具有零平均扰动的退化可逆谐振子的响应解

Pub Date : 2023-10-15 DOI:10.1007/s10114-023-1539-6
Xin Yu Guan, Jian Guo Si, Wen Si
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引用次数: 0

摘要

在本文中,我们考虑一类常退化的拟周期强迫可逆系统,该系统是作为一组谐振子的扰动获得的,$$\left\{\dotrix{\dot x=y+{f_1}(ωt,x,y),}\hfill\cr{\ddot y=\lambda{x^l}+{f _2}其中0≠λ∈ℝ, l>;1是整数,对应的对合G是(-θ,x,−y)→ (θ,x,y)。在[22]中已经证明了上述可逆系统的响应解的存在性,如果[f2(ωt,0,0)]满足一些非零平均条件(参见[22]中的条件(H)),这里[·]表示\({\mathbb{t}^d}\)上连续函数的平均值。然而,当[f2(ωt,0,0)]=0时,由于必须求解退化的隐函数,讨论上述系统的响应解的存在性会遇到困难。这篇文章将朝着这个方向努力。本文的目的是考虑[f2(ωt,0,0)]=0的情况。更准确地说,在2p<;l、 如果f2满足\([{f_2}(\ωt,0,0)]=[{\partial{f_2}(\ωt,,0)}\ over{\ppartial x}}]=[{{\pPartial ^2}(ωt,0,0)}\over{\ partial x ^2}}}]=\cdots=[{{\fpartial ^{p-1}}}(\ωt,0)}\ over{\partil{x ^{p-1}}]=0\),则\(λ^{-1}{{\partial ^p}{f_2}(ωt,0,0)}\在{\ppartial{x^p}}}上]<;0\)当l−p是偶数时,或者当l−p是奇数时,我们得到以下结果:(1)对于\(\tilde\lambda<;0\)(参见(2.2)中的\;(2) 对于足够小的\(\tilde\lambda<;0\)和\*,存在具有几乎全Lebesgue测度的Cantor集\({\cal E}\ in(0,{_*})\),使得如果ω满足丢番图条件,则每个\(\ in{\ccal E})都存在响应解。在剩余的情况下,其中\({\lambda ^{-1}}[{{\spartial ^p}{f_2}(\omega t,0,0)}\ over{\sPartial{x^p}}}]>;0\)和l−p是偶数时,我们证明了该系统在大多数区域不允许有响应解。
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Response Solutions for Degenerate Reversible Harmonic Oscillators with Zero-average Perturbation

In this paper, we consider a class of normally degenerate quasi-periodically forced reversible systems, obtained as perturbations of a set of harmonic oscillators,

$$\left\{ {\matrix{{\dot x = y + {f_1}(\omega t,x,y),} \hfill \cr {\dot y = \lambda {x^l} + {f_2}(\omega t,x,y),} \hfill \cr } } \right.$$

where 0 ≠ λ ∈ ℝ, l > 1 is an integer and the corresponding involution G is (−θ, x, −y) → (θ, x, y). The existence of response solutions of the above reversible systems has already been proved in [22] if [f2(ωt, 0, 0)] satisfies some non-zero average conditions (See the condition (H) in [22]), here [ · ] denotes the average of a continuous function on \({\mathbb{T}^d}\). However, discussing the existence of response solutions for the above systems encounters difficulties when [f2(ωt, 0, 0)] = 0, due to a degenerate implicit function must be solved. This article will be doing work in this direction. The purpose of this paper is to consider the case where [f2(ωt, 0, 0)] = 0. More precisely, with 2p < l, if f2 satisfies \([{f_2}(\omega t,0,0)] = [{{\partial {f_2}(\omega t,0,0)} \over {\partial x}}] = [{{{\partial ^2}{f_2}(\omega t,0,0)} \over {\partial {x^2}}}] = \cdots = [{{{\partial ^{p - 1}}{f_2}(\omega t,0,0)} \over {\partial {x^{p - 1}}}}] = 0\), either \({\lambda ^{ - 1}}[{{{\partial ^p}{f_2}(\omega t,0,0)} \over {\partial {x^p}}}] < 0\) as lp is even or \({\lambda ^{ - 1}}[{{{\partial ^p}{f_2}(\omega t,0,0)} \over {\partial {x^p}}}] \ne 0\) as lp is odd, we obtain the following results: (1) For \(\tilde \lambda < 0\) (see \({\tilde \lambda }\) in (2.2)) and ϵ sufficiently small, response solutions exist for each ω satisfying a weak non-resonant condition; (2) For \(\tilde \lambda < 0\) and ϵ* sufficiently small, there exists a Cantor set \({\cal E} \in (0,{_ * })\) with almost full Lebesgue measure such that response solutions exist for each \( \in {\cal E}\) if ω satisfies a Diophantine condition. In the remaining case where \({\lambda ^{ - 1}}[{{{\partial ^p}{f_2}(\omega t,0,0)} \over {\partial {x^p}}}] > 0\) and lp is even, we prove the system admits no response solutions in most regions.

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