Nonautonomous Differential Equations in Banach Space and Nonrectifiable Attractivity in Two-Dimensional Linear Differential Systems
Abstract
We study the asymptotic behaviour on a finite interval of a class of linear nonautonomous singular differential equations in Banach space by the nonintegrability of the first derivative of its solutions. According to these results, the nonrectifiable attractivity on a finite interval of the zero solution of the two-dimensional linear integrable differential systems with singular matrix-elements is characterized.
1. Introduction
Precisely, as a kind of singular behaviour near t = 0 of all solutions x(t) of linear integrable system (2), in Theorem 6, we involve on the matrix elements h(t) and g(t) a necessary and sufficient condition for the infiniteness of the length of every solution curve of x(t) (in our best knowledge, it is the first paper dealing with this kind of problems). Theorem 6 is a consequence of the precise asymptotic formula for all solutions x(t) near t = 0 of integrable differential system (2) presented in Lemmas 11 and 12. Of course, instead of interval (0, t0] and t → 0, we can also state our main results on [t0, ∞) and t → ∞.
In applications, the last years have seen an increasing interest in the analysis of differential equations and systems on finite time intervals. This is because the Finite-Time Stability (FTS) and the Finite-Time Lyapunov Exponent (FTLE) were introduced, respectively, in the control of systems within a finite time as well as in the Lagrangian Coherent Structure (LCS) on finite-time intervals in fluid, ocean, and atmosphere dynamics [1–3] and in the biological application [4]. It includes the time-varying vector fields known only on a finite-time interval, but not on the whole half line t ≥ t0.
In the theory of differential equations, the importance of studying the different kind of asymptotic behaviours of the nonautonomous linear differential systems comes from their application in the study of asymptotic and oscillatory behaviour of the second and higher order ordinary differential equations. For instance, in [5], authors study the asymptotic behaviour near t = ∞ of oscillatory solutions of the nonlinear second-order differential equation via the asymptotic formula for solutions of an auxiliary linear differential system having elements which are absolutely continuous functions on [t0, ∞). In [6], authors derive a precise asymptotic behaviour near t = ∞ of solutions u(t) of the third-order nonlinear differential equation u′′′ + ((m + 1)/2)uu′′ + m(1 − u′2) + M(1 − u′) = 0 such that u(0) = a, u′(0) = b, u′(∞) = 1, and 0 < u′ < 1 on [0, ∞), by using the asymptotic solution formula for the corresponding linear differential system based on Hartman and Wintner’s asymptotic integration (see [7, 8] and for its generalization [9, 10]). Similarly, in [11], authors prove an asymptotic solution formula for the second-order nonlinear differential equations depending on the asymptotic behaviour of fundamental solutions of the corresponding homogeneous equation . On certain types of asymptotic behaviour of linear and nonlinear differential and integro-differential systems, we refer reader to some recently published papers [12–14] and references therein. The attractivity of solutions of scalar delay differential equations is widely studied and it is important in mathematical biology; see, for instance, [15] and references therein.
This paper is mainly based on a part of the P.h.D degree thesis [16] of the first author.
2. Statement of the Main Results
Preliminarily, we state the following auxiliary result.
Theorem 1. For each x0 ∈ 𝕏, there exists a unique solution x of (1).
Next, we derive a necessary condition for a kind of singularities of (1) at t = 0 in terms of singular behaviour of the operator norm of A(t) near t = 0.
Theorem 2. Let there exist a solution x of (1) such that ∥x(t)∥𝕏 → 0 as t → 0. If ∥dx/dt∥𝕏 ∉ L1(0, t0), then one has:
Thus, if (3) is not satisfied, then the integrability of ∥dx/dt∥𝕏 occurs for all solutions x of (1), which is out of our interest. All results from this section will be proved in the next sections.
At the second, we impose on the operator-valued function A(t) the following structural hypotheses:
Theorem 3. Let the hypotheses (H1)-(H2) be fulfilled. Then, for every x0 ∈ 𝕏, the corresponding solution x of (1) satisfies
- (i)
∥x(t)∥𝕏 → 0 as t → 0;
- (ii)
x is an injective function on (0, t0] if and only if x0 is not an eigenvector of U−1(s)U(t) with an eigenvalue 1 for all s, t ∈ (0, t0], s ≠ t;
- (iii)
∥dx/dt∥𝕏 ∉ L1(0, t0) if and only if ωa ∉ L1(0, t0).
The meaning and importance of hypotheses (H1)-(H2) as well as the conclusions (i)–(iii) of Theorem 3 will be verified by Theorem 6, where 𝕏 = ℝ2 and (1) is a large class of two-dimensional linear differential systems.
Definition 4. The zero solution of system (8) is rectifiable attractive (resp., nonrectifiable attractive) if it is attractive and the curve Γx of every solution x of (8) is a rectifiable (resp., nonrectifiable) Jordan curve in ℝ2.
Following [17], we are interested in Jordan curves so that the parametrization of our solutions faithfully represents the length and rectifiability properties (omitting injectivity, we might find solutions that self-intersect on large sets or are just self-winding and, hence, artificially nonrectifiable).
On the rectifiability of graph of solutions of scalar second-order linear differential equations, we refer reader to [20].
Here the particular attention is paid to the case of the so-called linear integrable systems defined as follows.
Definition 5. Let ℳ2 denote the linear space of all 2 × 2 matrix with the elements in ℂ. We say that (8) is a linear integrable system if there exists an invertible matrix T ∈ ℳ2 such that for every t ∈ (0, t0] the matrix Λ(t) = T−1A(t)T ∈ ℳ2 is a diagonal matrix for every t ∈ (0, t0].
Note that the matrices A(t) are themselves always real. As commented in Section 6, we proceed with presentation of our results and arguments in terms of the coefficients of such matrices.
In Section 5, we show that the set of all matrix-valued functions A = A(t) that satisfy Definition 5 make an algebra.
This implies the third main result of the paper.
Theorem 6. Let μ2 − 4νρ < 0. One supposes (15) and
Remark 7. Under the assumptions of Theorem 6, we conclude that if g(t) ≡ 0, then the zero solution of integrable system (8) is rectifiable attractive.
Corollary 8. Let h0 > 0 and b ∈ ℝ. One has that:
As we see, in the case of a = 1, the rectifiable attractivity of (18) depends on the order of growth of the singular term t−b appearing in the antidiagonal coefficients of A(t). The existence of solutions for the integrable systems (8) and (18) is guaranteed by their explicit forms given in Lemma 11.
3. Proofs of Theorems 1, 2, and 3
In this section, we study the existence and uniqueness of solutions to (1) as well as its attractivity of the zero solution.
In the case when the operator-valued function A = A(t), A : [0, t0] → L(𝕏) is defined and continuous on the whole interval [0, t0], then the existence of a classic solution x = x(t) is well known; see, for instance, [22, Chapter 3], [23, Chapter 2], and [24, Chapter 5.1]; when A(t) are unbounded linear operators, we refer reader to [24, Chapter 5.4] and some selected papers from [25].
However, our operator-valued function A = A(t), A : (0, t0] → L(𝕏), is mainly singular and not defined at t = 0. By this reason, we cannot use the existence results and methods obtained and used on [0, t0]. One way to understand the main difficulties because of the pressumed singular behaviour of A(t) near t = 0, we can make the reflexion from t = 0 into τ = ∞ by the transformation τ = 1/t. Then, the existence of a solution of equation x′ = A(t)x, t ∈ (0, t0], x(t0) = x0, can be related with the existence of a global solution of equation , τ ∈ [τ0, ∞), where , , τ0 = 1/t0, and . Since [τ0, ∞) is an infinite interval, our approach to the existence and uniqueness of solution of (1) is motivated by the works [26–29].
Definition 9. Let (F, | · |n) be a Fréchet space. A mapping T : F → F is said to be an α-contraction on F if for each n ∈ ℕ there exists αn ∈ [0,1) such that
In applications, the inequality (21) need not be satisfied for the family of seminorms |·|n, rather only for another family of seminorms ∥·∥n which is equivalent to | · |n. Hence, the key point of the following α-contraction principle is that an operator T has a fixed point provided (21) is satisfied in ∥·∥n.
Lemma 10. Let (F, | · |n) be a Fréchet space and T : F → F be an α-contraction on F with respect to a family of seminorms ∥·∥n equivalent to | · |n. Then, T has a fixed point on F.
The previous lemma is a particular case of [29, Theorem 1.2].
Proof of Theorem 1. Let F = C((0, t0]; 𝕏), x ∈ F, and
Let T : F → F be an operator defined in (20). Since A(t) may be singular at t = 0, it is easy to check that in general T is not an α-contraction with respect to the family of seminorms |x|n given in (22).
Next, let ωn and hn be two sequences of real numbers determined by
Next, according to (20) and (23), for t ∈ [1/n, t0], we calculate
Now, we will show the uniqueness of solution of equation (1). Let u(t) and v(t) be two solutions of (1) such that u(t0) = v(t0) = x0. Integrating (1) with respect to u(t) and v(t), we obtain u = Tu and v = Tv, which yields ∥Tu−Tv∥n = ∥u−v∥n. Puting this equality into (29), we conclude that
Proof of Theorem 2. It is enough to show that if the statement (3) does not hold, then ∥dx/dt∥𝕏 ∈ L1(0, t0) for every x0 ∈ 𝕏 and the corresponding solution x of (1) such that x(t0) = x0. In fact, if we suppose contrary to (3), then there exists c0 > 0 such that ∥A(t)∥ ≤ c0, t ∈ (0, t0]. Also, because of ∥x(t)∥𝕏 → 0 as t → 0, there exists c1 > 0 such that ∥x(t)∥𝕏 ≤ c1, t ∈ (0, t0]. Hence, from (1), we obtain
Proof of Theorem 3. The conclusion (i) immediately follows from the hypothesis (H2) because as t → 0.
Next, we give the proof of the conclusion (ii). Let s, t ∈ (0, t0], s < t, be such that x0 is an eigenvector of U−1(s)U(t) with an eigenvalue 1. Then,
Finally, the conclusion (iii) follows from the hypotheses (H1)-(H2) because
Note that conclusion (ii) does not depend on any of the hypotheses (H1)-(H2).
4. Proofs of Theorem 6 and Corollary 8
In this section, we study the rectifiable and nonrectifiable attractivity of the linear integrable systems (8).
At the first, we state the following lemma in which a specific form of the matrix A(t) of linear integrable systems is proposed.
Lemma 11. Suppose that system (8) is integrable. Then, there exist functions g, h : (0, t0] → ℝ and constants μ, ν, ρ ∈ ℝ such that
Proof. Let λ1,2 : (0, t0] → ℂ be two eigenvalues of the matrix-valued function A(t). Since system (8) is supposed to be an integrable system, from Definition 5, there is a regular matrix T ∈ ℳ2 such that
We denote that
Putting previous notations in (41), we get the desired conclusion (36). Note that all of these functions and constants are real, since h is defined as a matrix-element of a real matrix, g is defined real in both cases, and the rest of the constants are necessarily real by virtue of satisfying (36). Now, the conclusion (37) immediately follows from (36).
By Theorem 1, we know that there exists a unique solution x(t) of system (8). Moreover, in the next lemma, we show that if (8) is a linear integrable system, then the solution x(t) is explicitly expressed by the matrix elements of A(t).
Lemma 12. Let x be a solution of linear integrable system (8) and let T ∈ ℳ2 be a matrix determined in Definition 5. Then, there exists a matrix-valued function U = U(t), U : (0, t0] → ℳ2, such that x(t) = U(t)x0 and satisfies the following properties:
- (1)
U(t0) is the identity matrix;
- (2)
U(t) is invertible for every t ∈ (0, t0];
- (3)
T−1U(t)T is a diagonal matrix for every t ∈ (0, t0];
- (4)
if λ(t) is an eigenvalue of A(t), then is an eigenvalue of U(t);
- (5)
U′(t) = A(t)U(t) for every t ∈ (0, t0].
Proof. Let T be the matrix that diagonalizes A(t). Let ΛA(t) = T−1A(t)T be of form
According to [23, p. 188], the matrix-valued function U(t) is called the evolution operator.
In the next lemma, we give some necessary and sufficient conditions such that the solution′s curve Γx of every solution x(t) of integrable system (8) is a Jordan curve. Results of that kind are important because Definition 4 requires the Jordan property.
Lemma 13. Let (8) be a linear integrable system such that μ2 − 4νρ < 0 and g(t) ≠ 0, t ∈ (0, t0], where the real numbers μ, ν, ρ, and g(t) are determined by Lemma 11. Then, the solution′s curve Γx of every solution x(t) is a Jordan curve in ℝ2 if and only if for every pair s, t ∈ (0, t0], s < t, at least one of the statements in (15) holds true.
Proof. In order to prove this lemma, we use the equivalence stated in the conclusion (ii) of Theorem 3 (we may use Theorem 3 because of Lemma 12; see also the remark at the end of Theorem 3). According to that, we need to find pairs s and t such that 1 is an eigenvalue of U−1(s)U(t). Since the evolution operator U(t) can be diagonalized into the form ΛU(t), we compute
Since by this argument, U−1(s)U(t) = I if and only if 1 is an eigenvalue of U−1(s)U(t), we get the full equivalence.
Proof of Theorem 6. The key point of this proof is to show that the integrable system (8) satisfies the required hypotheses (H1)-(H2), because all conclusions of Theorem 6 follow immediately from the conclusions (i), (ii), and (iii) of Theorem 3. Before we show that, we state the following two propositions which will be proved in Section 5.
Proposition 14. Let f : ℝ × ℝ → ℝ be defined by , where μ, ν, ρ are real numbers such that μ2 < 4νρ. Then, there exist constants c1, c2 > 0 such that
Proposition 15. Let Λ : (0, t0] → ℳ2 be a diagonal matrix of the form
Finally, by Lemma 13, we obtain that the solution′s curve Γx of every solution x is a Jordan curve. Thus, all assumptions of Theorem 3 are fulfilled, and, therefore, we may apply Theorem 3 here. Consequently, the proof of this theorem is complete.
Proof of Corollary 8. It is enough to show that all assumptions of Theorem 6: μ2 − 4νρ < 0, (15), (16), and (17) are fulfilled in particular for
5. Appendix
Theorem 16. The set 𝒜((0, t0]; ℳ2) is an algebra with respect to the classic matrix operations + and ∘; that is to say, if A, B ∈ 𝒜((0, t0]; ℳ2), then the following properties hold:
- (1)
αA + βB ∈ 𝒜((0, t0]; ℳ2) for all α, β ∈ ℝ;
- (2)
A∘B ∈ 𝒜((0, t0]; ℳ2);
- (3)
if det A(t) ≠ 0 for all t ∈ (0, t0], then A−1 ∈ 𝒜((0, t0]; ℳ2);
- (4)
if f : ℝ → ℝ is a real analytic function such that f(A(t)) converges absolutely for all t ∈ J, then f(A) ∈ 𝒜((0, t0]; ℳ2).
Proof. We denote the diagonal matrices ΛA = TAT1 and ΛB = TBT1.
- (1)
T(αA + βB)T−1 = αTAT−1 + βTBT−1 = αΛA + βΛB, which is diagonal.
- (2)
TABT−1 = TAT−1TBT−1 = ΛAΛB, which is diagonal.
- (3)
, which is also diagonal.
- (4)
, which is also diagonal.
Next, we give the proofs of some technical results used in previous sections for proving the main results.
Proof of Proposition 14. Denote by u ∈ ℝ2 the vector u = (x, y). It is enough to show that f = f(u) is a norm as a function f : ℝ2 → ℝ, since all the norms in ℝ2 are equivalent [30, p. 38], which, by definition, is the claim of this lemma. Let
Proof of Proposition 15. Let ϕ(t):(0, t0] → ℝ be such that λ(t) = |λ(t) | eiϕ(t). Then, ; so, for any z = (z1, z2) ∈ ℂ2, we have
6. Final Remarks
In our approach to the model over ℝ2, we have chosen to emphasize the a priori structure of the real matrices describing the integrable systems. Thus, we have stated and proved this theory in terms of such real functions, complexifying only when absolutely necessary.
We could have taken another approach, complexifying from the start and then easily diagonalizing all the relevant matrices, but this would not essentially simplify any argument except in notation, while we would run the risk of confusing the reader even further about which term or function is real and which one is complex.