Volume 2013, Issue 1 246343
Research Article
Open Access

Boundedness of Solutions for a Class of Sublinear Reversible Oscillators with Periodic Forcing

Tingting Zhang

Tingting Zhang

School of Mathematics, Shandong University, Jinan, Shandong 250100, China sdu.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: 11 June 2013
Academic Editor: Wenchang Sun

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

It is well known that the longtime behavior for periodically forced planar systems can be very intricate. For example, there are equations having unbounded solutions but with infinitely many zeros and with nearby unbounded solutions having randomly prescribed number of zeros and also periodic solutions; see [1]. In contrast to such unbounded phenomenon Littlewood [2] suggested to study the boundedness of all the solutions of the following differential equation:
()
in the following two cases:
  • (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.

The first result in superlinear case is obtained by Morris [3], who showed that all solutions of
()
are bounded, where e(t) ∈ C0. Later, a series results in superlinear case were obtained by several authors, see [413] and references therein. However, in general, it is harder to study the Lagrange stability of sublinear systems since smoothness of sublinear term is insufficient. There are only a few works in sublinear case so far. In 1999, Küpper and You [14] proved the first result in the study of the equation
()
where 0 < α < 1 and p(t) ∈ C(𝕋). Later, Liu [15] proved the same result for more general equation
()
where g(x) ∈ C6 satisfying the sublinear condition (ii) and some inequalities, and e(t) ∈ C5(𝕋). In 2004, Ortega and Verzini [16] studied the boundedness of (4) in a special case with the variational method. In 2009, Wang [17] gave a sufficient and necessary condition for the boundedness of all solutions for sublinear equation
()
where e(t), p(t) ∈ C5(𝕋).
As is widely known, there is a deep similarity between reversible and Hamiltonian dynamics. Many fundamental results of the Hamiltonian systems possess reversible counterparts. On boundedness problem for sublinear reversible systems, the first results were obtained by Li [18], later, Yang [19], in the study of a sublinear reversible systems
()
Recently, Wang [20] gave a sufficient and necessary condition for the boundedness of all solutions of the differential equation
()
with 0 < α < 1, γ ≠ 0.
By the discussions about the sublinear Hamiltonian equation (1.3) in [17] motivations, we will study the boundedness of all solutions for a sublinear reversible system like
()
where B ≠ 0 and 0 < α < 1. Furthermore, we also show that (8) has solutions of Mather type. The results obtained in [1820] can be regarded as corollary of result of this paper.

Remark 1. Using the method of this paper we also can consider the more general equation

()
provided of adding suitable conditions for g(x). For convenience, we only consider the case g(x) ≡ x.

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).

Throughout this paper, we denote two universal positive constants without regarding their values by c < 1 and C ≥ 1, and suppose that the following conditions hold:
  • (A1)

    f(x) ∈ C4(), 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 = /;

  • (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 ≤ iq − 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

()
is a Denjoys minimal set.

2. Reversible Systems and Action-Angle Variables

In this section, we will assume that B > 0 and A > 0. Firstly, we consider (8) which is equivalent to the following system:
()
where . Then we can obtain that (13) is reversible with respect to the transformation (x, z)↦(−x, z) by (A1).

Lemma 5. There exists a G-invariant diffeomorphism (x, y)→(x, z) such that (13) is transformed into the following system:

()
where .

Proof. Introduce a transformation Ψ:

()
where U(x, t) will be determined later. Under this transformation, the system (13) is transformed into a new system as follows:
()
Now, we define the function U(x, t) by
()
Since , so we can obtain U(x, t) = ɛE(t)|x|α−1x. Then the new system can be expressed as in (14) by direct computation.

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.

Let us consider the auxiliary system
()
which is a time-independent Hamiltonian system with Hamiltonian
()

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.

Assume that (S(t), C(t)) is the solution of (18) with initial conditions (S(0), C(0)) = (0,1), and let T0 > 0 be the minimal period. We can find that S(t) and C(t) satisfy
  • (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.

Then we introduce the transformation
()
which is
()
where b = 2/(3 + α). It is easy to see that 1/2 < b < 2/3 by 0 < α < 1. Since (S(−t), C(−t)) = (−S(t), C(t)), this transformation is invariant with respect to the involutions (ρ, φ)↦(ρ, −φ) and (x, y)↦(−x, y), and we can find that the mapping Φ is a generalized canonical transformation by (iv). In fact,
()
where d = ((1 − b)T0) −1.
Under the transformation Φ, the system (18) is transformed into the simpler form
()
where h0(ρ) = ((2 − 2b)T0) −1 · ρ2(1−b).
The original system (13) is transformed into the system
()
where
()
Let
()
Clearly, x is odd in φ and y is even in φ by the definitions of S(t) and C(t). Thus, by the evenness of P(t) and the oddness of f(x) and E(t) we have
()
This implies that system (24) is reversible with respect to the involutions (ρ, φ)↦(ρ, −φ).

Lemma 6. For 0 ≤ k + m ≤ 4, the following inequalities hold:

  • (1)

    |(k/ρk)l1(ρ, φ)| ≤ Cρk+2−γ−(5/2)b,

  • (2)

    |(k+m/ρktm)l2(ρ, φ, t)| ≤ Cρk+a,

  • (3)

    |(k+m/ρktm)l3(ρ, φ, t)| ≤ Cρk+3−4b,

  • (4)

    |(k+m/ρktm)l4(ρ, φ, t)| ≤ Cρk+3−4b,

  • (5)

    |(k/ρk)h1(ρ, φ)| ≤ Cρk+1−γ−(5/2)b,

  • (6)

    |(k+m/ρktm)h2(ρ, φ, t)| ≤ Cρk+τ,

  • (7)

    |(k+m/ρktm)h3(ρ, φ, t)| ≤ Cρk+2−4b,

where γ = βb, a = max (3 − (9/2)bγ, 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

()
where 0 ≤ i1, i2, i3k. Meanwhile, is a sum terms of the form
()
Hence, we obtain
()
by the assumptions on f(x) and the definitions of x(ρ, φ) and y(ρ, φ).

(2) From the expression of l2(ρ, φ, t), we have

()

We can find that

()
where a = max (3 − 9b/2 − γ, 1 − b).

(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

()
Hence, we can know that
()
where τ = max (3 − 6b, −b).

(7) From the expression of h3(ρ, φ, t), we have

()

For λ0 > 0, we define the domain
()

Lemma 7. There exists a G-invariant diffeomorphism Ψ1:

()
such that for some I < I0 < I+. Under this transformation, (24) is transformed into the system
()
where
()
with
()

Proof. Define a transformation Φ1 by

()
By
()
we get
()
()
Let , φ = θ. The system (24) is transformed into (41).

Lemma 8. For I large enough, the following conclusions hold:

  • (i)

    |kU1(I, θ)/Ik| ≤ CIk+1−γb/2,

  • (ii)

    U1(I, −θ) = U1(I, θ).

Proof. In view of

()
we obtain
()
By |(k/ρk)V1(ρ, φ)| ≤ Cρk+1−γb/2, we have |(/ρ)V1(ρ, φ)| ≤ Cργb/2 ≤ 1/2 for ρ large enough. Hence, U1 is uniquely determined by the contraction mapping principle. Moreover, , for some I0 > 0, as a consequence of the implicit function theorem and
()

Above all, if k = 1, from (47) and (49), we get

()

We note that

()
and the right side hand is sum of the term
()
where 1 ≤ sk, k1 + ⋯+ks = k, ki ≥ 1  (for  1 ≤ is). The highest order term in U1 is the one with s = 1, namely, (V1/ρ)·(k(I + U1)/Ik). We move the part (V1/ρ)·(kU1/Ik) to the left hand side of (52). Since |(/ρ)V1(ρ, φ)| ≤ 1/2 for ρ large enough, this also provides immediately a bound on kU1(I, θ)/Ik. The rest part |(V1/ρ)·(kI/Ik)| ≤ CIk+1−γb/2.

Now, we proceed inductively by assuming that for jk − 1 the estimates

()
hold and we wish to conclude that the same estimate holds for j = k.

Indeed, if s ≥ 2, we have

()
by
()
This proves (i) of Lemma 8.

Now we check (ii). In fact, since

()
we have
()
From (47), we have |(/ρ)V1(ρ, φ)| ≤ 1/2 for II0 sufficiently large and therefore we obtain U1(I, θ) = U1(I, −θ).

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

()
(2) Since
()
we can prove that
()
Their proofs are similar to the proofs in (1).

Next, we check the last part of   . We get

()
by the estimate in Lemma 6 and the definition of a.

(3) It is clearly by (3) in Lemma 6.

(4) It is clearly by (4) in Lemmas 6 and 8.

(5) We have that

()
From the last inequalities and (5) in Lemma 6, we obtain
()
(6) Since
()
we just have to prove that
()
In fact,
()
so we have proved (6).

(7) We have

()
by (7) in Lemma 6.

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.

We define the functions η0, η1, η2, η3, ξ1, ξ2, and ξ3 as
()
Then system (41) is equivalent to the following system:
()

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)| ≤ CIk−1−γ+3b/2,

  • (3)

    |(k+m/Iktm)η2(I, θ, t)| ≤ CIk+τ+4b−2,

  • (4)

    |(k+m/Iktm)η3(I, θ, t)| ≤ CIk,

  • (5)

    |(k+m/Iktm)ξ1(I, θ, t)| ≤ CIk+a+2b−1,

  • (6)

    |(k+m/Iktm)ξ2(I, θ, t)| ≤ CIk+2−2b,

  • (7)

    |(k+m/Iktm)ξ3(I, θ, t)| ≤ CIk+2−2b, for 0 ≤ k + m ≤ 4.

Proof. (1) It is clear.

(2) Note that 1 − 2b > 1 − γ − 2b/5, and

()
it follows that
()
as I ≫ 1.

Moreover, we also have

()
So
()
From (72) and (74), it is easy to see that
()
(3) We have
()
By (72), 1 − 2b > τ (τ = max (3 − 6b, −b)) and 1 − 2b > 2 − 4b, we have
()
for I ≫ 1.

Let . We find that

()
so
()

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.

When m = 0, then

()
by a > 2 − γ − 5b/2.

(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

()

Let t = t, θ = θ, r = η0(I) and
()
where I(r) is the inverse function of r = η0(I).
Then system (70) is transformed into the following form:
()
Moreover, one can verify that system (86) is reversible with respect to involution G : (t, r)↦(−t, r).

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)| ≤ Crk−(1 + γ − 3b/2)/(2b−1),

  • (2)

    |(k+m/rktm)F1(r, θ, t)| ≤ C(rk+(τ + 4b − 2)/(2b−1) + ɛrk),

  • (3)

    |(k+m/rktm)F2(r, θ, t)| ≤ C(rk+(a + 4b − 3)/(2b−1) + ɛrk),

  • (4)

    |(k+m/rktm)F3(r, θ, t)| ≤ Cɛrk.

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

()
(4) We have that
()

Lemma 12. The time 1 map Φ1 of the flow Φθ of the system (86) is of the form

()
where . And there exists a μ0 > 0 such that, for 0 ≤ k + m ≤ 4, sufficiently large r and sufficiently small ɛ,
()
hold. Moreover, the map Φ1 is reversible with respect to the involution G : (t, r)↦(−t, r).

Proof. Since

()
then we get is bounded.

Let αT0 | S(υT0)|α−1C(υT0) = S1(υ). Set (r(θ), t(θ)) = Φθ(r, t) with Φ0 = id for the flow:

()
Since
()
where X denotes the vector field of the system (86), we have
()
which is equivalent to the following equations for D1 and D2:
()

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

()
Next, we will prove that T is a contraction map. From the definition of T(D), we have
()
by Lemma 11 and the boundedness of . Then we have
()
by the definition of the norm ∥·∥.

Using the contraction principle, one verifies easily that for rr0, (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:

()
In order to prove (93), we just need to prove that
()
hold for k + m ≤ 4.

(1) When k + m = 0,

()
where μ0 = min ((1 + γ − 3b/2)/(2b − 1), (2 − 4bτ)/(2b − 1), (3 − 4ba)/(2b − 1)).

(2) When m = 0 and k ≠ 0, we check the case when k = 1 firstly

()
Hence,
()
Now, we proceed inductively by assuming that for j < k − 1 the estimates
()
hold and we wish to conclude that the same estimate holds for j = k
()
where s + ν ≤ 2. Hence,
()

(3) We can prove that

()
similarly to (2) when m ≠ 0.

(4) we have that

()
Hence,
()

(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.

Consider (8) which is equivalent to the following system:
()
Replacing (18) by an “auxiliary” system
()
Under the transformation (21), the system (113) is transformed into the form
()
where
()
Thus, the system (115) can be written in the form
()
From the equality
()
it follows that
()
Hence, the function is C1, 1-periodic and change the sign. Since |S(T0φT0)| = |S(φT0)| for any φ ∈ [0,1], there exists φ1 ∈ (0,1/2) such that
()
That is, . In view of
()
we find
()
Hence, we obtain that or is negative. This proves that there exists a φ* such that and . Therefore, there are υ > 0 and δ0 > 0 such that for φ ∈ [φ*υ, φ* + υ] and for φ ∈ (φ*υ, φ*), for φ ∈ (φ*, φ* + υ). Let
()
Then, if J is sufficiently large, on the set 𝒦J,υ, we have
()
()
From (117) and (124) we obtain, for t ≥ 0,
()
Moreover, for ρ(t, ρ0, φ0) > J and φ(t, ρ0, φ0)∈[φ*υ, φ*υ/2]∪[φ* + υ/2, φ* + υ], we have
()
From (126) and (127), it follows that any solution (ρ(t, ρ0, φ0), φ(t, ρ0, φ0)) of (115) with the initial condition (ρ(0, ρ0, φ0), φ(0, ρ0, φ0)) = (ρ0, φ0) ∈ 𝒦J,υ always stays in 𝒦J,υ and satisfies ρ(t, ρ0, φ0) > δt + ρ(0) with , for all t ≥ 0. The proof of Theorem 3 is completed.

5. The Proof of Theorem 4

In this section, we will prove Theorem 4 by using the abstract result on the existence of quasi-periodic solutions proved in [24] in the context Aubry-Mather theory for reversible systems. We only need to show that the Poincaré map (92) has the monotone property; that is,
()
We can get that
()
by Lemma 11, and
()
by Lemma 12. Then we have
()
where c0 ≥ 1 − ɛ. Therefore, we have
()
as r ≫ 1 and ɛ ≪ 1. This proves the validity of (128).

Acknowledgments

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

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