Volume 2011, Issue 1 825951
Research Article
Open Access

On the Differentiability of Weak Solutions of an Abstract Evolution Equation with a Scalar Type Spectral Operator

Marat V. Markin

Corresponding Author

Marat V. Markin

Department of Partial Differential Equations, Institute of Mathematics, National Academy of Sciences of Ukraine, 3 Tereshchekivs′ka Street, 01601 Kiev, Ukraine nas.gov.ua

Search for more papers by this author
First published: 22 May 2011
Citations: 1
Academic Editor: Palle E. Jorgensen

Abstract

For the evolution equation y(t) = Ay(t) with a scalar type spectral operator A in a Banach space, conditions on A are found that are necessary and sufficient for all weak solutions of the equation on [0, ) to be strongly infinite differentiable on [0, ) or [0, ). Certain effects of smoothness improvement of the weak solutions are analyzed.

1. Introduction

Consider the evolution equation
(1.1)
with a scalar type spectral operator A in a complex Banach space X.
Following [1], we understand by a weak solution of equation (1.1) on an interval [0, T) (0 < T) such a vector function y : [0, T) → X that
  • (1)

    y(·) is strongly continuous on [0, T);

  • (2)

    for any g*D(A*),

    (1.2)

  • (D(·) is the domain of an operator, A* is the operator adjoint to A, and 〈·, ·〉 is the pairing between the space X and its dual X*).

As was shown [2], Theorem 4.2, the general weak solution of (1.1) on [0, T) (0 < T) is as follows:
(1.3)
the operator exponentials etA, 0 ≤ t < T, defined in the sense of the operational calculus for scalar type spectral operators (see Section 2).

Here, we are to find conditions on A that are necessary and sufficient for all weak solutions of (1.1) on [0, ) to be strongly infinite differentiable on [0, ) or (0, ).

This goal attained; all the principal results of paper [3] and the corresponding ones of [4] obtain their natural generalizations.

2. Preliminaries

Henceforth, unless specified otherwise, let A be a scalar type spectral operator in a complex Banach space X with a norm ∥·∥, EA(·) its spectral measure (the resolution of the identity), and σ(A) the operator′s spectrum, with the latter being the support for the former.

Observe that, in a Hilbert space, the scalar type spectral operators are those similar to the normal ones [5].

For scalar type spectral operators, there has been developed an operational calculus for Borel measurable functions defined on σ(A) [6, 7]. With F(·) being such a function, a new scalar type spectral operator
(2.1)
is defined as follows:
(2.2)
where
(2.3)
(χα(·) is the characteristic function of a set α) and
(2.4)
are bounded scalar type spectral operators on X defined in the same manner as for normal operators (see, e.g., [8, 9]).
In particular,
(2.5)
The properties of the spectral measure, EA(·), and the operational calculus underlying our discourse are exhaustively delineated in [6, 7]. We will outline here a few noteworthy facts.
Due to its strong countable additivity, the spectral measure EA(·) is bounded [10], that is, there is an M > 0 such that
(2.6)
( is the σ-algebra of Borel sets in the complex plane ).

Observe that ∥·∥ is used in (2.6) to designate the norm in the space of bounded linear operators on X. We will adhere to this rather common economy of symbols adopting the same notation for the norm in the dual space X* as well.

For any fX and g*X*, let v(f, g*, ·) be the total variation of the complex-valued measure 〈EA(·)f, g*〉 on .

As we discussed in [4, 11], with F(·) being an arbitrary Borel measurable function on , for any fD(F(A)), g*X*, and δ,
(2.7)
where M > 0 is the constant from (2.6).
In particular, for F(λ) = 1, λ, and δ = (or any Borel set containing σ(A)), we have
(2.8)
Further, for a Borel measurable nonnegative function F(·) on , a δ, and a sequence of pairwise disjoint Borel sets in ,
(2.9)
Indeed, since for the spectral measure [6, 7]
(2.10)
for the total variation, we have
(2.11)
Whence, due to nonnegativity of F(·) [12],
(2.12)
We shall need the following regions in the complex plane:
(2.13)
where b+ and b are positive constants.

The terms spectral measure and operational calculus frequently referred to will be abbreviated to s.m. and o.c., respectively.

3. Differentiability of a Particular Weak Solution

Proposition 3.1. Let n = 1,2, … and I be a subinterval of an interval [0, T)  (0 < T). A weak solution y(·) of (1.1) on [0, T) is n times strongly differentiable on I if and only if

(3.1)
in which case,
(3.2)

Proof. “Only if” part.

Let n = 1,2, … and suppose that a weak solution y(·) of (1.1) on [0, T) is n times strongly differentiable on a subinterval I⊆[0, T).

Then for any g*D(A*),

(3.3)
Hence, by the closedness of the operator A (cf. [1]),
(3.4)
This concludes proving the “only if” part for n = 1, in which case, as is to be noted, the subinterval I can shrink to a single point t ∈ [0, T).

Let n ≥ 2 and let the interval I be not a singleton. Then differentiating (3.4) at an arbitrary tI, we obtain

(3.5)
with the increments Δt being such that t + Δ ∈ I.

Since

(3.6)
by the closedness of A, we infer that
(3.7)
Considering (3.4) and (3.7),
(3.8)
Continuing inductively in this manner, we arrive at
(3.9)
“If” part.

Let y(·) be a weak solution of (1.1) on an interval [0, T) (0 < T) such that for an n = 1,2, … and a subinterval I⊆[0, T),

(3.10)
As was discussed (see Section 1),
(3.11)
with some f ∈ ⋂0≤t<TD(etA).

The fact that etAfD(An), tI, implies by the properties of the o.c. and [2], Proposition 3.1, that, for any g*X*,

(3.12)
Given a k = 1, …, n and an arbitrary tI, let us choose a segment [a, b] ⊂ I (a < b) so that t is its midpoint if 0 < t < T or a = 0 if t = 0. For increments Δt such that at + Δtb and any g*X*, we have
(3.13)
Indeed, for any k = 1, …, n and an arbitrary λσ(A),
(3.14)

Therefore, for any g*X*,

(3.15)
For Δm : = {λ∣|λ| ≤ m}, m = 1,2, …, let us fix an arbitrary k = 1, …, n and consider the sequence of vector functions
(3.16)
Since fD(AketA), tI, by the properties of the o.c.,
(3.17)
Due to the boundedness of Δm, m = 1,2, …, by the properties of the o.c., AEAm), m = 1,2, …, is a bounded linear operator on X (∥AEAm)∥≤4Mm, m = 1,2, …, [7]). Hence, the vector functions
(3.18)
are strongly continuous on I.

For an arbitrary segment [a, b]⊆I, we have

(3.19)
Hence, for any k = 1, …, n, the vector function AketAf, tI, is strongly continuous on I, being the uniform limit of the sequence of strongly continuous on I vector functions on any segment [a, b]⊆I.

Let us fix an arbitrary aI and integrate (3.15) for k = 1 between a and an arbitrary tI. Considering the strong continuity of AetAf, tI, we have

(3.20)
Whence, as follows from the Hahn-Banach Theorem,
(3.21)
By the strong continuity of AetAf, tI,
(3.22)
Consequently, by (3.15), for n = 2,
(3.23)
Whence, analogously,
(3.24)
Continuing inductively in this manner, we infer that, for any k = 1, …, n,
(3.25)

Corollary 3.2. Let I be a subinterval of an interval [0, T)  (0 < T). A weak solution y(·) of (1.1) on [0, T) is strongly infinite differentiable on I if and only if

(3.26)
in which case,
(3.27)

Thus, we have obtained generalizations of Proposition 4.1 and Corollary 4.1 of [3], respectively.

4. Differentiability of Weak Solutions

Theorem 4.1. Every weak solution of (1.1) on [0, ) is strongly infinite differentiable on [0, ) if and only if there is a b+ > 0 such that the set is bounded.

Proof. “If” part.

Let b+ > 0 be such that the set is bounded and y(·) a weak solution of (1.1) on [0, ). Then (see Section 1)

(4.1)
with some

For any n = 1,2, …, t ≥ 0 and an arbitrary g*X*,

(4.2)
Indeed, the former integral is finite due to the boundedness of the set , the finiteness of the measure v(f, g*, ·) and the continuity of the integrated function on .

For the latter one, we have

(4.3)
Further, for any n = 1,2, … and t ≥ 0,
(4.4)
Indeed, since, due to the boundedness of the set , the set is void for all sufficiently large m′s,
(4.5)
In addition to this
(4.6)

By the properties of the o.c. and [2], Proposition 3.1, (4.2) and (4.4) imply that

(4.7)

Then, by Corollary 3.2, y(·) is strongly infinite differentiable on [0, ).

“Only if” part.

We will prove this part by contrapositive.

Assume that, for any b+ > 0, the set is unbounded.

In particular, for any n = 1,2, …, unbounded is the set .

Hence, we can choose a sequence of points in the complex plane as follows:

(4.8)

The latter implies in particular that the points λn are distinct (λiλj, ij).

Since, for any n = 1,2, …, the set

(4.9)
is open in , there exists an ɛn > 0 such that this set along with the point λn contains the open disk of radius ɛn centered at λn
(4.10)
Then, for any λ ∈ Δn, n = 1,2, …,
(4.11)
Further, since the points λn, n = 1,2, …, are distinct, we can regard the radii of the disks, ɛn, n = 1,2, …, to be small enough so that
(4.12)
Whence, by the properties of the s.m.,
(4.13)
Observe also, that the subspaces EAn)X, n = 1,2, …, are nontrivial since Δnσ(A) ≠ , with Δn being an open set.

By choosing a unit vector enEAn)X (∥en∥ = 1), n = 1,2, …, we obtain a vector sequence such that

(4.14)
(δij is the Kronecker delta symbol).

As is readily verified, (4.14) implies that the vectors {e1, e2, …} are linearly independent.

Moreover, there is an ɛ > 0 such that

(4.15)
Indeed, the opposite implies the existence of a subsequence such that
(4.16)
Then, for any k = 1,2, …, by selecting a vector fn(k) ∈ span ({ejj = 1,2, …,   jn(k)}) such that ∥en(k)fn(k)∥<dn(k) + 1/k, considering (4.14) and (2.6), we arrive at the contradiction:
(4.17)
As follows from the Hahn-Banach Theorem, for any n = 1,2, …, there is an such that
(4.18)
Concerning the sequence of the real parts, , there are two possibilities: it is either bounded or unbounded above.

Suppose that the sequence is bounded above, that is, there is such an ω > 0 that

(4.19)
Let
(4.20)
By (4.14),
(4.21)
For any t ≥ 0 and an arbitrary g*X*,
(4.22)
Similarly, for any t ≥ 0,
(4.23)
By [2], Proposition 3.1, (4.22) and (4.23) imply that

Therefore (see Section 1), y(t): = etAf, 0 ≤ t < , is a weak solution of (1.1) on [0, ).

Let

(4.24)
(cf. (4.18)).

Considering (4.18) and (4.15), we have

(4.25)
Similarly to (4.22),
(4.26)
Whence, by [2], Proposition 3.1, y(0) = fD(A).

Consequently, by Proposition 3.1, the weak solution y(t) = etAf, 0 ≤ t < , of (1.1) on [0, ) is not strongly differentiable at 0.

Now, assume that the sequence is unbounded above.

Therefore, there is a subsequence such that

(4.27)
Then the vector
(4.28)
is well defined.

By (4.14),

(4.29)
For any t ≥ 0 and an arbitrary g*X*, similar to (4.22),
(4.30)
Indeed, for all sufficiently large k′s, n(k) − t ≥ 1 and by (4.27),
(4.31)
Analogously, for an arbitrary t ≥ 0,
(4.32)

From (4.30) and (4.32), by [2], Proposition 3.1, we infer that f ∈ ⋂0≤t<D(etA).

Therefore (see Section 1), y(t): = etAf, 0 ≤ t < , is a weak solution of (1.1) on [0, ).

For any λ ∈ Δn(k), k = 1,2, …, by (4.11), (4.12), and (4.27),

(4.33)
Hence, for λ ∈ Δn(k), k = 1,2, …,
(4.34)
Using this estimate, we obtain
(4.35)
Whence, by [2], Proposition 3.1, y(0) = fD(A).

Therefore, by Proposition 3.1, the weak solution y(t) = etAf, 0 ≤ t < , of (1.1) on [0, ) is not strongly differentiable at 0.

With every possibility concerning considered, we infer that the opposite to the assumption that, for a certain b+ > 0, the set is bounded, allows to single out a weak solution of (1.1) on [0, ) that is not strongly differentiable at 0, much less strongly infinite differentiable on [0, ).

Thus, the “only if” part has been proved by contrapositive.

Theorem 5.1 of [3] has been generalized.

Theorem 4.2. Every weak solution of (1.1) on [0, ) is strongly infinite differentiable on (0, ) if and only if there is a b+ > 0 such that, for any b > 0, the set is bounded.

Proof. “If” part.

Let b+ > 0 be such that, for an arbitrary b > 0, the set is bounded.

Let y(·) be a weak solution of (1.1) on [0, ). Then (see Section 1)

(4.36)
with some f ∈ ⋂0≤t<D(etA).

For any n = 1,2, …, t > 0, and an arbitrary g*X*,

(4.37)

The first integral in this sum is finite due the boundedness of the set , the finiteness of the measure v(f, g*, ·), and the continuity of the integrated function on .

The finiteness of the second integral is proved in absolutely the same manner as for the corresponding integral in the proof of the “if” part of Theorem 4.1.

Finally for the third one, considering that b > 0 is arbitrary and setting b : = nt−1, we have

(4.38)
Further, for any n = 1,2, … and t > 0,
(4.39)
Indeed, since, due to the boundedness of the set , the set is void for all sufficiently large m′s,
(4.40)
Similarly to the “if” part of Theorem 4.1 and (4.38), we have
(4.41)
By the properties of the o.c. and [2], Proposition 3.1, (4.37) and (4.39) imply that
(4.42)
Whence, by Corollary 3.2, y(·) is strongly infinite differentiable on (0, ).

“Only if” part.

As well as in Theorem 4.1, we will prove this part by contrapositive.

Thus, we assume that, for any b+ > 0, there is such a b > 0 that the set is unbounded.

Let us show that this assumption can even be strengthened. To wit: there is such a b > 0 that, for any b+ > 0, the set is unbounded.

Indeed, there are two possibilities:

  • (1)

    for a certain b > 0, the set {λσ(A)∣ − bln  | Imλ | < Reλ ≤ 0} is unbounded;

  • (2)

    for any b > 0, the set {λσ(A)∣ − bln  | Imλ | < Reλ ≤ 0} is bounded.

In the first case, the set is unbounded with the very b > 0, for which the set {λσ(A)∣ − bln  | Imλ | < Reλ ≤ 0} is unbounded, and an arbitrary b+ > 0.

In the second case, based on the premise we infer that, for any b+ > 0, the set {λσ(A)∣0 < Reλ < b+ln  | Imλ|} is unbounded. Then so is the set for any b > 0 and b+ > 0.

Thus, let us fix a b > 0 such that the set is unbounded for an arbitrary b+ > 0.

In particular, for any n = 1,2, …, the set is unbounded.

Hence, we can select a sequence of points in the complex plane in the following manner:

(4.43)
The latter, in particular, implies that the points λn are distinct.

Since, for any n = 1,2, …, the set

(4.44)
is open in , there exists such an ɛn > 0 that this set, along with the point λn, contains the open disk of radius ɛn centered at λn
(4.45)
Hence, for any λ ∈ Δn, n = 1,2, …,
(4.46)
Since the points λn are distinct, we can regard the radii of the disks, ɛn, to be small enough so that
(4.47)

By the properties of the s.m., the latter implies

(4.48)
Observe that the subspaces EAn)X, n = 1,2, …, are nontrivial since Δnσ(A) ≠ , Δn being an open set.

By choosing a unit vector enEAn)X (∥en∥ = 1), n = 1,2, …, we obtain a vector sequence such that

(4.49)
In the same manner as in the proof of Theorem 4.1, one can show that there is an ɛ > 0 such that
(4.50)
As follows from the Hahn-Banach Theorem, for any n = 1,2, …, there is an such that
(4.51)
Concerning the sequence of the real parts, , there are two possibilities: it is either bounded or unbounded.

First, assume that the sequence is bounded, that is, there is an ω > 0 such that

(4.52)
Let
(4.53)
By (4.49),
(4.54)
In absolutely the same fashion as it was done in the case of bounded above sequence in the proof of the “only if” part of Theorem 4.1, it is shown that f ∈ ⋂0≤t<D(etA).

Therefore (see Section 1), y(t): = etAf, 0 ≤ t < , is a weak solution of (1.1) on [0, ).

Let

(4.55)
(cf. (4.51)).

Taking (4.50) and (4.51) into account, we have

(4.56)
Thus,
(4.57)
Whence, by the properties of the o.c. and [2], Proposition 3.1, y(1) = eAfD(A).

Consequently, by Proposition 3.1, the weak solution y(t) = etAf,   0 ≤ t < , of (1.1) on [0, ) is not once strongly differentiable on (0, ).

Now, assume that the sequence is unbounded. Therefore, there is a subsequence such that

(4.58)
Suppose that Reλn(k) as k.

Without restricting generality, we can regard that

(4.59)
Considering this case just like the analogous one in the proof of the “only if” part of Theorem 4.1, one can show that the vector
(4.60)
belongs to ⋂0≤t<D(etA) and, hence, (see Section 1) y(t): = etAf, 0 ≤ t < , is a weak solution of (1.1) on [0, ).

For any λ ∈ Δn(k), k = 1,2, …, by (4.46), (4.47), and (4.59),

(4.61)
Hence, for λ ∈ Δn(k), k = 1,2, …,
(4.62)
Using this estimate, we have
(4.63)
Whence, by the properties of the o.c. and [2], Proposition 3.1, y(1) = eAfD(A).

Therefore, by Proposition 3.1, the weak solution y(t) = etAf, 0 ≤ t < , of (1.1) on [0, ) is not once strongly differentiable on (0, ).

Now, suppose that Reλn(k) → − as k.

Without restricting generality, we can regard that

(4.64)
Let
(4.65)
For any t ≥ 0 and an arbitrary g*X*,
(4.66)
Analogously, for an arbitrary t ≥ 0,
(4.67)
From (4.66) and (4.67), by [2], Proposition 3.1, we infer that f ∈ ⋂0≤t<D(etA).

Therefore (see Section 1), y(t): = etAf, 0 ≤ t < , is a weak solution of (1.1) on [0, ).

Let

(4.68)
(cf. (4.51)).

Taking into account (4.50) and (4.51), we have

(4.69)
For any λ ∈ Δn(k), k = 1,2, …, by (4.47) and (4.64),
(4.70)
Hence, for λ ∈ Δn(k), k = 1,2, …,
(4.71)
Using these estimates, we have
(4.72)
Whence, by the properties of the o.c. and [2], Proposition 3.1, .

Therefore, by Proposition 3.1, the weak solution y(t) = etAf, 0 ≤ t < , of (1.1) on [0, ) is not once strongly differentiable on (0, ).

With every possibility concerning considered, we infer that the opposite to the assumption that there is a b+ > 0 such that, for any b > 0, the set is bounded, allows to single out a weak solution of (1.1) on [0, ) that is not once strongly differentiable on (0, ), much less strongly infinite differentiable on (0, ).

Thus, the “only if” part has been proved by contrapositive.

Theorem 5.2 of [3] and Theorem 4.1 of [4] have been generalized.

5. Certain Effects of Smoothness Improvement

As we observed in the proofs of the “only if” parts of Theorems 4.1 and 4.2, the opposits to the “if” parts’ premises imply that there is a weak solution of (1.1) on [0, ), which is not strongly differentiable at 0 or, respectively, once strongly differentiable on (0, ).

Therefore, the case of finite strong differentiability of the weak solutions is superfluous and we obtain the following effects of smoothness improvement.

Proposition 5.1. If every weak solution of (1.1) on [0, ) is strongly differentiable at 0, then all of them are strongly infinite differentiable on [0, ).

Proposition 5.2. If every weak solution of (1.1) on [0, ) is once strongly differentiable on (0, ), then all of them are strongly infinite differentiable on (0, ).

These statements generalize Propositions 6.1 and 6.2 of [3], respectively, the latter agreeing with the case when A is a linear operator (not necessarily spectral of scalar type) generating a C0-semigroup (cf. [1, 13]).

6. Final Remarks

Due to the scalar type spectrality of the operator A, all the above criteria are formulated exclusively in terms of its spectrum, no restrictions on the operator′s resolvent behavior necessary, which makes them inherently qualitative and more transparent than similar results for C0-semigroups (cf. [14]).

If a scalar type spectral A generates a C0-semigroup (cf. [15]), we immediately obtain the results of paper [4] regarding infinite differentiability.

Acknowledgment

The author would like to express his gratitude to Mr. Michael and Jonell McCullough.

      The full text of this article hosted at iucr.org is unavailable due to technical difficulties.