Reducibility for a Class of Almost-Periodic Differential Equations with Degenerate Equilibrium Point under Small Almost-Periodic Perturbations
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
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 = {θ ∈ ℂm/2πℤm∣|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 ∈ ℂ | 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:
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 ℕ is the natural number set and τ is a set composed of the subset of ℕ. We say that (τ, [·]) is the finite spatial structure on ℕ if τ satisfies the following:
- (1)
the empty set ∅ ∈ τ;
- (2)
if Λ1, Λ2 ∈ τ, then Λ1 ∪ Λ2 ∈ τ;
- (3)
⋃Λ∈τΛ = ℕ, [∅] = 0 and [Λ1 ∪ Λ2]≤[Λ1]+[Λ2] ([·] is called a weight function defined in τ).
Definition 5. Assume k = (k1, k2, …) ∈ ℤ∞, the set
Definition 6. If Q(t) = ∑Λ∈τQΛ(t) with QΛ(t) is quasiperiodic function with the frequency ωΛ = {ωi∣i ∈ 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
Definition 7. Let Q(t) = ∑Λ∈τQΛ(t) with the frequency ω = (ω1, ω2, …). For m ≥ 0, s ≥ 0,
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,
-
(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〉| ≥ α/Δ4(|k|)Δ4([k]), k ∈ ℤ∞∖{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
2. Normal Form for an Almost-Periodic Equation with Parameters
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
Furthermore, for p ∈ T, 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+1 − λ + h(p), p = (ξ, λ) ∈ M. Suppose that h is real analytic on M ⊂ ℂ2 with
Proof. Let M+ = B(T, 3ϵ/E)∩(Iσ/2+ϵ/E × ℂ). Since ϵ/E ≤ ϵ−/4E− and σ ≤ σ−, by B(T, ϵ−/E−) ⊂ M it follows easily that M+ ⊂ M and dist (M+, ∂M) ≥ ϵ−/4E−. Using Cauchy’s estimate we have
Lemma 12. Assume that R0(t) = ∑Λ∈τR0Λ(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
Moreover, for , ,
Proof. We assume
Now we consider the following real analytic almost-periodic differential equation with parameters
Lemma 13. Consider the above equation, where N(p) = (A + ϵ[a])ξ2n+1 − λ + h(p). Let and . Let , and N+(p) = (A + ϵ[a])ξ2n+1 − λ + 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 = e−ρK.
- (2)
4ϵ/E ≤ σ.
- (3)
N, , and h+ are real analytic on M ⊂ C2 and all the assumptions of Lemma 11 hold. Let M+ ⊂ M be the domain defined in Lemma 11.
Then, for any p ∈ M+, there exists an affine analytic almost-periodic transformation
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
(B) Construnction of the Transformation. Define the transformation ϕ1 : x = u(t) + y, where u satisfies
Define the transformation ϕ2 : y = (1 + ϵQ)x+; Q satisfies
Then
By the transformation ϕ2, the equation becomes
Thus, by the transformation Φ = ϕ1∘ϕ2 : x = u + (1 + ϵQ)x+, the equation is transformed to
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,
Iteration. Now we choose some suitable parameters so that the above KAM step can be iterated infinitely. At the initial step, let
By , we have . Thus, if E0 is sufficiently small, we have cEj ≤ 1 and . Moreover, by definition it follows that
Now we prove that, for E0 sufficiently small, 4ϵj/Ej ≤ σj hold for all j ≤ 0.
Let Gj = 4ϵj/Ejσj; from (21) we have G0 ≤ 1. Moreover, we have
Let M0 = M, N0 = (A + ϵ[a])ξ2n+1 − λ, 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+1 ⊂ Mj and a sequence of affine transformations
The correction terms and satisfy
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 M1 ⊂ M0 and dist (M1, ∂M0) ≥ σ0/4. For Cauchy’s estimate we have
Let Fj = ϵjEj−1/ϵj−1rj; then
From Lemma 11, Nj(p) = (A + ϵ[a])ξ2n+1 − λ + hj(p) = 0 defines implicitly a real analytic curve Tj ⊂ Mj : λ = λj(ξ), , satisfying
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
Let
Thus
From (86) it is easy to show that λj is convergent on I. In fact, ϵj+1/ϵj ≤ cEj ≤ 1/2. For i > j, it follows that
Moreover, by Cauchy’s estimate we have
Let Lj = 4ϵj/σj; then Lj+1/Lj ≤ cEj. 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 Ti ⊂ Mi ⊂ Mj, for all i ≥ j, letting i → ∞ we have T = {(ξ, λ)∣λ = λ(ξ), ξ ∈ I ⊂ Mj} and T = M* = ∩j≤0Mj. Obviously, Nj(p) → 0, for p ∈ T. Let Ωj → Ω* and let Pj → P*. By Cauchy’s estimate we have
Noting that and , we have
3. Proof of Theorem 9
By Theorem 10, we will prove that there exists a smooth curve T : λ = λ(ξ), ξ ∈ I, 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*.
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 p ∈ T, . 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).