“…(see [2,7,10,13] etc.) In order to prove the existence of such invariant curves for every $< <1, it suffices to verify that for every $< <1, the Poincare map P satisfies all the assumptions of a variant of Moser's small twist theorem which is due to Ortega [16]. In the rest of this part, we will give an expression for (…”
Section: An Expression Of the Poincare Map Of (511)mentioning
confidence: 98%
“…As far as we know, this is the first nontrivial result of boundedness in a semilinear case. Recently, further results have appeared in [16] and [10] for semilinear Duffing equations.…”
mentioning
confidence: 97%
“…The Poincare map of the transformed system is closed to a so-called twist map in R 2 "D. Then a variant of Moser's twist theorem [16] guarantees the existence of arbitrarily large invariant curves diffeomorphic to circles and surrounding the origin in the (x, x$)-plane. Every such curve is the base of a time-periodic and flow-invariant cylinder in the extended phase space (x, x$, t) # R 2 _R, which confines the solutions in the interior and which leads to a bound of these solutions.…”
“…(see [2,7,10,13] etc.) In order to prove the existence of such invariant curves for every $< <1, it suffices to verify that for every $< <1, the Poincare map P satisfies all the assumptions of a variant of Moser's small twist theorem which is due to Ortega [16]. In the rest of this part, we will give an expression for (…”
Section: An Expression Of the Poincare Map Of (511)mentioning
confidence: 98%
“…As far as we know, this is the first nontrivial result of boundedness in a semilinear case. Recently, further results have appeared in [16] and [10] for semilinear Duffing equations.…”
mentioning
confidence: 97%
“…The Poincare map of the transformed system is closed to a so-called twist map in R 2 "D. Then a variant of Moser's twist theorem [16] guarantees the existence of arbitrarily large invariant curves diffeomorphic to circles and surrounding the origin in the (x, x$)-plane. Every such curve is the base of a time-periodic and flow-invariant cylinder in the extended phase space (x, x$, t) # R 2 _R, which confines the solutions in the interior and which leads to a bound of these solutions.…”
“…On the other hand, the sublinear and semilinear cases are relatively new fields; see [4], [9], [10], [11], [12], [13], [17], [18], [19] and the references therein for details.…”
Abstract. In this paper we will study the boundedness of all solutions for second-order differential equationswhere λ ∈ R and g(x) satisfies the sublinear growth condition. Since the system in general is non-Hamiltonian, we have to introduce reversibility assumptions to apply the twist theorem for reversible mappings. Under some suitable conditions we then obtain the existence of invariant tori and thus the boundedness of all solutions.
“…Later Liu [11] and Ortega [21] improved the result for the cases 1/`a+1/`b ¥ Q and 1/`a+1/`b ¥ R 0 Q, respectively. Further results have appeared in [12,13,22,27] for semilinear Duffing's equation.…”
In this paper we will prove the boundedness of all the solutions and the existence of quasiperiodic solutions for the second order scalar differential equation ẍ+arctan x=ee (t), where e is a small parameter and the 1-periodic function e(t) is a smooth function.
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