Volume 2013, Issue 1 386812
Research Article
Open Access

Reducibility for a Class of Almost-Periodic Differential Equations with Degenerate Equilibrium Point under Small Almost-Periodic Perturbations

Wenhua Qiu

Wenhua Qiu

School of Mathematics, Shandong University, Jinan, Shandong 250100, China sdu.edu.cn

School of Mathematics and Statistics, Zaozhuang University, Zaozhuang, Shandong 277160, China uzz.edu.cn

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Jianguo Si

Corresponding Author

Jianguo Si

School of Mathematics, Shandong University, Jinan, Shandong 250100, China sdu.edu.cn

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First published: 24 November 2013
Academic Editor: Svatoslav Staněk

Abstract

This paper focuses on almost-periodic time-dependent perturbations of an almost-periodic differential equation near the degenerate equilibrium point. Using the KAM method, the perturbed equation can be reduced to a suitable normal form with zero as equilibrium point by an affine almost-periodic transformation. Hence, for the equation we can obtain a small almost-periodic solution.

1. Introduction and Main Result

Reducibility of nonautonomous finite-dimensional systems with quasiperiodic coefficients has basic importance in the analysis of dynamical systems; see [1, 2]. Unfortunately, we cannot guarantee in general such reducibility. In the last years, establishing the reducibility of finite-dimensional systems by means of the KAM tools is an active field of research, and many authors are devoted to the study of reducibility of such systems. In 1996, Jorba and Simó [3] considered reducibility of the following nonlinear quasiperiodic system near an elliptic equilibrium point:
()
where A is assumed to be elliptic. Q(t, ϵ), g(t, ϵ) and h(x, t, ϵ) depend on time in a quasiperiodic way with basic frequencies (ω1, …, ωr), h(x, ωt) = O(x2) as x → 0. Under a nondegenerate condition and a nonresonant condition, using KAM iteration they proved that for most sufficiently small ϵ by an affine quasiperiodic transformation the system (1) is reducible to the following form:
()
where A* is a constant matrix close to A and h*(x, t, ϵ) = O(x2) (x → 0) is a high-order term close to h. Therefore, the system (1) has a quasiperiodic solution near the zero equilibrium point. Some similar results were obtained in [4].
Recently, Xu and Jiang [5] considered the following nonlinear quasiperiodic differential equation:
()
where n ≥ 0 is an integer, h = O(x2n+2)  (x → 0) is a higher-order term, f is a small perturbation term, and h and f are all real analytic in x and t, quasiperiodic in t with frequency ω. Under the Diophantine condition, when f is sufficiently small the differential equation (3) can be reduced to a suitable normal form with zero as equilibrium point by an affine quasiperiodic transformation, so it has a quasiperiodic solution near zero.
In 1996, Xu and You [6] considered the following linear almost-periodic differential equation:
()
where A is a constant d × d matrix with different eigenvalues λ1, …, λd and Q(t) is a d × d almost-periodic matrix with the frequency ω = (ω1, ω2, …). Under some small divisor condition, they proved that, for most sufficiently small ϵ the system (4) is reducible to the form by an affine almost-periodic transformation.
By the above inspired works [5, 6], we consider the following nonlinear almost-periodic differential equation:
()
where n ≥ 0 is an integer, A is a positive number, ϵ is a small parameter, h is a higher-order term, and f is a small perturbation term. Under some suitable conditions, we show that the differential equation (5) can be reduced to a suitable normal form with zero as equilibrium point by an affine almost-periodic transformation, so it has an almost-periodic solution near zero.

For our purpose, we first introduce some definitions and notations.

Definition 1. The function f(t) is called a quasiperiodic function of t with frequencies ω1, ω2, …, ωm, if there is a function F(θ) = F(θ1, θ2, …,θm), which is 2π-periodic in all its arguments θi  (i = 1, …, m), such that f(t) = F(ωt) = F(ω1t, ω2t, …, ωmt).

If F(θ) is analytic on a strip domain 𝕋s = {θm/2πm∣|Imθj| ≤ s,  j = 1,2, …, m}, we say that f(t) is analytic quasiperiodic on 𝕋s. Expand f(t) as a Fourier series , where and θ = ωt. Define .

Write D(0, r) = {x | x | ≤ r} and Δr,s = D(0, r) × 𝕋s.

Definition 2. Let P(x, t) be real analytic in x and t on Δr,s, and let P(x, t) be quasiperiodic with respect to t with the frequency ω. Then P can be expanded as a Fourier series as follows:

()
Define a norm by
()
where and . It is easy to see that
()

Definition 3 (see [7].)A function Δ is called an approximation function if it satisfies the following:

  • (1)

    Δ : [0, +)→[1, +), Δ(0) = 1, and Δ is a nondecreasing function;

  • (2)

    log Δ(t)/t is a decreasing function in [0, +);

  • (3)

    .

Obviously, any positive power of an approximation function is again an approximation function, so is the product of two such functions.

Definition 4 (see [8].)Suppose that is the natural number set and τ is a set composed of the subset of . We say that (τ, [·]) is the finite spatial structure on if τ satisfies the following:

  • (1)

    the empty set τ;

  • (2)

    if Λ1, Λ2τ, then Λ1 ∪ Λ2τ;

  • (3)

    Λ∈τΛ = , [] = 0 and [Λ1 ∪ Λ2]≤[Λ1]+[Λ2] ([·] is called a weight function defined in τ).

Definition 5. Assume k = (k1, k2, …) ∈ , the set

()
is called the support set of k. Consider
()
is called the weight of k, and .

Definition 6. If Q(t) = ∑Λ∈τQΛ(t) with QΛ(t) is quasiperiodic function with the frequency ωΛ = {ωii ∈ Λ}, then Q(t) is said to be almost-periodic function with the finite spatial structure (τ, [·]). If ω = (ω1, ω2, …) is the biggest subset of ∪ωΛ in the sense of integer modulus, then ω is called to be the frequency of Q(t).

If almost-periodic function Q(t) has a rapidly converging Fourier series expansion

()
where ω = (ω1, ω2, …) is the frequency and k = (k1, k2, …) have only finitely many nonzero components, then Q(t) is analytic in t.

Definition 7. Let Q(t) = ∑Λ∈τQΛ(t) with the frequency ω = (ω1, ω2, …). For m ≥ 0, s ≥ 0,

()
is called the weight norm of Q(t) in the finite spatial structure (τ, [·]).

From Definition 7, we know that |Q(t)| ≤ |||Q(t)|||0,s ≤ |||Q(t)|||m,s, for m ≥ 0, s ≥ 0.

Definition 8. Let P(x, t) = ∑Λ∈τPΛ(x, t) with the frequency ω = (ω1, ω2⋯), for m ≥ 0, s ≥ 0,

()
is called the weight norm of P(x, t) in the finite spatial structure (τ, [·]).

Let Q(t) = ∑Λ∈τQΛ(t) be almost-periodic function; then
()
is called the mean value of Q(t). The existence of the limit can be found in [9].
Throughout this paper, we assume that the following hypotheses hold
  • (H1) the functions a, h, and f are real analytic in all variables and almost-periodic in t with common frequency vector ω = (ω1, ω2, …); they also have the the finite spatial structure (τ, [·]);

  • (H2) |〈k, ω〉| ≥ α4(|k|)Δ4([k]), k∖{0}, where α > 0 is a constant and Δ is an approximation function;

  • (H3) h = 𝒪(x2n+2)  (x → 0), where n ≥ 0, and for fixed m0, s > 0, we have

    ()

Now we are ready to state the main result of this paper.

Theorem 9. Suppose that conditions (H1)–(H3) hold. Then there exists sufficiently small ϵ > 0, such that if

()
then there exists an affine real analytic almost-periodic transformation of the form x = y + u(t) such that the differential equation (5) is changed to
()
where f*(y, t) = O(y) as y → 0. Moreover, u is a real analytic almost-periodic in t with
()
and x = u(t) is also an almost-periodic solution of (5).

2. Normal Form for an Almost-Periodic Equation with Parameters

The proof of Theorem 9 is based on a norm form theorem for an almost-periodic equation with parameters. In this section, we first consider the following real almost-periodic differential equation with two parameters:
()
where [a] is the mean value of a(t). λJ = [−1,1], ξI = [−δ, δ] are parameters and Ω(ξ) = (2n + 1)ξ2n.
Let T2 and p = (ξ, λ). Denote by
()
the complex σ-neighborhood of T in the two-dimensional complex space 2.

We will invoke the KAM iteration technique to prove the following normal form theorem.

Theorem 10. Let M0 = B(I × J, σ0). Suppose that Ω and P are analytic on M0 and , respectively. Let ρ0 = s0/8 and let E0 > 0. Let K0 > 0 such that . There exists a sufficiently small E0 > 0 such that if

()
()
where
()
then there exists a real C-smooth curve in M0,
()
And for every pT, there exists an affine analytic almost-periodic transformation
()
which changes (19) to
()
with P*(y, t, p) = O(y2)  (y → 0). Moreover,
()

Furthermore, for pT, x = u*(t, p) is an analytic almost-periodic solution of the differential equation (19) with λ = λ(ξ).

Lemma 11. Let N(p) = (A + ϵ[a])ξ2n+1λ + h(p), p = (ξ, λ) ∈ M. Suppose that h is real analytic on M2 with

()
Suppose that, on the domain M, N(ξ, λ) = 0 determines implicitly a real analytic curve T : λ = λ(ξ), , such that B(T, ϵ/E) ⊂ M, where ϵ, E and σ are supposed to be well defined. Let N+(p) = (A + ϵ[a])ξ2n+1λ + h+(p), where with . Suppose that ϵ/Eϵ/4E with E > 0. Then there exists a domain of 2, M+M with dist (M+, M) ≥ ϵ/4E, such that N+ is real analytic on M+ and satisfies . If
()
then, on the domain M+, N+(p) = 0 determines implicitly a real analytic curve T+ : λ = λ+(ξ), ξIσ/2  (σ < σ), such that
()
and B(T+, ϵ/E) ⊂ M+. Moreover, one has
()

Proof. Let M+ = B(T, 3ϵ/E)∩(Iσ/2+ϵ/E × ). Since ϵ/Eϵ/4E and σσ, by B(T, ϵ/E) ⊂ M it follows easily that M+M and dist (M+, M) ≥ ϵ/4E. Using Cauchy’s estimate we have

()
By condition (29), the equation
()
determines implicitly an analytic curve on M+,
()
It follows that
()
so
()
Thus, B(T+, ϵ/E) ⊂ M+. Let E ≤ 1/2. For each p = (ξ, λ) ∈ M+, we have
()
Noting that |N+λ(p)| ≤ 2, for all pM+, and N+(p) = 0, for all p = (ξ, λ+(ξ)), we have
()
Thus we prove Lemma 11.

Lemma 12. Assume that R0(t) = ∑Λ∈τR(t) is an analytic almost-periodic function with respect to t with the frequency ω = (ω1, ω2, …); it has the finite spatial structure (τ, [·]), and

()
If
()
then there exists an almost-periodic function u(t) with the same spatial structure as R0(t), which satisfies
()
where ωu = 〈ω, ∇θu〉 is the direction derivative of u along with ω  (θ = ωt).    is the truncation of R0 with order K.

Moreover, for , ,

()

Proof. We assume

()
Insert the above formulas into the equation , and compare the coefficients on both sides, thus we can find
()
Then
()
From Definition 7,
()
Thus, u(t) = ∑Λ∈τuΛ(t) is convergent in the smaller domain with the norm .

Now we consider the following real analytic almost-periodic differential equation with parameters

()
with S(t, p) = a(t)Ω(p).

Lemma 13. Consider the above equation, where N(p) = (A + ϵ[a])ξ2n+1λ + h(p). Let and . Let , and N+(p) = (A + ϵ[a])ξ2n+1λ + h+(p). Assume the following hold.

  • (1)

    P is real analytic on Δr,s × M and satisfies

    ()

  • with 0 ≤ E < 1/2, 0 < ρ < s/2, and E = eρK.

  • (2)

    4ϵ/Eσ.

  • (3)

    N, , and h+ are real analytic on MC2 and all the assumptions of Lemma 11 hold. Let M+M be the domain defined in Lemma 11.

Then, for any pM+, there exists an affine analytic almost-periodic transformation

()
where Φ is real analytic on D(r+, s+) × M+, such that the above differential equation is transformed to
()
where S+ and P+ will be get in the proof.

Moreover, one has

()

The new perturbation term P+ satisfies

()

with

()

Proof. The proof is the standard KAM step and we divide it into several parts.

(A) Truncation. Let R = R0 + R1x with R0 = P|x=0 and R1 = Px|x=0. It follows easily that

()
Hence . Let
()
By definition, we have
()

(B) Construnction of the Transformation. Define the transformation ϕ1 : x = u(t) + y, where u satisfies

()
From Lemma 12, we have
()
By the transformation ϕ1, the equation becomes
()
()
then
()

Define the transformation ϕ2 : y = (1 + ϵQ)x+; Q satisfies

()
We assume
()

Then

()
Similar to Lemma 12, we have
()

By the transformation ϕ2, the equation becomes

()
then
()

Thus, by the transformation Φ = ϕ1ϕ2 : x = u + (1 + ϵQ)x+, the equation is transformed to

()
where
()
With the estimates of u and Q, we have
()

Let η = E1/2 ≤ 1/4, s+ = s − 2ρ, and r+ = ηr. Then the transformation Φ : x+D(0, r+) → D(0,2r+) is analytic almost-periodic on with respect to t and affine in x+.

(C) Estimates of Error Terms. Because , then 1/(1 + ϵQ) = 1 − ϵQ + (ϵQ) 2 − (ϵQ) 3 + ⋯+(−ϵQ) n + ⋯. Thus,

()
Let η = E1/2. Then, it follows that
()
So
()
where ρ+ = (1/2)ρ, r+ = ηr, E+ = cE3/2, and m+ = (1/2)m. Thus we have proved Lemma 13.

Iteration. Now we choose some suitable parameters so that the above KAM step can be iterated infinitely. At the initial step, let

()
Let K0 satisfy and σ0 = δ. Inductively, we define
()
And Kj satisfies .

By , we have . Thus, if E0 is sufficiently small, we have cEj ≤ 1 and . Moreover, by definition it follows that

()
Thus ϵj+1/Ej+1ϵj/Ej, j ≤ 0.

Now we prove that, for E0 sufficiently small, 4ϵj/Ejσj hold for all j ≤ 0.

Let Gj = 4ϵj/Ejσj; from (21) we have G0 ≤ 1. Moreover, we have

()
for all j ≤ 0. Thus, GjG0 ≤ 1. So the inequalities in the assumption 2 of Lemma 13 hold for all j ≤ 0.

Let M0 = M, N0 = (A + ϵ[a])ξ2n+1λ, h0 = 0, Ω0 = AΩ, S0 = aΩ, and P0 = P. By Lemmas 11, 12, and 13, we have a sequence of closed domains Mj with Mj+1Mj and a sequence of affine transformations

()
We also have
()
Let Φj = Φ0∘Φ1∘⋯Φj−1 with Φ0 = id. Then, after the transformation Φj, (19) is changed to
()
By the inductive assumptions of KAM iteration, we have .

The correction terms and satisfy

()
By Lemma 11, we have dist (Mj+1, Mj) ≥ ϵj−1/4Ej−1.  For Cauchy’s estimate we have
()

Noting that M0 = B(I × J, σ0) and T0 : λ = (A + ϵ[a])ξ2n+1, |ξ | ≤ δ ≤ 1. Since σ0 ≥ 4ϵ0/E0 and , it follows that M1M0 and dist (M1, M0) ≥ σ0/4. For Cauchy’s estimate we have

()

Let Fj = ϵjEj−1/ϵj−1rj; then

()
So . Obviously, we can choose E0 sufficiently small so that Rj+1/Rj ≤ 1/2, Rj+1 ≤ (1/2)Rj. Noting that h0 = 0 and ϵ0/r0σ0 ≤ 1/16, we have
()
So condition (29) holds for all j ≤ 0.

From Lemma 11, Nj(p) = (A + ϵ[a])ξ2n+1λ + hj(p) = 0 defines implicitly a real analytic curve TjMj : λ = λj(ξ), , satisfying

()
Furthermore, .

Convergence of KAM Iteration. Now we prove the convergence of KAM iteration. By the definition of Ej, if E0 is sufficiently small, it follows that

()
Therefore, we have
()

Let

()
We have
()

Thus

()
So we have the convergence of Φj to Φ on .

From (86) it is easy to show that λj is convergent on I. In fact, ϵj+1/ϵjcEj ≤ 1/2. For i > j, it follows that

()
Let , ξI. For λ0(ξ) = (A + ϵ[a])ξ2n+1, we have
()

Moreover, by Cauchy’s estimate we have

()

Let Lj = 4ϵj/σj; then Lj+1/LjcEj. Thus, it is easy to prove that is convergent uniformly on I, and so λ(ξ) is differentiable on I. In fact, in the same way as in [7], we can prove that λ(ξ) is C-smooth on I.

Since TiMiMj, for all ij, letting i we have T = {(ξ, λ)∣λ = λ(ξ),   ξIMj} and T = M* = ∩j≤0Mj. Obviously, Nj(p) → 0, for pT. Let ΩjΩ* and let PjP*. By Cauchy’s estimate we have

()
Thus P*|x=0 = 0 and DxP*|x=0 = 0. Hence P*(x, t; p) = O(x2) for pT.

Noting that and , we have

()
The proof of Theorem 10 is complete.

3. Proof of Theorem 9

Let x = ξ + y with |ξ | ≤ δ and |y | ≤ r0δ. Then (5) becomes
()
Let
()
with
()
We write h(y + ξ, t) = h(y, t, ξ) and f(y + ξ, t) = f(y, t, ξ) and decompose a(t) as , where [a] is the average of a(t) and has zero mean value. Then the differential equation (5) becomes
()
where .
Let I = [−δ, δ] and Iσ = {ξ∣dist (ξ, I) ≤ σ}. By assumption and the choice of r and δ, it is easy to see that g, h, and f are all real analytic on with r0δ, σ0δ and s0 = s. Moreover, we have that
()
where c is a constant depending on n. Note that we always use c to denote different constants in estimates. Similarly, we have and . Let δ = ϵ1/(2n+2) and let r0 = ϵ2n+1/(4n+4). Then δ2n+2 = ϵ and r0 = δ2n+1/2. Let σ0 = δ. Then it follows that
()
Now (97) is equivalent to the following parameterized differential equation:
()
where Ω(ξ) = (2n + 1)ξ2n.
Now we want to prove that if ϵ is sufficiently small, then there exists ξ*I such that at ξ = ξ* the differential equation (103) is reducible to a normal form with zero as equilibrium point. We introduce an external parameter and consider the following almost-periodic differential equation:
()
where λJ = [−1,1] is an external parameter. Obviously, (103) corresponds to (104) with λ = 0.

By Theorem 10, we will prove that there exists a smooth curve T : λ = λ(ξ), ξI, such that for (ξ, λ) ∈ T the differential equation (104) can be reduced to a normal form with zero equilibrium. Moreover, we can find ξ*I such that λ(ξ*) = 0 and then come back to the original equation (103) with ξ = ξ*.

To apply Theorem 10 to (104), we verify all the assumptions. Note that
()
Let
()
Thus when ϵ is small enough, E0 is also small. Moreover, we have
()
So all the inequalities of (21) hold. Moreover, we have
()
Thus Theorem 10 holds for (104).
Since , it follows that must have a different sign for δ > 0 sufficiently small. Thus there exists a ξ*I, such that λ(ξ*) = 0. Moreover, we have |ξ* | ≤ δ = ϵ1/(2n+2) and p* = (ξ*, 0) ∈ T. Hence, by the transformation x = Φ(y, t; p*) the differential equation (103) at ξ = ξ* is changed to
()
with P*(y, t, p*) = O(y2)  (y → 0). Therefore by the transformation x = Φ(y + ξ*, t; p*) the system (5) is changed to the form of (17). Moreover, x(t) = Φ(ξ*, t; p*) is an almost-periodic solution with the frequency ω.

Since Φ(y + ξ*, t; p*) = y + u*(t; p) + ξ*, we have x = y + u(t) with u(t) = u*(t; p) + ξ*. Noting that |ξ* | ≤ ϵ1/(2n+2), it follows that, for pT, . Thus, Theorem 9 is proved.

Acknowledgments

This work was partially supported by the National Natural Science Foundation of China (Grant nos. 10871117, 11171185) and SDNSF (Grant no. ZR2010AM013).

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