{"title":"具有零平均扰动的退化可逆谐振子的响应解","authors":"Xin Yu Guan, Jian Guo Si, Wen Si","doi":"10.1007/s10114-023-1539-6","DOIUrl":null,"url":null,"abstract":"<div><p>In this paper, we consider a class of normally degenerate quasi-periodically forced reversible systems, obtained as perturbations of a set of harmonic oscillators, </p><div><div><span>$$\\left\\{ {\\matrix{{\\dot x = y + {f_1}(\\omega t,x,y),} \\hfill \\cr {\\dot y = \\lambda {x^l} + {f_2}(\\omega t,x,y),} \\hfill \\cr } } \\right.$$</span></div></div><p> where 0 ≠ λ ∈ ℝ, <i>l</i> > 1 is an integer and the corresponding involution <i>G</i> is (−<i>θ, x</i>, −<i>y</i>) → (<i>θ, x, y</i>). The existence of response solutions of the above reversible systems has already been proved in [22] if [<i>f</i><sub>2</sub>(<i>ωt</i>, 0, 0)] satisfies some non-zero average conditions (See the condition (<b>H</b>) in [22]), here [ · ] denotes the average of a continuous function on <span>\\({\\mathbb{T}^d}\\)</span>. However, discussing the existence of response solutions for the above systems encounters difficulties when [<i>f</i><sub>2</sub>(<i>ωt</i>, 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 [<i>f</i><sub>2</sub>(<i>ωt</i>, 0, 0)] = 0. More precisely, with 2<i>p</i> < <i>l</i>, if <i>f</i><sub>2</sub> satisfies <span>\\([{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\\)</span>, either <span>\\({\\lambda ^{ - 1}}[{{{\\partial ^p}{f_2}(\\omega t,0,0)} \\over {\\partial {x^p}}}] < 0\\)</span> as <i>l</i> − <i>p</i> is even or <span>\\({\\lambda ^{ - 1}}[{{{\\partial ^p}{f_2}(\\omega t,0,0)} \\over {\\partial {x^p}}}] \\ne 0\\)</span> as <i>l</i> − <i>p</i> is odd, we obtain the following results: (1) For <span>\\(\\tilde \\lambda < 0\\)</span> (see <span>\\({\\tilde \\lambda }\\)</span> in (2.2)) and <i>ϵ</i> sufficiently small, response solutions exist for each <i>ω</i> satisfying a weak non-resonant condition; (2) For <span>\\(\\tilde \\lambda < 0\\)</span> and <i>ϵ</i><sub>*</sub> sufficiently small, there exists a Cantor set <span>\\({\\cal E} \\in (0,{_ * })\\)</span> with almost full Lebesgue measure such that response solutions exist for each <span>\\( \\in {\\cal E}\\)</span> if <i>ω</i> satisfies a Diophantine condition. In the remaining case where <span>\\({\\lambda ^{ - 1}}[{{{\\partial ^p}{f_2}(\\omega t,0,0)} \\over {\\partial {x^p}}}] > 0\\)</span> and <i>l</i> − <i>p</i> is even, we prove the system admits no response solutions in most regions.</p></div>","PeriodicalId":0,"journal":{"name":"","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2023-10-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Response Solutions for Degenerate Reversible Harmonic Oscillators with Zero-average Perturbation\",\"authors\":\"Xin Yu Guan, Jian Guo Si, Wen Si\",\"doi\":\"10.1007/s10114-023-1539-6\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>In this paper, we consider a class of normally degenerate quasi-periodically forced reversible systems, obtained as perturbations of a set of harmonic oscillators, </p><div><div><span>$$\\\\left\\\\{ {\\\\matrix{{\\\\dot x = y + {f_1}(\\\\omega t,x,y),} \\\\hfill \\\\cr {\\\\dot y = \\\\lambda {x^l} + {f_2}(\\\\omega t,x,y),} \\\\hfill \\\\cr } } \\\\right.$$</span></div></div><p> where 0 ≠ λ ∈ ℝ, <i>l</i> > 1 is an integer and the corresponding involution <i>G</i> is (−<i>θ, x</i>, −<i>y</i>) → (<i>θ, x, y</i>). The existence of response solutions of the above reversible systems has already been proved in [22] if [<i>f</i><sub>2</sub>(<i>ωt</i>, 0, 0)] satisfies some non-zero average conditions (See the condition (<b>H</b>) in [22]), here [ · ] denotes the average of a continuous function on <span>\\\\({\\\\mathbb{T}^d}\\\\)</span>. However, discussing the existence of response solutions for the above systems encounters difficulties when [<i>f</i><sub>2</sub>(<i>ωt</i>, 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 [<i>f</i><sub>2</sub>(<i>ωt</i>, 0, 0)] = 0. More precisely, with 2<i>p</i> < <i>l</i>, if <i>f</i><sub>2</sub> satisfies <span>\\\\([{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\\\\)</span>, either <span>\\\\({\\\\lambda ^{ - 1}}[{{{\\\\partial ^p}{f_2}(\\\\omega t,0,0)} \\\\over {\\\\partial {x^p}}}] < 0\\\\)</span> as <i>l</i> − <i>p</i> is even or <span>\\\\({\\\\lambda ^{ - 1}}[{{{\\\\partial ^p}{f_2}(\\\\omega t,0,0)} \\\\over {\\\\partial {x^p}}}] \\\\ne 0\\\\)</span> as <i>l</i> − <i>p</i> is odd, we obtain the following results: (1) For <span>\\\\(\\\\tilde \\\\lambda < 0\\\\)</span> (see <span>\\\\({\\\\tilde \\\\lambda }\\\\)</span> in (2.2)) and <i>ϵ</i> sufficiently small, response solutions exist for each <i>ω</i> satisfying a weak non-resonant condition; (2) For <span>\\\\(\\\\tilde \\\\lambda < 0\\\\)</span> and <i>ϵ</i><sub>*</sub> sufficiently small, there exists a Cantor set <span>\\\\({\\\\cal E} \\\\in (0,{_ * })\\\\)</span> with almost full Lebesgue measure such that response solutions exist for each <span>\\\\( \\\\in {\\\\cal E}\\\\)</span> if <i>ω</i> satisfies a Diophantine condition. In the remaining case where <span>\\\\({\\\\lambda ^{ - 1}}[{{{\\\\partial ^p}{f_2}(\\\\omega t,0,0)} \\\\over {\\\\partial {x^p}}}] > 0\\\\)</span> and <i>l</i> − <i>p</i> is even, we prove the system admits no response solutions in most regions.</p></div>\",\"PeriodicalId\":0,\"journal\":{\"name\":\"\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0,\"publicationDate\":\"2023-10-15\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"\",\"FirstCategoryId\":\"100\",\"ListUrlMain\":\"https://link.springer.com/article/10.1007/s10114-023-1539-6\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"","FirstCategoryId":"100","ListUrlMain":"https://link.springer.com/article/10.1007/s10114-023-1539-6","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
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 l − p is even or \({\lambda ^{ - 1}}[{{{\partial ^p}{f_2}(\omega t,0,0)} \over {\partial {x^p}}}] \ne 0\) as l − p 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 l − p is even, we prove the system admits no response solutions in most regions.