Pub Date : 2024-08-28DOI: 10.1016/j.jde.2024.08.047
We study asymptotic behaviour of positive ground state solutions of the nonlinear Choquard equation(Pε)where is an integer, , , is the Riesz potential of order and is a parameter. We show that as (resp. ), the ground state solutions of , after appropriate rescalings dependent on parameter regimes, converge in to particular solutions of five different limit equations. We also establish a sharp asymptotic characterisation of such rescalings, and the precise asymptotic behaviour of , , ,
{"title":"Asymptotic profiles for Choquard equations with combined attractive nonlinearities","authors":"","doi":"10.1016/j.jde.2024.08.047","DOIUrl":"10.1016/j.jde.2024.08.047","url":null,"abstract":"<div><p>We study asymptotic behaviour of positive ground state solutions of the nonlinear Choquard equation<span><span><span>(<em>P</em><sub><em>ε</em></sub>)</span><span><math><mo>−</mo><mi>Δ</mi><mi>u</mi><mo>+</mo><mi>ε</mi><mi>u</mi><mo>=</mo><mo>(</mo><msub><mrow><mi>I</mi></mrow><mrow><mi>α</mi></mrow></msub><mo>⁎</mo><mo>|</mo><mi>u</mi><msup><mrow><mo>|</mo></mrow><mrow><mi>p</mi></mrow></msup><mo>)</mo><mo>|</mo><mi>u</mi><msup><mrow><mo>|</mo></mrow><mrow><mi>p</mi><mo>−</mo><mn>2</mn></mrow></msup><mi>u</mi><mo>+</mo><mo>|</mo><mi>u</mi><msup><mrow><mo>|</mo></mrow><mrow><mi>q</mi><mo>−</mo><mn>2</mn></mrow></msup><mi>u</mi><mo>,</mo><mspace></mspace><mtext>in</mtext><mspace></mspace><msup><mrow><mi>R</mi></mrow><mrow><mi>N</mi></mrow></msup><mo>,</mo></math></span></span></span>where <span><math><mi>N</mi><mo>≥</mo><mn>3</mn></math></span> is an integer, <span><math><mi>p</mi><mo>∈</mo><mo>[</mo><mfrac><mrow><mi>N</mi><mo>+</mo><mi>α</mi></mrow><mrow><mi>N</mi></mrow></mfrac><mo>,</mo><mfrac><mrow><mi>N</mi><mo>+</mo><mi>α</mi></mrow><mrow><mi>N</mi><mo>−</mo><mn>2</mn></mrow></mfrac><mo>]</mo></math></span>, <span><math><mi>q</mi><mo>∈</mo><mo>(</mo><mn>2</mn><mo>,</mo><mfrac><mrow><mn>2</mn><mi>N</mi></mrow><mrow><mi>N</mi><mo>−</mo><mn>2</mn></mrow></mfrac><mo>)</mo></math></span>, <span><math><msub><mrow><mi>I</mi></mrow><mrow><mi>α</mi></mrow></msub></math></span> is the Riesz potential of order <span><math><mi>α</mi><mo>∈</mo><mo>(</mo><mn>0</mn><mo>,</mo><mi>N</mi><mo>)</mo></math></span> and <span><math><mi>ε</mi><mo>></mo><mn>0</mn></math></span> is a parameter. We show that as <span><math><mi>ε</mi><mo>→</mo><mn>0</mn></math></span> (resp. <span><math><mi>ε</mi><mo>→</mo><mo>∞</mo></math></span>), the ground state solutions of <span><math><mo>(</mo><msub><mrow><mi>P</mi></mrow><mrow><mi>ε</mi></mrow></msub><mo>)</mo></math></span>, after appropriate rescalings dependent on parameter regimes, converge in <span><math><msup><mrow><mi>H</mi></mrow><mrow><mn>1</mn></mrow></msup><mo>(</mo><msup><mrow><mi>R</mi></mrow><mrow><mi>N</mi></mrow></msup><mo>)</mo></math></span> to particular solutions of five different limit equations. We also establish a sharp asymptotic characterisation of such rescalings, and the precise asymptotic behaviour of <span><math><msub><mrow><mi>u</mi></mrow><mrow><mi>ε</mi></mrow></msub><mo>(</mo><mn>0</mn><mo>)</mo></math></span>, <span><math><msubsup><mrow><mo>‖</mo><mi>∇</mi><msub><mrow><mi>u</mi></mrow><mrow><mi>ε</mi></mrow></msub><mo>‖</mo></mrow><mrow><mn>2</mn></mrow><mrow><mn>2</mn></mrow></msubsup></math></span>, <span><math><msubsup><mrow><mo>‖</mo><msub><mrow><mi>u</mi></mrow><mrow><mi>ε</mi></mrow></msub><mo>‖</mo></mrow><mrow><mn>2</mn></mrow><mrow><mn>2</mn></mrow></msubsup></math></span>, <span><math><msub><mrow><mo>∫</mo></mrow><mrow><msup><mrow><mi>R</mi></mrow><mrow><mi>N</mi></mrow></msup></mrow></msub><mo>(</mo><msub><mrow><mi>I</mi></mrow><mrow><mi>α</mi></mrow></msub><mo>⁎</mo><mo>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-08-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0022039624005291/pdfft?md5=91be345861f0636705f5c30a10983fa0&pid=1-s2.0-S0022039624005291-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142087554","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-28DOI: 10.1016/j.jde.2024.08.038
The aim of this paper is to obtain the sharp estimate for the lowest positive eigenvalue for the general Sturm–Liouville problem with the Neumann-Dirichlet boundary conditions, where q is a nonnegative potential and another potential m admits to change sign. First, we will study the optimal lower bound for the smallest positive eigenvalue in the measure differential equations to make our results more applicable. Second, based on the relationship between the minimization problem of the smallest positive eigenvalue for the ODE and the one for the MDE, we find the explicit optimal lower bound of the smallest positive eigenvalue for the general Sturm–Liouville equation.
{"title":"Minimization of the lowest positive Neumann-Dirichlet eigenvalue for general indefinite Sturm-Liouville problems","authors":"","doi":"10.1016/j.jde.2024.08.038","DOIUrl":"10.1016/j.jde.2024.08.038","url":null,"abstract":"<div><p>The aim of this paper is to obtain the sharp estimate for the lowest positive eigenvalue <span><math><msubsup><mrow><mi>λ</mi></mrow><mrow><mn>0</mn></mrow><mrow><mi>N</mi><mi>D</mi><mo>+</mo></mrow></msubsup></math></span> for the general Sturm–Liouville problem<span><span><span><math><msup><mrow><mi>y</mi></mrow><mrow><mo>″</mo></mrow></msup><mo>=</mo><mi>q</mi><mo>(</mo><mi>t</mi><mo>)</mo><mi>y</mi><mo>+</mo><mi>λ</mi><mi>m</mi><mo>(</mo><mi>t</mi><mo>)</mo><mi>y</mi><mo>,</mo></math></span></span></span> with the Neumann-Dirichlet boundary conditions, where <em>q</em> is a nonnegative potential and another potential <em>m</em> admits to change sign. First, we will study the optimal lower bound for the smallest positive eigenvalue in the measure differential equations to make our results more applicable. Second, based on the relationship between the minimization problem of the smallest positive eigenvalue for the ODE and the one for the MDE, we find the explicit optimal lower bound of the smallest positive eigenvalue for the general Sturm–Liouville equation.</p></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-08-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142087911","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-27DOI: 10.1016/j.jde.2024.08.049
Given a separable and real Hilbert space , we consider the following stochastic differential equation (SDE) on : where is a cylindrical pure jump Lévy process on which may be degenerate in the sense that the support of Z is contained in a finite dimensional space. When the nonlinear drift term is contractive with respect to some proper modified norm of for large distances, we obtain explicit exponential contraction rates of the SDE above in terms of Wasserstein distance under mild assumptions on the Lévy process Z. The approach is based on the refined basic coupling of Lévy noises, and it also works well when the so-called Lyapunov condition is satisfied.
给定一个可分离的实希尔伯特空间 H,我们考虑 H 上的以下随机微分方程(SDE):dXt=-Xtdt+b(Xt)dt+dZt,其中 Z:=(Zt)t≥0 是 H 上的圆柱纯跃迁莱维过程,从 Z 的支持包含在有限维空间中的意义上讲,它可能是退化的。当非线性漂移项 b(x) 相对于 H 的某些适当修正规范在大距离上具有收缩性时,在对勒维过程 Z 作温和假设的条件下,我们可以用瓦瑟斯坦距离得到上述 SDE 的指数收缩率。
{"title":"Exponential contraction rates for a class of degenerate SDEs with Lévy noises","authors":"","doi":"10.1016/j.jde.2024.08.049","DOIUrl":"10.1016/j.jde.2024.08.049","url":null,"abstract":"<div><p>Given a separable and real Hilbert space <span><math><mi>H</mi></math></span>, we consider the following stochastic differential equation (SDE) on <span><math><mi>H</mi></math></span>:<span><span><span><math><mi>d</mi><msub><mrow><mi>X</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><mo>−</mo><msub><mrow><mi>X</mi></mrow><mrow><mi>t</mi></mrow></msub><mspace></mspace><mi>d</mi><mi>t</mi><mo>+</mo><mi>b</mi><mo>(</mo><msub><mrow><mi>X</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>)</mo><mspace></mspace><mi>d</mi><mi>t</mi><mo>+</mo><mi>d</mi><msub><mrow><mi>Z</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>,</mo></math></span></span></span> where <span><math><mi>Z</mi><mo>:</mo><mo>=</mo><msub><mrow><mo>(</mo><msub><mrow><mi>Z</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>)</mo></mrow><mrow><mi>t</mi><mo>≥</mo><mn>0</mn></mrow></msub></math></span> is a cylindrical pure jump Lévy process on <span><math><mi>H</mi></math></span> which may be degenerate in the sense that the support of <em>Z</em> is contained in a finite dimensional space. When the nonlinear drift term <span><math><mi>b</mi><mo>(</mo><mi>x</mi><mo>)</mo></math></span> is contractive with respect to some proper modified norm of <span><math><mi>H</mi></math></span> for large distances, we obtain explicit exponential contraction rates of the SDE above in terms of Wasserstein distance under mild assumptions on the Lévy process <em>Z</em>. The approach is based on the refined basic coupling of Lévy noises, and it also works well when the so-called Lyapunov condition is satisfied.</p></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-08-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142083310","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-26DOI: 10.1016/j.jde.2024.08.036
We show that the Cauchy problem for the Camassa–Holm equation has a unique, global, weak, and dissipative solution for any initial data , such that is bounded from above almost everywhere. In particular, we establish a one-to-one correspondence between the properties specific to the dissipative solutions and a solution operator associating to each initial data exactly one solution.
{"title":"Uniqueness of dissipative solutions for the Camassa–Holm equation","authors":"","doi":"10.1016/j.jde.2024.08.036","DOIUrl":"10.1016/j.jde.2024.08.036","url":null,"abstract":"<div><p>We show that the Cauchy problem for the Camassa–Holm equation has a unique, global, weak, and dissipative solution for any initial data <span><math><msub><mrow><mi>u</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>∈</mo><msup><mrow><mi>H</mi></mrow><mrow><mn>1</mn></mrow></msup><mo>(</mo><mi>R</mi><mo>)</mo></math></span>, such that <span><math><msub><mrow><mi>u</mi></mrow><mrow><mn>0</mn><mo>,</mo><mi>x</mi></mrow></msub></math></span> is bounded from above almost everywhere. In particular, we establish a one-to-one correspondence between the properties specific to the dissipative solutions and a solution operator associating to each initial data exactly one solution.</p></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-08-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0022039624005187/pdfft?md5=a349f44866e2ca0ff6ed88a2d0a4e246&pid=1-s2.0-S0022039624005187-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142076886","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-26DOI: 10.1016/j.jde.2024.08.046
The main aim in this paper is to carry out a comprehensive research on the critical Hénon problem where , , , , , Ω is a smooth bounded domain containing the origin in , . Based on Lyapunov-Schmidt reduction argument, we provide some sufficient conditions for the existence of concentrating solutions without any condition on the Robin function. The main results depend on the non-resonant case that and the resonant case that . The novelty in our study is significantly different from the case that .
{"title":"Concentration phenomena of solutions for critical perturbed Hénon problems","authors":"","doi":"10.1016/j.jde.2024.08.046","DOIUrl":"10.1016/j.jde.2024.08.046","url":null,"abstract":"<div><p>The main aim in this paper is to carry out a comprehensive research on the critical Hénon problem<span><span><span><math><mrow><mo>{</mo><mtable><mtr><mtd><mo>−</mo><mi>Δ</mi><mi>u</mi><mo>=</mo><mo>|</mo><mi>x</mi><msup><mrow><mo>|</mo></mrow><mrow><mi>α</mi></mrow></msup><msup><mrow><mi>u</mi></mrow><mrow><msub><mrow><mi>p</mi></mrow><mrow><mi>α</mi></mrow></msub></mrow></msup><mo>+</mo><mi>ϵ</mi><mi>k</mi><mo>(</mo><mi>x</mi><mo>)</mo><msup><mrow><mi>u</mi></mrow><mrow><mi>q</mi></mrow></msup><mspace></mspace></mtd><mtd><mtext>in</mtext><mspace></mspace><mi>Ω</mi><mo>,</mo></mtd></mtr><mtr><mtd><mspace></mspace><mspace></mspace><mi>u</mi><mo>></mo><mn>0</mn><mspace></mspace></mtd><mtd><mtext>in</mtext><mspace></mspace><mi>Ω</mi><mo>,</mo></mtd></mtr><mtr><mtd><mspace></mspace><mi>u</mi><mo>=</mo><mn>0</mn><mspace></mspace></mtd><mtd><mtext>on</mtext><mspace></mspace><mspace></mspace><mo>∂</mo><mi>Ω</mi><mo>,</mo></mtd></mtr></mtable></mrow></math></span></span></span> where <span><math><mi>α</mi><mo>></mo><mn>0</mn></math></span>, <span><math><msub><mrow><mi>p</mi></mrow><mrow><mi>α</mi></mrow></msub><mo>=</mo><mfrac><mrow><mi>N</mi><mo>+</mo><mn>2</mn><mo>+</mo><mn>2</mn><mi>α</mi></mrow><mrow><mi>N</mi><mo>−</mo><mn>2</mn></mrow></mfrac></math></span>, <span><math><mi>q</mi><mo>≥</mo><mn>1</mn></math></span>, <span><math><mi>ϵ</mi><mo>></mo><mn>0</mn></math></span>, <span><math><mi>k</mi><mo>(</mo><mi>x</mi><mo>)</mo><mo>∈</mo><msup><mrow><mi>C</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>(</mo><mover><mrow><mi>Ω</mi></mrow><mrow><mo>¯</mo></mrow></mover><mo>)</mo></math></span>, Ω is a smooth bounded domain containing the origin in <span><math><msup><mrow><mi>R</mi></mrow><mrow><mi>N</mi></mrow></msup></math></span>, <span><math><mi>N</mi><mo>≥</mo><mn>3</mn></math></span>. Based on Lyapunov-Schmidt reduction argument, we provide some sufficient conditions for the existence of concentrating solutions without any condition on the Robin function. The main results depend on the non-resonant case that <span><math><mi>k</mi><mo>(</mo><mn>0</mn><mo>)</mo><mo>≠</mo><mn>0</mn><mspace></mspace><mtext>and</mtext><mspace></mspace><mi>q</mi><mo>≠</mo><mfrac><mrow><mi>N</mi><mo>+</mo><mn>2</mn></mrow><mrow><mi>N</mi><mo>−</mo><mn>2</mn></mrow></mfrac></math></span> and the resonant case that <span><math><mi>k</mi><mo>(</mo><mn>0</mn><mo>)</mo><mo>=</mo><mn>0</mn><mspace></mspace><mtext>or</mtext><mspace></mspace><mi>q</mi><mo>=</mo><mfrac><mrow><mi>N</mi><mo>+</mo><mn>2</mn></mrow><mrow><mi>N</mi><mo>−</mo><mn>2</mn></mrow></mfrac></math></span>. The novelty in our study is significantly different from the case that <span><math><mi>α</mi><mo>=</mo><mn>0</mn></math></span>.</p></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-08-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142077009","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-26DOI: 10.1016/j.jde.2024.08.052
In this paper, we study the number of zeros of Abelian integrals associated to some perturbed pendulum equations, and derive the new lower and upper bounds for the number of zeros of these integrals. The results we obtained correct some results of Theorem B and Proposition 1.1 in the paper (Gasull et al., 2016 [4]).
本文研究了与一些扰动摆方程相关的阿贝尔积分的零点个数,并推导出了这些积分零点个数的新下界和新上界。我们得到的结果修正了论文(Gasull 等,2016 [4])中定理 B 和命题 1.1 的一些结果。
{"title":"Revisiting the number of zeros of Abelian integrals for perturbed pendulum equations","authors":"","doi":"10.1016/j.jde.2024.08.052","DOIUrl":"10.1016/j.jde.2024.08.052","url":null,"abstract":"<div><p>In this paper, we study the number of zeros of Abelian integrals associated to some perturbed pendulum equations, and derive the new lower and upper bounds for the number of zeros of these integrals. The results we obtained correct some results of Theorem B and Proposition 1.1 in the paper (Gasull et al., 2016 <span><span>[4]</span></span>).</p></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-08-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142077010","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-26DOI: 10.1016/j.jde.2024.08.041
In this paper we study the stability of a special magnetic Bénard system near equilibrium, where there exists Laplacian magnetic diffusion and temperature damping but the velocity equation involves no dissipation. Without any velocity dissipation, the fluid velocity is governed by the two-dimensional incompressible Euler equation, whose solution can grow rapidly in time. However, when the fluid is coupled with the magnetic field and temperature through the magnetic Bénard system, we show that the solution is stable. Our results mathematically illustrate that the magnetic field and temperature have the effect of enhancing dissipation and contribute to stabilize the fluid.
{"title":"The stabilizing effect of temperature and magnetic field on a 2D magnetic Bénard fluids","authors":"","doi":"10.1016/j.jde.2024.08.041","DOIUrl":"10.1016/j.jde.2024.08.041","url":null,"abstract":"<div><p>In this paper we study the stability of a special magnetic Bénard system near equilibrium, where there exists Laplacian magnetic diffusion and temperature damping but the velocity equation involves no dissipation. Without any velocity dissipation, the fluid velocity is governed by the two-dimensional incompressible Euler equation, whose solution can grow rapidly in time. However, when the fluid is coupled with the magnetic field and temperature through the magnetic Bénard system, we show that the solution is stable. Our results mathematically illustrate that the magnetic field and temperature have the effect of enhancing dissipation and contribute to stabilize the fluid.</p></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-08-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142076298","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-26DOI: 10.1016/j.jde.2024.08.028
In [1] the Theorems 1, 2 and 3, as well as Proposition 1, are incorrect as they are stated. To make them correct it suffices to add the extra condition to the expressions (1.1) and (1.4).
{"title":"Corrigendum to “A flow box theorem for 2d slow-fast vector fields and diffeomorphisms and the slow log-determinant integral” [J. Differ. Equ. 333 (2022) 361–406]","authors":"","doi":"10.1016/j.jde.2024.08.028","DOIUrl":"10.1016/j.jde.2024.08.028","url":null,"abstract":"<div><p>In <span><span>[1]</span></span> the Theorems 1, 2 and 3, as well as Proposition 1, are incorrect as they are stated. To make them correct it suffices to add the extra condition<span><span><span><math><mi>D</mi><mo>(</mo><mi>x</mi><mo>,</mo><mn>0</mn><mo>,</mo><mi>λ</mi><mo>)</mo><mo>=</mo><mn>0</mn></math></span></span></span> to the expressions (1.1) and (1.4).</p><p>The same holds for Definition 2.</p></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-08-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0022039624005102/pdfft?md5=b84ce3461b5329a57c4602e132f983de&pid=1-s2.0-S0022039624005102-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142122864","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-26DOI: 10.1016/j.jde.2024.08.044
We study the global boundedness of the solutions of a non-smooth forced oscillator with a periodic and real analytic forcing. We show that the impact map associated with this discontinuous equation becomes a real analytic and exact symplectic map when written in suitable canonical coordinates. By an accurate study of the behaviour of the map for large amplitudes and by employing a parametrization KAM theorem, we show that the periodic solutions of the unperturbed oscillator persist as two-dimensional tori under conditions that depend on the Diophantine conditions of the frequency, but are independent on both the amplitude of the orbit and of the specific value of the frequency. This allows the construction of a sequence of nested invariant tori of increasing amplitude that confine the solutions within them, ensuring their boundedness. The same construction may be useful to address such persistence problem for a larger class of non-smooth forced oscillators.
我们研究了具有周期性实解析强迫的非光滑强迫振荡器解的全局有界性。我们的研究表明,与这个不连续方程相关的冲击图在用合适的对偶坐标书写时,会变成一个实解析的精确对偶图。通过对大振幅时该映射行为的精确研究,并利用参数化 KAM 定理,我们证明了在取决于频率的 Diophantine 条件,但与轨道振幅和频率的具体值无关的条件下,未受扰动振荡器的周期解作为二维环持续存在。这样就可以构建一连串振幅递增的嵌套不变环,将解限制在其中,确保解的有界性。同样的构造可能有助于解决更大一类非光滑受迫振荡器的持久性问题。
{"title":"On the boundedness of solutions of a forced discontinuous oscillator","authors":"","doi":"10.1016/j.jde.2024.08.044","DOIUrl":"10.1016/j.jde.2024.08.044","url":null,"abstract":"<div><p>We study the global boundedness of the solutions of a non-smooth forced oscillator with a periodic and real analytic forcing. We show that the impact map associated with this discontinuous equation becomes a real analytic and exact symplectic map when written in suitable canonical coordinates. By an accurate study of the behaviour of the map for large amplitudes and by employing a parametrization KAM theorem, we show that the periodic solutions of the unperturbed oscillator persist as two-dimensional tori under conditions that depend on the Diophantine conditions of the frequency, but are independent on both the amplitude of the orbit and of the specific value of the frequency. This allows the construction of a sequence of nested invariant tori of increasing amplitude that confine the solutions within them, ensuring their boundedness. The same construction may be useful to address such persistence problem for a larger class of non-smooth forced oscillators.</p></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-08-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142076887","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-26DOI: 10.1016/j.jde.2024.08.043
This paper is devoted to studying the initial-boundary value problem for the radiative full Euler equations, which are a fundamental system in the radiative hydrodynamics with many practical applications in astrophysical and nuclear phenomena, with the non-slip boundary condition on an impermeable wall. Due to the difficulty from the disappearance of the velocity on the impermeable boundary, quite few results for compressible Navier-Stokes equations and no result for the radiative Euler equations are available at this moment. So the asymptotic stability of the rarefaction wave proven in this paper is the first rigorous result on the global stability of solutions of the radiative Euler equations with the non-slip boundary condition. It also contributes to our systematical study on the asymptotic behaviors of the rarefaction wave with the radiative effect and different boundary conditions such as the inflow/outflow problem and the impermeable boundary problem in our series papers including [5], [6].
{"title":"Asymptotic stability of rarefaction wave with non-slip boundary condition for radiative Euler flows","authors":"","doi":"10.1016/j.jde.2024.08.043","DOIUrl":"10.1016/j.jde.2024.08.043","url":null,"abstract":"<div><p>This paper is devoted to studying the initial-boundary value problem for the radiative full Euler equations, which are a fundamental system in the radiative hydrodynamics with many practical applications in astrophysical and nuclear phenomena, with the non-slip boundary condition on an impermeable wall. Due to the difficulty from the disappearance of the velocity on the impermeable boundary, quite few results for compressible Navier-Stokes equations and no result for the radiative Euler equations are available at this moment. So the asymptotic stability of the rarefaction wave proven in this paper is the first rigorous result on the global stability of solutions of the radiative Euler equations with the non-slip boundary condition. It also contributes to our systematical study on the asymptotic behaviors of the rarefaction wave with the radiative effect and different boundary conditions such as the inflow/outflow problem and the impermeable boundary problem in our series papers including <span><span>[5]</span></span>, <span><span>[6]</span></span>.</p></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-08-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142076297","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}