Boundedness of Solutions for a Class of Sublinear Reversible Oscillators with Periodic Forcing
Abstract
We study the boundedness of all solutions for the following differential equation x′′ + f(x)x′ + (B + εe(t)) | x|α−1x = p(t), where f(x), p(t) are odd functions, e(t) is an even function, e(t), p(t) are smooth 1-periodic functions, B is a nonzero constant, and ε is a small parameter. A sufficient and necessary condition for the boundedness of all solutions of the above equation is established. Moreover, the existence of Aubry-Mather sets is obtained as well.
1. Introduction
- (i)
superlinear case: g(x)/x → +∞ as x → ±∞;
- (ii)
sublinear case: sgn (x) · g(x)→+∞ and g(x)/x → 0 as x → ±∞. Later, one calls this subject as Littlewood boundedness problem.
Remark 1. Using the method of this paper we also can consider the more general equation
Remark 2. Adding the perturbation term ɛe(t) | x|α−1x will lead to a new difficulty for estimating |S(θT0)|α−1C(θT0) appeared in (86). Fortunately, we can easily verify that is bounded by a constant (see in the proof of Lemma 12).
- (A1)
f(x) ∈ C4(ℝ), p(t) ∈ C3(𝕋) and e(t) ∈ C3(𝕋), f(x) and p(t) are odd, e(t) is even, and e(t), p(t) are both 1-periodic functions, 𝕋 = ℝ/ℤ;
- (A2)
there is some positive constant μ such that the inequalities
() -
are satisfied for 0 ≤ i ≤ 4 and all |x | ≥ μ, where 0 < β < α/2.
We decompose e(t) as , where is the average of e(t) and has zero mean value. That is and . If we write that , then it is easy to see that A and B have the same sign when 0 < ɛ < ɛ* with .
Now we state the main results of this paper.
Theorem 3. Assume that B ≠ 0 and (A1)-(A2) hold. Then there exists an 0 < ɛ** < ɛ* such that for any 0 < ɛ < ɛ**, every solution of (8) is bounded if and only if B > 0.
Theorem 4. Under the conditions of Theorem 3, there is an ɛ0 > 0 such that, for any ω ∈ (n, n + ɛ0), (8) has a solution of Mather type with rotation number ω. More precisely:
- (i)
if ω = p/q is rational, the solutions , 1 ≤ i ≤ q − 1, are periodic solutions of period q; moreover, in this case
() - (ii)
if ω is irrational, the solution is either a usual quasi-periodic solution or a generalized one.
We recall that a solution is called generalized quasi-periodic if the closed set
2. Reversible Systems and Action-Angle Variables
Lemma 5. There exists a G-invariant diffeomorphism (x, y)→(x, z) such that (13) is transformed into the following system:
Proof. Introduce a transformation Ψ:
It is easy to know that U(−x, −t) = U(x, t) by (A1), then we can obtain that the transformation Ψ is a G-invariant diffeomorphism.
It is easy to see that H0(x, y) > 0, (x, y) ∈ R2∖{0}, H0(0,0) = 0. Note that each level line H0(x, y) = h > 0 is a close orbit of system (18), hence, all the solutions of (18) are periodic with period tending to zero as h tends to infinity.
- (i)
S(t) ∈ C2(R), C(t) ∈ C1(R);
- (ii)
(S(−t), C(−t)) = (−S(t), C(t)), (S(t + T0), C(t + T0)) = (S(t), C(t));
- (iii)
, ;
- (iv)
(1/2)C2(t)+(A/(α + 1))|S(t)|α+1 = 1/2;
- (v)
C(T0t) = 0⇔t(mod (1/4)) = 0;
- (vi)
(S(T0(1/2 − t)), C(T0(1/2 − t))) = (S(T0t), −C(T0t));
- (vii)
S(T0t) = 0⇔t(mod (1/2)) = 0.
Lemma 6. For 0 ≤ k + m ≤ 4, the following inequalities hold:
- (1)
|(∂k/∂ρk)l1(ρ, φ)| ≤ Cρ−k+2−γ−(5/2)b,
- (2)
|(∂k+m/∂ρk∂tm)l2(ρ, φ, t)| ≤ Cρ−k+a,
- (3)
|(∂k+m/∂ρk∂tm)l3(ρ, φ, t)| ≤ Cρ−k+3−4b,
- (4)
|(∂k+m/∂ρk∂tm)l4(ρ, φ, t)| ≤ Cρ−k+3−4b,
- (5)
|(∂k/∂ρk)h1(ρ, φ)| ≤ Cρ−k+1−γ−(5/2)b,
- (6)
|(∂k+m/∂ρk∂tm)h2(ρ, φ, t)| ≤ Cρ−k+τ,
- (7)
|(∂k+m/∂ρk∂tm)h3(ρ, φ, t)| ≤ Cρ−k+2−4b,
where γ = βb, a = max (3 − (9/2)b − γ, 1 − b), and τ = max (3 − 6b, −b).
Proof. (1) It is easy to know that (∂k/∂ρk)l1(ρ, φ) is a sum of terms of the form
(2) From the expression of l2(ρ, φ, t), we have
We can find that
(3) From the expression of l3(ρ, φ, t), we have
(4) From the expression of l4(ρ, φ, t), we can obtain that
(5) From the definition of h1(ρ, φ), we have
(6) From the definition of h2(ρ, φ, t), we can obtain
(7) From the expression of h3(ρ, φ, t), we have
Lemma 7. There exists a G-invariant diffeomorphism Ψ1:
Proof. Define a transformation Φ1 by
Lemma 8. For I large enough, the following conclusions hold:
- (i)
|∂kU1(I, θ)/∂Ik| ≤ CI−k+1−γ−b/2,
- (ii)
U1(I, −θ) = U1(I, θ).
Proof. In view of
Above all, if k = 1, from (47) and (49), we get
We note that
Now, we proceed inductively by assuming that for j ≤ k − 1 the estimates
Indeed, if s ≥ 2, we have
Now we check (ii). In fact, since
By the estimates in Lemma 6, we can prove the following inequalities.
Lemma 9. For 0 ≤ k + m ≤ 4, the following inequalities hold:
- (1)
,
- (2)
,
- (3)
,
- (4)
,
- (5)
,
- (6)
,
- (7)
.
Proof. (1) From the estimates (1) and (5) of Lemmas 6 and 8, it follows that
Next, we check the last part of . We get
(3) It is clearly by (3) in Lemma 6.
(4) It is clearly by (4) in Lemmas 6 and 8.
(5) We have that
(7) We have
3. The Proof of Boundedness
In this section, all the solutions of (8) which are bounded will be proved via the KAM theory for reversible systems developed by Sevryuk [21] or Moser [22, 23] if B > 0.
In addition, one can verify that system (70) is reversible with respect to involution G : (t, I)↦(−t, I).
Then some estimates on the functions ηi (i = 0,1, 2,3) and ξi (i = 1,2, 3) are given.
Lemma 10. The following inequalities hold:
- (1)
cI2b−1≤|η0(I)| ≤ CI2b−1,
- (2)
|(∂k/∂Ik)η1(I, θ)| ≤ CI−k−1−γ+3b/2,
- (3)
|(∂k+m/∂Ik∂tm)η2(I, θ, t)| ≤ CI−k+τ+4b−2,
- (4)
|(∂k+m/∂Ik∂tm)η3(I, θ, t)| ≤ CI−k,
- (5)
|(∂k+m/∂Ik∂tm)ξ1(I, θ, t)| ≤ CI−k+a+2b−1,
- (6)
|(∂k+m/∂Ik∂tm)ξ2(I, θ, t)| ≤ CI−k+2−2b,
- (7)
|(∂k+m/∂Ik∂tm)ξ3(I, θ, t)| ≤ CI−k+2−2b, for 0 ≤ k + m ≤ 4.
Proof. (1) It is clear.
(2) Note that 1 − 2b > 1 − γ − 2b/5, and
Moreover, we also have
Let . We find that
When m = 0, the proof of (3) is similar to the proof of (2).
When m > 0, then
(4) The proof of (4) is similar to the proof of (3).
(5) Let η0(I) + η1(I, θ) + η2(I, θ, t) + ɛη3(I, θ, t) = η(I, θ, t). By using the estimates on the functions and ηj (j = 0,1, 2,3), it follows that
When m = 0, then
(6) By using the estimates on the functions and ηi (i = 0,1, 2,3), it follows that
(7) By using the estimates on the functions and ηi (i = 0,1, 2,3), it follows that
It is easy to see that I ≫ 1 if and only if r ≫ 1, and the solutions of system (86) do exist on 0 ≤ θ ≤ 1 when r(0) = r ≫ 1.
By using the estimates on ηi and ξi (i = 1,2, 3) in Lemma 10, the following inequalities can be proved.
Lemma 11. For 0 ≤ k + m ≤ 4 and r ≫ 1, the following inequalities hold:
- (1)
|(∂k/∂rk)F0(r, θ)| ≤ Cr−k−(1 + γ − 3b/2)/(2b−1),
- (2)
|(∂k+m/∂rk∂tm)F1(r, θ, t)| ≤ C(r−k+(τ + 4b − 2)/(2b−1) + ɛr−k),
- (3)
|(∂k+m/∂rk∂tm)F2(r, θ, t)| ≤ C(r−k+(a + 4b − 3)/(2b−1) + ɛr−k),
- (4)
|(∂k+m/∂rk∂tm)F3(r, θ, t)| ≤ Cɛr−k.
Proof. Above all, we know that r = η0(I) = T0I2b−1, so we can get I = ((1/T0)r) 1/(2b−1). Then we have
(1) We have that
(2) We have that
(3) We have that
Lemma 12. The time 1 map Φ1 of the flow Φθ of the system (86) is of the form
Proof. Since
Let αT0 | S(υT0)|α−1C(υT0) = S1(υ). Set (r(θ), t(θ)) = Φθ(r, t) with Φ0 = id for the flow:
Let D(r, t, θ) = (D1(r, t, θ), D2(r, t, θ)), . Define ∥D∥ = :|D1 | /3 + 2 | D1 | /3, and T(D) = :(T1(D), T2(D)), where
Using the contraction principle, one verifies easily that for r ≥ r0, (98) has a unique solution in the space {|D1 | ≤ 1, |D2 | ≤ 1}. Moreover, D1 and D2 are smooth.
Next, we will estimate Q1(r, t) and Q2(r, t) as follows:
(1) When k + m = 0,
(2) When m = 0 and k ≠ 0, we check the case when k = 1 firstly
(3) We can prove that
(4) we have that
(5) We can prove (103) similarly to (4) for the left k + m ≤ 4.
Proof of Boundedness. From Theorem 1.1 in [21] we can see Φ1 possesses a sequence of invariant circles tending to infinity. So, in the original system (13), there exists a corresponding sequence of invariant tori in phase space . Then any solution of system (13) is bounded because it must stay within one of those tori.
4. The Proof of Unboundedness
In this section, we will prove that all solutions of (8) are unbounded if B < 0. In this case, A < 0.
5. The Proof of Theorem 4
Acknowledgments
This work was partially supported by the National Natural Science Foundation of China (Grant nos. 11171185, 10871117) and SDNSF (Grant no. ZR2010AM013).