuous bounded functions on , the space of continuous functions on which tend to [math] at , and the space of Lipschitz functions on . Let denote the group of all permutations of the set . For any , let denote the th order divided difference of . We recall that it is defined recursively as follows:
[TABLE]
We also recall that is bounded provided that .
2. Multiple operator integration
In this section we collect existing and derive new properties of multiple operator integrals that are crucial for proofs of our main results.
Gâteaux and Fréchet derivatives of our operator functions will be represented via multiple operator integrals introduced in [22, Definition 3.1]. We recall this definition below.
Let , , and denote
[TABLE]
for every , , and . Let and , . Let and let be a bounded Borel function.
Definition 2.1*.*
Suppose that for every , the series
[TABLE]
converges in the norm of and
[TABLE]
is a sequence of bounded multilinear operators that map . If the sequence of operators converges strongly to some bounded multilinear operator , then is called the multiple operator integral associated with and the operators (or the spectral measures ), and is denoted by .
We note that there are other multiple operator integral constructions (see, e.g., [28]), but the one described in Definition 2.1 allows to handle for the largest set of functions treated in this paper, that is, for with .
The following conditions for existence of bounded multiple operator integrals and estimates for their norms are crucial in our proofs.
Theorem 2.2**.**
Let , , , . Let be self-adjoint operators and let . Then, and there exists such that
[TABLE]
Proof.
We note that the inequality (2.2) follows from (2.1) because and focus on the proof of (2.1).
In the case , the inequality (2.1) is established in [22, Theorem 5.3 and Remark 5.4].
Assume now that some of are distinct. A careful investigation of the proofs of [22, Lemmas 3.3 and 5.5] shows that their results also hold for distinct . This immediately implies that to get (2.1) in the general case it suffices to prove (2.1) for whose spectra are finite subsets of .
Assume now that the spectra of are finite subsets of . Then the transformation is well defined and represented by a finite sum. Let and assume that the last self-adjoint operators are equal. Let denote the elementary matrix whose nonzero entry has indices . Let for , , and for . Then for any , let be the self-adjoint operator with the spectral measure and for any , let . Consider , with , and let . A straightforward calculation (see, e.g., the proof of [27, Theorem 3.3]) implies that
[TABLE]
Note that by construction, the self-adjoint operators are equal. Further for any and . Using this process inductively for , we obtain that to prove (2.1), it suffices to have it when the self-adjoint operators are all equal. This concludes the proof. ∎
Lemma 2.3**.**
Let , , , , bounded, . Let , , , . Assume that . Then,
[TABLE]
Proof.
Both multiple operator integrals in (2.3) are well defined bounded multilinear transformations by Theorem 2.2. Since for every in the domain of ,
[TABLE]
by [9, Lemma 5.6.17]. Let , so . By the spectral decomposition,
[TABLE]
We obtain the decomposition of the spectral measure of ,
[TABLE]
Hence,
[TABLE]
Summarizing the observations made above we arrive at
[TABLE]
which implies (2.3). ∎
There is a different approach to multiple operator integrals (see [19]) that allows to estimate their -norm and operator norm, but it applies to a set of functions significantly smaller than the one in Theorem 2.2. By [22, Lemma 3.5], the multiple operator integral constructed in [19] coincides with the one presented in Definition 2.1 for in a certain Besov class, which definition is recalled below.
Let be such that its Fourier transform is supported in the set , is an even function and for . Set
[TABLE]
for . Following [19], the Besov space is defined as the set
[TABLE]
equipped with the seminorm
[TABLE]
The following estimate for the -norm, of the transformation is derived completely analogously to the estimate of in the operator norm proved in [19, Theorem 5.5].
Theorem 2.4**.**
Let and . Let . Let be self-adjoint operators and let . Then, and there exists such that
[TABLE]
We will also need properties of multiple operator integrals that follow from the approach of [5]. Again let , and let be a scalar-valued spectral measure for (that is, a measure on the Borel subsets of having the sames sets of measure zero as ). Let be the product measurable space. Then the tensor product space
[TABLE]
is a -dense subspace.
Further is a dual space, namely it naturally identifies with the -fold projective tensor product of (see [5, Section 3.1]).
Definition 2.5*.*
Let be the unique linear map from the tensor product space into such that
[TABLE]
for all , and all . According to [5, Proposition 6], uniquely extends to a -continuous and contractive map
[TABLE]
Let be a bounded Borel function and let be the class of its restriction to . Then the -linear map will be simply denoted by
[TABLE]
in the sequel.
According to [5, Remark 8], the above multiple operator integrals coincide with Pavlov’s ones [15]. The crucial point in the construction leading to Definition 2.5 is the -continuity of , which allows to reduce various computations to elementary tensor product manipulations. See [4] for illustrations.
Proposition 2.6**.**
Let , let be self-adjoint operators and . If , then
[TABLE]
Proof.
By Theorem 2.2(2.2), is well defined.
For any , set J_{l,r}=\bigl{[}\frac{l}{r},\frac{l+1}{r}\bigr{)} and for , consider
[TABLE]
Since is continuous,
[TABLE]
in . Hence for any ,
[TABLE]
in . Comparing with Definition 2.1, we deduce (2.5). ∎
Remark 2.7*.*
(i) In the case when , Theorem 2.2(2.2) has a simple proof and the constant appearing in (2.2) is . More generally it can be shown that for any bounded continuous function , is well defined. Then the above proof implies that \big{[}\Gamma^{A_{1},\ldots,A_{n+1}}(\varphi)\big{]}(X_{1},\ldots,X_{n})=T_{\varphi}^{A_{1},\ldots,A_{n+1}}(X_{1},\ldots,X_{n}) for any . These facts, which will not be used in this paper, are left as an exercise for the reader.
(ii) Let and be as in Proposition 2.6 and let . Then the mapping extends to a bounded -linear map from into , and (2.5) holds true for any in . This follows from Theorem 2.2(2.1), Proposition 2.6 and the density of in .
3. Differentiability in ,
In this section we prove our main results on differentiability of functions of operators in -norms, .
We start by defining Gâteaux and Fréchet differentiability of operator functions. The first order Gâteaux and Fréchet differentiability as well as higher order Fréchet differentiability are standard concepts (see, e.g., [24, Chapter I, Sections B and F]). In this paper we understand higher order Gâteaux differentiability in the sense described below.
Let , , . By [3, 21], the function
[TABLE]
is well defined for every .
Definition 3.1*.*
Let . A function is said to be times Gâteaux -differentiable at if
- (i)
The function defined by (3.1) is times differentiable at [math].
- (ii)
is a bounded homogeneous transformation of order for any .
The transformation is called the th Gâteaux derivative of at and denoted .
Let . By a -neighborhood of , we mean the set , where is a neighborhood of [math]. Elements of are possibly unbounded self-adjoint operators.
Definition 3.2*.*
Let . A function is said to be times Fréchet -differentiable at if it is times Fréchet -differentiable in a -neighborhood of and there is a -linear bounded operator
[TABLE]
satisfying
[TABLE]
as , , for all .
We further say that is times continuously Fréchet -differentiable at if it is times Fréchet -differentiable in a -neighborhood of and for small ,
[TABLE]
as , for all .
For and , define
[TABLE]
A thorough look at Definition 3.2 shows that is times Fréchet -differentiable at (resp. times continuously Fréchet -differentiable at ) if and only if is times Fréchet differentiable at [math] (resp. times continuously Fréchet differentiable at [math]) in the usual sense of differential calculus.
Since , it follows from standard functional analysis that if is times Fréchet -differentiable at , then it is also times Gâteaux -differentiable at and
[TABLE]
If is bounded, then all the above definitions make sense if f is a locally Lipschitz function. Indeed, the definition of an operator only depends on the restrictions of to the spectra of and , which are compact subsets of .
Our main results are stated below.
Theorem 3.3**.**
Let , , and satisfy . Then is times continuously Fréchet -differentiable at every and
[TABLE]
for every , and all .
Theorem 3.4**.**
Let , . Let satisfy and . Then is times continuously Fréchet -differentiable at every and
[TABLE]
for every , and all .
Remark 3.5*.*
Under the assumptions of either Theorem 3.3 or Theorem 3.4, we will actually prove the following stronger results.
- (i)
For every , and given , there exists such that for all and for every with ,
[TABLE]
- (ii)
Given , there exists such that for every with and for all ,
[TABLE]
Since on , the results stated above imply Theorems 3.3 and 3.4.
We have the following strengthening of operator differentiability in the case of a bounded operator .
Theorem 3.6**.**
Let , , and let be a locally Lipschitz function. Then is times continuously Fréchet -differentiable at every bounded operator and (3.6) holds if and only if .
We also establish th order Gâteaux differentiability of under relaxed assumptions on .
Theorem 3.7**.**
Let , . Let satisfy . Then is times continuously Fréchet -differentiable and the following assertions hold.
- (i)
For any , any , and any , there exists such that implies
[TABLE] 2. (ii)
*The function is times Gâteaux -differentiable at every , with *
[TABLE]
for all .
Finally, as a consequence of Theorem 3.7, we will obtain the following estimate for operator Taylor remainders. It generalizes the analogous result of [23, Theorem 4.1] from bounded to unbounded operators .
Theorem 3.8**.**
Let , and . Let satisfy and let . Denote
[TABLE]
Then,
[TABLE]
The rest of this section is dedicated to the proofs of our main results.
The next proposition extends the result of [10, Proposition 7.14] from to the case of a general .
Proposition 3.9**.**
Let be a locally Lipschitz function, , . Then, the following assertions hold.
- (i)
If is times Gâteaux -differentiable at every bounded self-adjoint operator, then is times differentiable on and are bounded on compact subsets of . Moreover, if is times Gâteaux -differentiable at every self-adjoint operator, then are bounded on . 2. (ii)
If is times Fréchet -differentiable at every bounded self-adjoint operator, then .
Proof.
Let be a sequence of mutually orthogonal rank one orthogonal projections with , and note . Let be a sequence in and define
[TABLE]
We note that is a self-adjoint operator satisfying . Furthermore, is bounded if and only if is bounded.
(i) Assume that is times Gâteaux -differentiable at . For any and any ,
[TABLE]
hence
[TABLE]
By the composition rule, this implies that is times differentiable on .
Moreover for any , for any and for any , we have
[TABLE]
Hence
[TABLE]
for any .
Applying (3.11) to the bounded sequences implies that are bounded on compact subsets of whenever is times Gâteaux -differentiable at every bounded self-adjoint operator. Applying (3.11) to all sequences implies that are bounded whenever is times Gâteaux -differentiable at every self-adjoint operator.
(ii) By part (i), is times differentiable. It follows from (3.10) that
[TABLE]
uniformly in . Hence, given , there exists such that
[TABLE]
whenever and .
Fix and let be a sequence in converging to . Then, there exists such that for every , , we have . Applying (3.12) with and implies
[TABLE]
and applying (3.12) with and implies
[TABLE]
Therefore, whenever , implying
[TABLE]
for every sequence converging to , for every . Thus, is continuous. ∎
We continue with important technical lemmas. All operators in the next statements are well defined thanks to Theorem 2.2.
Lemma 3.10**.**
Let , , , and , . Let be self-adjoint operators with , let . Then, for every ,
[TABLE]
Proof.
If , then (3.10) follows from [4, Corollary 4.4] because the transformations and given by Definitions 2.1 and 2.5 coincide on (see Proposition 2.6).
If , then , so (3.10) holds for all .
Let and recall that , with
[TABLE]
Assume that and . Let be such that
[TABLE]
For brevity, we introduce the notations
[TABLE]
and
[TABLE]
We have
[TABLE]
Since resolvent strongly converges to , by [4, Proposition 3.1] and (3.14), the first group of summands in (3.17) satisfies
[TABLE]
By (3.10) applied in to the second group of summands in (3.17),
[TABLE]
[TABLE]
By [4, Proposition 3.1] and (3.14), for every ,
[TABLE]
that is, given , there exists such that for every natural ,
[TABLE]
Given , let be such that
[TABLE]
By Theorem 2.2(2.2), we obtain
[TABLE]
Combining (3.21) and (3.22) implies
[TABLE]
Combining (3.17)–(3) and (3.23) implies (3.10) for and , .
Approximating each by a sequence in the -norm and passing to the limit in
[TABLE]
as with use of the estimate in Theorem 2.2 completes the proof of (3.10) in the full generality. ∎
A useful straightforward consequence of Lemma 3.10 is stated below.
We will frequently use the notation for any operator .
Lemma 3.11**.**
Let , , , . Let be self-adjoint operators with , let . Then,
[TABLE]
Proof.
We have
[TABLE]
which along with Lemma 3.10 implies the result. ∎
Proof of Theorem 3.3.
We prove this theorem by induction on . The base of induction and the induction step can be proved in a completely analogous way, so we demonstrate the latter and omit the former.
We show below that if the result holds for , then it also holds for . Consider and . Since the result holds for , we have
[TABLE]
By Lemma 3.11, for every ,
[TABLE]
Note that
[TABLE]
[TABLE]
It follows from Lemma 3.10 that for every ,
[TABLE]
By a reasoning similar to the one in the proof of Lemma 3.11,
[TABLE]
Combining (3) and (3.29) and then applying Theorem 2.2 ensures that for every ,
[TABLE]
Combining the latter with (3.27) implies
[TABLE]
as . Hence, is times Fréchet -differentiable at and (3.5) holds. By the principal of mathematical induction we obtain that satisfies Remark 3.5(i), that is times Fréchet -differentiable at and that (3.5) holds for every .
To prove Remark 3.5(ii), and hence the continuity property (3.3), we apply (3.5) with , Lemma 3.11, and Theorem 2.2. For any and for small , we have
[TABLE]
which yields the result. ∎
The following lemma on continuity of a multiple operator integral is the last auxiliary result needed to prove Theorem 3.4.
Lemma 3.12**.**
Let , , . Let , . Then, for every there exists such that for all self-adjoint and all the estimate
[TABLE]
holds whenever satisfies .
Proof.
In this proof we adopt the notations (3.15) and (3.16).
Assume first that , so that . By Lemma 3.10,
[TABLE]
By the inequality , representation (3.34) and Theorem 2.2,
[TABLE]
Assume now that , . Given , there exists such that and
[TABLE]
We have
[TABLE]
[TABLE]
Combining (3) for , (3.37), (3) guarantees that if
[TABLE]
then (3.12) holds. ∎
Proof of Theorem 3.4.
It follows from Theorem 3.3 that is at least times Fréchet -differentiable at every and (3.6) holds for .
Our goal is to show that the statement of Remark 3.5(i) holds, that is
[TABLE]
as , , for all .
Combining (3) and (3.25) for gives
[TABLE]
Since
[TABLE]
for every , it follows from (3) and Lemma 3.12 that (3) holds.
To prove the continuity property stated in Remark 3.5(ii) (and hence to prove (3.3)), we recall (3) and note
[TABLE]
Then by Lemma 3.12,
[TABLE]
as , , for all , yielding the result. ∎
Proof of Theorem 3.6.
The necessary condition is proved in Proposition 3.9. For any and for any bounded interval , there exists a function with compact support such that and coincide on . Since the definition of an operator only depends on the restrictions of to the spectra of and , the sufficient condition is an immediate consequence of Theorem 3.4. ∎
Proof of Theorem 3.7.
The fact that is times continuously Fréchet differentiable follows from Theorem 3.3. The Gâteaux differentiability in the case is proved in [10, Theorem 7.18].
Furthermore, (ii) follows from (i) applied with . Hence it suffices to establish (i).
Let . We fix and and we let . Let be as in Lemma 2.3. By Theorem 3.6 and Remark 3.5, is times Fréchet -differentiable at and given , there exists such that implies
[TABLE]
We have
[TABLE]
The first two lines are treated by (3). By (3.5) and Lemma 2.3,
[TABLE]
Hence,
[TABLE]
By (3.5) and Lemma 3.11, the first difference in (3.43) equals
[TABLE]
Likewise, the second difference in (3.43) equals
[TABLE]
By letting in (3.43)–(3.45) we obtain
[TABLE]
Combining (3.43)–(3.46) implies
[TABLE]
[TABLE]
To treat , we note that by Lemma 3.11, for every and every ,
[TABLE]
where, for any , is a permutation of the -tuple
[TABLE]
Hence, by Theorem 2.2(2.1) and by ,
[TABLE]
Let be such that
[TABLE]
Combining (3.47)–(3.49) implies
[TABLE]
We now deal with . Applying Lemma 2.3 gives
[TABLE]
for every . Hence, by Theorem 2.2(2.1),
[TABLE]
By taking as in (3.50), we deduce from the latter that
[TABLE]
Let be chosen as in (3), where satisfies (3.50). It follows from (3), (3), (3.51), (3.52) that if , then (i) holds. ∎
Proof of Theorem 3.8.
Existence of the derivatives is justified by Theorem 3.7. By Lemma 3.10 and induction on , we obtain
[TABLE]
The estimate (3.9) follows from the latter representation and Theorem 2.2. ∎
4. Differentiability in ,
In this section we demonstrate that the functions proved to be Gâteaux differentiable with respect to the operator norm in [19] are continuously Fréchet differentiable with respect to the -norm, .
Theorem 4.1**.**
Let and . Then is times continuously Fréchet -differentiable, , at every and
[TABLE]
for every , and all .
The proof of Theorem 4.1 is completely analogous to the proof of Theorem 3.4 and is based on the counterparts of Lemmas 3.10, 3.11, 3.12 for Besov functions stated below.
The following perturbation formula is a higher order extension of the analogous formulas proved in [3] and [19, Theorem 5.1 and Lemma 5.4] for and , respectively.
Lemma 4.2**.**
Let , , and . Let be self-adjoint operators with , , let . Then, for every ,
[TABLE]
Remark 4.3*.*
We note that the result of Lemma 4.2 for is a particular case of the result of Lemma 3.10. The proof in the case is based on the integral projective tensor product representation of for . The latter representation is not available for a general with , which is treated in Lemma 3.10.
As an immediate consequence of Lemma 4.2, we obtain the following analog of Lemma 3.11.
Lemma 4.4**.**
Let , , and . Let be self-adjoint operators with , , let . Then,
[TABLE]
We also need the analog of Lemma 3.12 proved below.
Lemma 4.5**.**
Let , , and . Then, for every there exists such that for all self-adjoint and all , , the estimate
[TABLE]
holds whenever satisfies .
Proof.
In this proof we adopt the notations (3.15) and (3.16).
For each , let , where is defined in (2.4). Then, and
[TABLE]
By Lemma 4.2,
[TABLE]
By the representation (4.4) and Theorem 2.4,
[TABLE]
Given , let be such that
[TABLE]
We have
[TABLE]
[TABLE]
Combining (4.5), (4.7), (4) guarantees that if
[TABLE]
then (4.5) holds. ∎
Proof of Theorem 4.1.
The result is proved by induction on . Note that by a known property of Besov spaces, contains for every .
The base of induction, case , is known. The Fréchet differentiability and (4.1) for follow from the Gâteaux differentiability established in [18, Theorem 2], properties of double operator integrals derived in [3], properties of Besov spaces, and the fact that every Gâteaux differentiable function whose derivative is a bounded linear operator continuously depending on the point of differentiation (see [24, Lemma 1.15]) is Fréchet differentiable.
We have
[TABLE]
Thus, by Lemma 4.5, the Fréchet differential of is continuous.
The inductive step is proved along the lines of the one in Theorem 3.4 with replacement of Lemmas 3.10, 3.11, 3.12 by Lemmas 4.2, 4.4, 4.5, respectively. ∎
Acknowledgement.
A.S. is grateful to the Université de Franche-Comté, Besançon for hospitality during her work on this project. The authors are grateful to the anonymous referee for the careful reading and relevant suggestions regarding the presentation of some of the proofs.
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