On the Differentiability of Weak Solutions of an Abstract Evolution Equation with a Scalar Type Spectral Operator
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
- (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*).
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].
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 f ∈ X and g* ∈ X*, let v(f, g*, ·) be the total variation of the complex-valued measure 〈EA(·)f, g*〉 on ℬ.
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
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*),
Let n ≥ 2 and let the interval I be not a singleton. Then differentiating (3.4) at an arbitrary t ∈ I, we obtain
Since
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),
The fact that etAf ∈ D(An), t ∈ I, implies by the properties of the o.c. and [2], Proposition 3.1, that, for any g* ∈ X*,
Therefore, for any g* ∈ X*,
For an arbitrary segment [a, b]⊆I, we have
Let us fix an arbitrary a ∈ I and integrate (3.15) for k = 1 between a and an arbitrary t ∈ I. Considering the strong continuity of AetAf, t ∈ I, we have
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
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)
For any n = 1,2, …, t ≥ 0 and an arbitrary g* ∈ X*,
For the latter one, we have
By the properties of the o.c. and [2], Proposition 3.1, (4.2) and (4.4) imply that
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:
The latter implies in particular that the points λn are distinct (λi ≠ λj, i ≠ j).
Since, for any n = 1,2, …, the set
By choosing a unit vector en ∈ EA(Δn)X (∥en∥ = 1), n = 1,2, …, we obtain a vector sequence such that
As is readily verified, (4.14) implies that the vectors {e1, e2, …} are linearly independent.
Moreover, there is an ɛ > 0 such that
Suppose that the sequence is bounded above, that is, there is such an ω > 0 that
Therefore (see Section 1), y(t): = etAf, 0 ≤ t < ∞, is a weak solution of (1.1) on [0, ∞).
Let
Considering (4.18) and (4.15), we have
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
By (4.14),
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),
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)
For any n = 1,2, …, t > 0, and an arbitrary g* ∈ X*,
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 ℂ.
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
“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 {λ ∈ σ(A)∣ − b−ln | Im λ | < Reλ ≤ 0} is unbounded;
- (2)
for any b− > 0, the set {λ ∈ σ(A)∣ − b−ln | Im λ | < Reλ ≤ 0} is bounded.
In the first case, the set is unbounded with the very b− > 0, for which the set {λ ∈ σ(A)∣ − b−ln | Im λ | < 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 {λ ∈ σ(A)∣0 < Reλ < b+ln | Im λ|} 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:
Since, for any n = 1,2, …, the set
By the properties of the s.m., the latter implies
By choosing a unit vector en ∈ EA(Δn)X (∥en∥ = 1), n = 1,2, …, we obtain a vector sequence such that
First, assume that the sequence is bounded, that is, there is an ω > 0 such that
Therefore (see Section 1), y(t): = etAf, 0 ≤ t < ∞, is a weak solution of (1.1) on [0, ∞).
Let
Taking (4.50) and (4.51) into account, we have
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
Without restricting generality, we can regard that
For any λ ∈ Δn(k), k = 1,2, …, by (4.46), (4.47), and (4.59),
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
Therefore (see Section 1), y(t): = etAf, 0 ≤ t < ∞, is a weak solution of (1.1) on [0, ∞).
Let
Taking into account (4.50) and (4.51), we have
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.