Pub Date : 2024-09-24DOI: 10.1016/j.jde.2024.09.034
We study step-wise time approximations of non-linear hyperbolic initial value problems. The technique used here is a generalization of the minimizing movements method, using two time-scales: one for velocity, the other (potentially much larger) for acceleration. The main applications are from elastodynamics, namely so-called generalized solids, undergoing large deformations. The evolution follows an underlying variational structure exploited by step-wise minimization. We show for a large family of (elastic) energies that the introduced scheme is stable; allowing for non-linearities of highest order. If the highest order can be assumed to be linear, we show that the limit solutions are regular and that the minimizing movements scheme converges with optimal linear rate. Thus this work extends numerical time-step minimization methods to the realm of hyperbolic problems.
{"title":"Stability and convergence of in time approximations of hyperbolic elastodynamics via stepwise minimization","authors":"","doi":"10.1016/j.jde.2024.09.034","DOIUrl":"10.1016/j.jde.2024.09.034","url":null,"abstract":"<div><div>We study step-wise time approximations of non-linear hyperbolic initial value problems. The technique used here is a generalization of the minimizing movements method, using two time-scales: one for velocity, the other (potentially much larger) for acceleration. The main applications are from elastodynamics, namely so-called generalized solids, undergoing large deformations. The evolution follows an underlying variational structure exploited by step-wise minimization. We show for a large family of (elastic) energies that the introduced scheme is stable; allowing for non-linearities of highest order. If the highest order can be assumed to be linear, we show that the limit solutions are regular and that the minimizing movements scheme converges with optimal linear rate. Thus this work extends numerical time-step minimization methods to the realm of hyperbolic problems.</div></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-09-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142315769","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 : 2024-09-23DOI: 10.1016/j.jde.2024.09.035
This study examines nonnegative solutions to the problem where , , and are constants. The possible asymptotic behaviors of at and are classified according to . In particular, the results show that for some , exhibits only “isotropic” behavior at and . However, in other cases, may exhibit the “anisotropic” behavior at or . Furthermore, the relation between the limit at and the limit at for a global solution is investigated.
{"title":"Study on the behaviors of rupture solutions for a class of elliptic MEMS equations in R2","authors":"","doi":"10.1016/j.jde.2024.09.035","DOIUrl":"10.1016/j.jde.2024.09.035","url":null,"abstract":"<div><div>This study examines nonnegative solutions to the problem<span><span><span><math><mrow><mo>{</mo><mtable><mtr><mtd><mi>Δ</mi><mi>u</mi><mo>=</mo><mfrac><mrow><mi>λ</mi><mo>|</mo><mi>x</mi><msup><mrow><mo>|</mo></mrow><mrow><mi>α</mi></mrow></msup></mrow><mrow><msup><mrow><mi>u</mi></mrow><mrow><mi>p</mi></mrow></msup></mrow></mfrac><mspace></mspace></mtd><mtd><mtext> in</mtext><mspace></mspace><mspace></mspace><msup><mrow><mi>R</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>∖</mo><mo>{</mo><mn>0</mn><mo>}</mo><mo>,</mo></mtd></mtr><mtr><mtd><mi>u</mi><mo>(</mo><mn>0</mn><mo>)</mo><mo>=</mo><mn>0</mn><mspace></mspace><mtext>and</mtext><mspace></mspace><mi>u</mi><mo>></mo><mn>0</mn><mspace></mspace></mtd><mtd><mtext> in</mtext><mspace></mspace><mspace></mspace><msup><mrow><mi>R</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>∖</mo><mo>{</mo><mn>0</mn><mo>}</mo><mo>,</mo></mtd></mtr></mtable></mrow></math></span></span></span> where <span><math><mi>λ</mi><mo>></mo><mn>0</mn></math></span>, <span><math><mi>α</mi><mo>></mo><mo>−</mo><mn>2</mn></math></span>, and <span><math><mi>p</mi><mo>></mo><mn>0</mn></math></span> are constants. The possible asymptotic behaviors of <span><math><mi>u</mi><mo>(</mo><mi>x</mi><mo>)</mo></math></span> at <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>=</mo><mn>0</mn></math></span> and <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>=</mo><mo>∞</mo></math></span> are classified according to <span><math><mo>(</mo><mi>α</mi><mo>,</mo><mi>p</mi><mo>)</mo></math></span>. In particular, the results show that for some <span><math><mo>(</mo><mi>α</mi><mo>,</mo><mi>p</mi><mo>)</mo></math></span>, <span><math><mi>u</mi><mo>(</mo><mi>x</mi><mo>)</mo></math></span> exhibits only “isotropic” behavior at <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>=</mo><mn>0</mn></math></span> and <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>=</mo><mo>∞</mo></math></span>. However, in other cases, <span><math><mi>u</mi><mo>(</mo><mi>x</mi><mo>)</mo></math></span> may exhibit the “anisotropic” behavior at <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>=</mo><mn>0</mn></math></span> or <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>=</mo><mo>∞</mo></math></span>. Furthermore, the relation between the limit at <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>=</mo><mn>0</mn></math></span> and the limit at <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>=</mo><mo>∞</mo></math></span> for a global solution is investigated.</div></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-09-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142312203","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 : 2024-09-23DOI: 10.1016/j.jde.2024.09.027
<div><div>In this paper, we consider the two-species chemotaxis-competition system with loop and nonlocal kinetics<span><span><span><math><mrow><mo>{</mo><mtable><mtr><mtd><msub><mrow><mi>u</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><mi>Δ</mi><mi>u</mi><mo>−</mo><msub><mrow><mi>χ</mi></mrow><mrow><mn>11</mn></mrow></msub><mi>∇</mi><mo>⋅</mo><mo>(</mo><mi>u</mi><mi>∇</mi><mi>v</mi><mo>)</mo><mo>−</mo><msub><mrow><mi>χ</mi></mrow><mrow><mn>12</mn></mrow></msub><mi>∇</mi><mo>⋅</mo><mo>(</mo><mi>u</mi><mi>∇</mi><mi>z</mi><mo>)</mo><mo>+</mo><msub><mrow><mi>f</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>(</mo><mi>u</mi><mo>,</mo><mi>w</mi><mo>)</mo><mo>,</mo><mspace></mspace></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mspace></mspace><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr><mtr><mtd><mn>0</mn><mo>=</mo><mi>Δ</mi><mi>v</mi><mo>−</mo><mi>v</mi><mo>+</mo><mi>u</mi><mo>+</mo><mi>w</mi><mo>,</mo><mspace></mspace></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mspace></mspace><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr><mtr><mtd><msub><mrow><mi>w</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><mi>Δ</mi><mi>w</mi><mo>−</mo><msub><mrow><mi>χ</mi></mrow><mrow><mn>21</mn></mrow></msub><mi>∇</mi><mo>⋅</mo><mo>(</mo><mi>w</mi><mi>∇</mi><mi>v</mi><mo>)</mo><mo>−</mo><msub><mrow><mi>χ</mi></mrow><mrow><mn>22</mn></mrow></msub><mi>∇</mi><mo>⋅</mo><mo>(</mo><mi>w</mi><mi>∇</mi><mi>z</mi><mo>)</mo><mo>+</mo><msub><mrow><mi>f</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>(</mo><mi>u</mi><mo>,</mo><mi>w</mi><mo>)</mo><mo>,</mo><mspace></mspace></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mspace></mspace><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr><mtr><mtd><mn>0</mn><mo>=</mo><mi>Δ</mi><mi>z</mi><mo>−</mo><mi>z</mi><mo>+</mo><mi>u</mi><mo>+</mo><mi>w</mi><mo>,</mo><mspace></mspace></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mspace></mspace><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr></mtable></mrow></math></span></span></span> subject to homogeneous Neumann boundary conditions in a smooth bounded domain <span><math><mi>Ω</mi><mo>⊂</mo><msup><mrow><mi>R</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>(</mo><mi>n</mi><mo>≥</mo><mn>1</mn><mo>)</mo></math></span>, where <span><math><msub><mrow><mi>χ</mi></mrow><mrow><mi>i</mi><mi>j</mi></mrow></msub><mo>></mo><mn>0</mn><mo>(</mo><mi>i</mi><mo>,</mo><mi>j</mi><mo>=</mo><mn>1</mn><mo>,</mo><mn>2</mn><mo>)</mo></math></span>, <span><math><msub><mrow><mi>f</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>(</mo><mi>u</mi><mo>,</mo><mi>w</mi><mo>)</mo><mo>=</mo><mi>u</mi><mrow><mo>(</mo><msub><mrow><mi>a</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>−</mo><msub><mrow><mi>a</mi></mrow><mrow><mn>1</mn></mrow></msub><mi>u</mi><mo>−</mo><msub><mrow><mi>a</mi></mrow><mrow><mn>2</mn></mrow></msub><mi>w</mi><mo>−</mo><msub><mrow><mi>a</mi></mrow><mrow><mn>3</mn></mrow></msub><msub><mrow><mo>∫</mo></mrow><mrow><mi>Ω</mi></mrow></msub><mi>u</mi><mi>d</mi><mi>
{"title":"Global dynamics for a two-species chemotaxis-competition system with loop and nonlocal kinetics","authors":"","doi":"10.1016/j.jde.2024.09.027","DOIUrl":"10.1016/j.jde.2024.09.027","url":null,"abstract":"<div><div>In this paper, we consider the two-species chemotaxis-competition system with loop and nonlocal kinetics<span><span><span><math><mrow><mo>{</mo><mtable><mtr><mtd><msub><mrow><mi>u</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><mi>Δ</mi><mi>u</mi><mo>−</mo><msub><mrow><mi>χ</mi></mrow><mrow><mn>11</mn></mrow></msub><mi>∇</mi><mo>⋅</mo><mo>(</mo><mi>u</mi><mi>∇</mi><mi>v</mi><mo>)</mo><mo>−</mo><msub><mrow><mi>χ</mi></mrow><mrow><mn>12</mn></mrow></msub><mi>∇</mi><mo>⋅</mo><mo>(</mo><mi>u</mi><mi>∇</mi><mi>z</mi><mo>)</mo><mo>+</mo><msub><mrow><mi>f</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>(</mo><mi>u</mi><mo>,</mo><mi>w</mi><mo>)</mo><mo>,</mo><mspace></mspace></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mspace></mspace><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr><mtr><mtd><mn>0</mn><mo>=</mo><mi>Δ</mi><mi>v</mi><mo>−</mo><mi>v</mi><mo>+</mo><mi>u</mi><mo>+</mo><mi>w</mi><mo>,</mo><mspace></mspace></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mspace></mspace><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr><mtr><mtd><msub><mrow><mi>w</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><mi>Δ</mi><mi>w</mi><mo>−</mo><msub><mrow><mi>χ</mi></mrow><mrow><mn>21</mn></mrow></msub><mi>∇</mi><mo>⋅</mo><mo>(</mo><mi>w</mi><mi>∇</mi><mi>v</mi><mo>)</mo><mo>−</mo><msub><mrow><mi>χ</mi></mrow><mrow><mn>22</mn></mrow></msub><mi>∇</mi><mo>⋅</mo><mo>(</mo><mi>w</mi><mi>∇</mi><mi>z</mi><mo>)</mo><mo>+</mo><msub><mrow><mi>f</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>(</mo><mi>u</mi><mo>,</mo><mi>w</mi><mo>)</mo><mo>,</mo><mspace></mspace></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mspace></mspace><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr><mtr><mtd><mn>0</mn><mo>=</mo><mi>Δ</mi><mi>z</mi><mo>−</mo><mi>z</mi><mo>+</mo><mi>u</mi><mo>+</mo><mi>w</mi><mo>,</mo><mspace></mspace></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mspace></mspace><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr></mtable></mrow></math></span></span></span> subject to homogeneous Neumann boundary conditions in a smooth bounded domain <span><math><mi>Ω</mi><mo>⊂</mo><msup><mrow><mi>R</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>(</mo><mi>n</mi><mo>≥</mo><mn>1</mn><mo>)</mo></math></span>, where <span><math><msub><mrow><mi>χ</mi></mrow><mrow><mi>i</mi><mi>j</mi></mrow></msub><mo>></mo><mn>0</mn><mo>(</mo><mi>i</mi><mo>,</mo><mi>j</mi><mo>=</mo><mn>1</mn><mo>,</mo><mn>2</mn><mo>)</mo></math></span>, <span><math><msub><mrow><mi>f</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>(</mo><mi>u</mi><mo>,</mo><mi>w</mi><mo>)</mo><mo>=</mo><mi>u</mi><mrow><mo>(</mo><msub><mrow><mi>a</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>−</mo><msub><mrow><mi>a</mi></mrow><mrow><mn>1</mn></mrow></msub><mi>u</mi><mo>−</mo><msub><mrow><mi>a</mi></mrow><mrow><mn>2</mn></mrow></msub><mi>w</mi><mo>−</mo><msub><mrow><mi>a</mi></mrow><mrow><mn>3</mn></mrow></msub><msub><mrow><mo>∫</mo></mrow><mrow><mi>Ω</mi></mrow></msub><mi>u</mi><mi>d</mi><mi>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-09-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142310593","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 : 2024-09-23DOI: 10.1016/j.jde.2024.09.025
We analyze finite-time blowup scenarios of locally self-similar type for the inviscid generalized surface quasi-geostrophic equation (gSQG) in . Under an growth assumption on the self-similar profile and its gradient, we identify appropriate ranges of the self-similar parameter where the profile is either identically zero, and hence blowup cannot occur, or its asymptotic behavior can be characterized, for suitable . Our results extend the work by Xue [38] regarding the SQG equation, and also partially recover the results proved by Cannone and Xue [3] concerning globally self-similar solutions of the gSQG equation.
{"title":"On the locally self-similar blowup for the generalized SQG equation","authors":"","doi":"10.1016/j.jde.2024.09.025","DOIUrl":"10.1016/j.jde.2024.09.025","url":null,"abstract":"<div><div>We analyze finite-time blowup scenarios of locally self-similar type for the inviscid generalized surface quasi-geostrophic equation (gSQG) in <span><math><msup><mrow><mi>R</mi></mrow><mrow><mn>2</mn></mrow></msup></math></span>. Under an <span><math><msup><mrow><mi>L</mi></mrow><mrow><mi>r</mi></mrow></msup></math></span> growth assumption on the self-similar profile and its gradient, we identify appropriate ranges of the self-similar parameter where the profile is either identically zero, and hence blowup cannot occur, or its <span><math><msup><mrow><mi>L</mi></mrow><mrow><mi>p</mi></mrow></msup></math></span> asymptotic behavior can be characterized, for suitable <span><math><mi>r</mi><mo>,</mo><mi>p</mi></math></span>. Our results extend the work by Xue <span><span>[38]</span></span> regarding the SQG equation, and also partially recover the results proved by Cannone and Xue <span><span>[3]</span></span> concerning globally self-similar solutions of the gSQG equation.</div></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-09-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142310594","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 : 2024-09-23DOI: 10.1016/j.jde.2024.09.029
We prove the existence of a normalized, stationary solution with frequency of the nonlinear Dirac equation. The result covers the case in which the nonlinearity is the gradient of a function of the form with , and sufficiently small. Here , are the Dirac's matrices.
We find the solution as a critical point of a suitable functional restricted to the unit sphere in , and ω turns out to be the corresponding Lagrange multiplier.
{"title":"Normalized solutions for a nonlinear Dirac equation","authors":"","doi":"10.1016/j.jde.2024.09.029","DOIUrl":"10.1016/j.jde.2024.09.029","url":null,"abstract":"<div><div>We prove the existence of a normalized, stationary solution <span><math><mi>ψ</mi><mo>:</mo><msup><mrow><mi>R</mi></mrow><mrow><mn>3</mn></mrow></msup><mo>→</mo><msup><mrow><mi>C</mi></mrow><mrow><mn>4</mn></mrow></msup></math></span> with frequency <span><math><mi>ω</mi><mo>></mo><mn>0</mn></math></span> of the nonlinear Dirac equation. The result covers the case in which the nonlinearity is the gradient of a function of the form<span><span><span><math><mi>F</mi><mo>(</mo><mi>Ψ</mi><mo>)</mo><mo>=</mo><mi>a</mi><mo>|</mo><mo>(</mo><mi>Ψ</mi><mo>,</mo><msup><mrow><mi>γ</mi></mrow><mrow><mn>0</mn></mrow></msup><mi>Ψ</mi><mo>)</mo><msup><mrow><mo>|</mo></mrow><mrow><mfrac><mrow><mi>α</mi></mrow><mrow><mn>2</mn></mrow></mfrac></mrow></msup><mo>+</mo><mi>b</mi><mo>|</mo><mo>(</mo><mi>Ψ</mi><mo>,</mo><msup><mrow><mi>γ</mi></mrow><mrow><mn>1</mn></mrow></msup><msup><mrow><mi>γ</mi></mrow><mrow><mn>2</mn></mrow></msup><msup><mrow><mi>γ</mi></mrow><mrow><mn>3</mn></mrow></msup><mi>Ψ</mi><mo>)</mo><msup><mrow><mo>|</mo></mrow><mrow><mfrac><mrow><mi>α</mi></mrow><mrow><mn>2</mn></mrow></mfrac></mrow></msup></math></span></span></span> with <span><math><mi>α</mi><mo>∈</mo><mo>(</mo><mn>2</mn><mo>,</mo><mfrac><mrow><mn>8</mn></mrow><mrow><mn>3</mn></mrow></mfrac><mo>]</mo></math></span>, <span><math><mi>b</mi><mo>≥</mo><mn>0</mn></math></span> and <span><math><mi>a</mi><mo>></mo><mn>0</mn></math></span> sufficiently small. Here <span><math><msup><mrow><mi>γ</mi></mrow><mrow><mi>i</mi></mrow></msup></math></span>, <span><math><mi>i</mi><mo>=</mo><mn>0</mn><mo>,</mo><mo>…</mo><mo>,</mo><mn>3</mn></math></span> are the <span><math><mn>4</mn><mo>×</mo><mn>4</mn></math></span> Dirac's matrices.</div><div>We find the solution as a critical point of a suitable functional restricted to the unit sphere in <span><math><msup><mrow><mi>L</mi></mrow><mrow><mn>2</mn></mrow></msup></math></span>, and <em>ω</em> turns out to be the corresponding Lagrange multiplier.</div></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-09-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0022039624006144/pdfft?md5=cb690464016ef3752322a3f835e48f7c&pid=1-s2.0-S0022039624006144-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142312201","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 : 2024-09-23DOI: 10.1016/j.jde.2024.09.038
In this paper, we investigate the large-order asymptotics of multi-rational solitons of the focusing complex modified Korteweg-de Vries (c-mKdV) equation with nonzero background via the Riemann-Hilbert problems. First, based on the Lax pair, inverse scattering transform, and a series of deformations, we construct a multi-rational soliton of the c-mKdV equation via a solvable Riemann-Hilbert problem (RHP). Then, through a scale transformation, we construct a RHP corresponding to the limit function which is a new solution of the c-mKdV equation in the rescaled variables , and prove the existence and uniqueness of the RHP's solution. Moreover, we also find that the limit function satisfies the ordinary differential equations (ODEs) with respect to space X and time T, respectively. The ODEs with respect to space X are identified with certain members of the Painlevé-III hierarchy. We study the large X and transitional asymptotic behaviors of near-field limit solutions, and we provide some part results for the case of large T. These results will be useful to understand and apply the large-order rational solitons in the nonlinear wave equations.
本文通过黎曼-希尔伯特(Riemann-Hilbert)问题研究了具有非零背景的聚焦复修正科特韦格-德弗里斯(c-mKdV)方程的多理性孤子的大阶渐近性。首先,基于拉克斯对、反散射变换和一系列变形,我们通过可解黎曼-希尔伯特问题(Riemann-Hilbert problem,RHP)构建了 c-mKdV 方程的多理性孤子。然后,通过尺度变换,我们构建了一个与极限函数相对应的 RHP,该极限函数是 c-mKdV 方程在重标度变量 X,T 中的新解,并证明了 RHP 解的存在性和唯一性。此外,我们还发现极限函数分别满足空间 X 和时间 T 的常微分方程。关于空间 X 的 ODE 与 Painlevé-III 层次结构的某些成员相一致。我们研究了近场极限解的大 X 和过渡渐近行为,并提供了大 T 情况下的部分结果。这些结果将有助于理解和应用非线性波方程中的大阶有理孤子。
{"title":"The focusing complex mKdV equation with nonzero background: Large N-order asymptotics of multi-rational solitons and related Painlevé-III hierarchy","authors":"","doi":"10.1016/j.jde.2024.09.038","DOIUrl":"10.1016/j.jde.2024.09.038","url":null,"abstract":"<div><div>In this paper, we investigate the large-order asymptotics of multi-rational solitons of the focusing complex modified Korteweg-de Vries (c-mKdV) equation with nonzero background via the Riemann-Hilbert problems. First, based on the Lax pair, inverse scattering transform, and a series of deformations, we construct a multi-rational soliton of the c-mKdV equation via a solvable Riemann-Hilbert problem (RHP). Then, through a scale transformation, we construct a RHP corresponding to the limit function which is a new solution of the c-mKdV equation in the rescaled variables <span><math><mi>X</mi><mo>,</mo><mspace></mspace><mi>T</mi></math></span>, and prove the existence and uniqueness of the RHP's solution. Moreover, we also find that the limit function satisfies the ordinary differential equations (ODEs) with respect to space <em>X</em> and time <em>T</em>, respectively. The ODEs with respect to space <em>X</em> are identified with certain members of the Painlevé-III hierarchy. We study the large <em>X</em> and transitional asymptotic behaviors of near-field limit solutions, and we provide some part results for the case of large <em>T</em>. These results will be useful to understand and apply the large-order rational solitons in the nonlinear wave equations.</div></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-09-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142310595","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 : 2024-09-23DOI: 10.1016/j.jde.2024.09.002
We study the dynamics of waves, oscillations, and other spatio-temporal patterns in stochastic evolution systems, including SPDE and stochastic integral equations. Representing a given pattern as a smooth, stable invariant manifold of the deterministic dynamics, we reduce the stochastic dynamics to a finite dimensional SDE on this manifold using the isochronal phase. The isochronal phase is defined by mapping a neighborhood of the manifold onto the manifold itself, analogous to the isochronal phase defined for finite-dimensional oscillators by A.T. Winfree and J. Guckenheimer. We then determine a probability measure that indicates the average position of the stochastic perturbation of the pattern/wave as it wanders over the manifold. It is proved that this probability measure is accurate on time-scales greater than , but less than , where is the amplitude of the stochastic perturbation. Moreover, using this measure, we determine the expected velocity of the difference between the deterministic and stochastic motion on the manifold.
{"title":"The isochronal phase of stochastic PDE and integral equations: Metastability and other properties","authors":"","doi":"10.1016/j.jde.2024.09.002","DOIUrl":"10.1016/j.jde.2024.09.002","url":null,"abstract":"<div><div>We study the dynamics of waves, oscillations, and other spatio-temporal patterns in stochastic evolution systems, including SPDE and stochastic integral equations. Representing a given pattern as a smooth, stable invariant manifold of the deterministic dynamics, we reduce the stochastic dynamics to a finite dimensional SDE on this manifold using the isochronal phase. The isochronal phase is defined by mapping a neighborhood of the manifold onto the manifold itself, analogous to the isochronal phase defined for finite-dimensional oscillators by A.T. Winfree and J. Guckenheimer. We then determine a probability measure that indicates the average position of the stochastic perturbation of the pattern/wave as it wanders over the manifold. It is proved that this probability measure is accurate on time-scales greater than <span><math><mi>O</mi><mo>(</mo><msup><mrow><mi>σ</mi></mrow><mrow><mo>−</mo><mn>2</mn></mrow></msup><mo>)</mo></math></span>, but less than <span><math><mi>O</mi><mo>(</mo><mi>exp</mi><mo></mo><mo>(</mo><mi>C</mi><msup><mrow><mi>σ</mi></mrow><mrow><mo>−</mo><mn>2</mn></mrow></msup><mo>)</mo><mo>)</mo></math></span>, where <span><math><mi>σ</mi><mo>≪</mo><mn>1</mn></math></span> is the amplitude of the stochastic perturbation. Moreover, using this measure, we determine the expected velocity of the difference between the deterministic and stochastic motion on the manifold.</div></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-09-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142312202","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 : 2024-09-20DOI: 10.1016/j.jde.2024.09.026
This paper is concerned with the weak solution for the fast diffusion equation with absorption and singularity in the form of . We first prove the existence and decay estimate of weak solution when the fast diffusion index satisfies and the absorption index is . Then we show the asymptotic convergence of weak solution to the corresponding Barenblatt solution for and via the entropy dissipation method combining the generalized Shannon's inequality and Csiszár-Kullback inequality. The singularity of spatial diffusion causes us the technical challenges for the asymptotic behavior of weak solution.
{"title":"Asymptotic behavior for the fast diffusion equation with absorption and singularity","authors":"","doi":"10.1016/j.jde.2024.09.026","DOIUrl":"10.1016/j.jde.2024.09.026","url":null,"abstract":"<div><p>This paper is concerned with the weak solution for the fast diffusion equation with absorption and singularity in the form of <span><math><msub><mrow><mi>u</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><mo>△</mo><msup><mrow><mi>u</mi></mrow><mrow><mi>m</mi></mrow></msup><mo>−</mo><msup><mrow><mi>u</mi></mrow><mrow><mi>p</mi></mrow></msup></math></span>. We first prove the existence and decay estimate of weak solution when the fast diffusion index satisfies <span><math><mn>0</mn><mo><</mo><mi>m</mi><mo><</mo><mn>1</mn></math></span> and the absorption index is <span><math><mi>p</mi><mo>></mo><mn>1</mn></math></span>. Then we show the asymptotic convergence of weak solution to the corresponding Barenblatt solution for <span><math><mfrac><mrow><mi>n</mi><mo>−</mo><mn>1</mn></mrow><mrow><mi>n</mi></mrow></mfrac><mo><</mo><mi>m</mi><mo><</mo><mn>1</mn></math></span> and <span><math><mi>p</mi><mo>></mo><mi>m</mi><mo>+</mo><mfrac><mrow><mn>2</mn></mrow><mrow><mi>n</mi></mrow></mfrac></math></span> via the entropy dissipation method combining the generalized Shannon's inequality and Csiszár-Kullback inequality. The singularity of spatial diffusion causes us the technical challenges for the asymptotic behavior of weak solution.</p></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-09-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142272360","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 : 2024-09-20DOI: 10.1016/j.jde.2024.09.024
The Monge-Ampère type equations over bounded convex domains arise in a host of geometric applications. In this paper, we focus on the Dirichlet problem for a class of Monge-Ampère type equations, which can be degenerate or singular near the boundary of convex domains. Viscosity subsolutions and viscosity supersolutions to the problem can be constructed via comparison principle. Finally, we demonstrate the existence, uniqueness and a series of interior regularities (including with , with , and ) of the viscosity solution to the problem.
{"title":"Existence, uniqueness and interior regularity of viscosity solutions for a class of Monge-Ampère type equations","authors":"","doi":"10.1016/j.jde.2024.09.024","DOIUrl":"10.1016/j.jde.2024.09.024","url":null,"abstract":"<div><p>The Monge-Ampère type equations over bounded convex domains arise in a host of geometric applications. In this paper, we focus on the Dirichlet problem for a class of Monge-Ampère type equations, which can be degenerate or singular near the boundary of convex domains. Viscosity subsolutions and viscosity supersolutions to the problem can be constructed via comparison principle. Finally, we demonstrate the existence, uniqueness and a series of interior regularities (including <span><math><msup><mrow><mi>W</mi></mrow><mrow><mn>2</mn><mo>,</mo><mi>p</mi></mrow></msup></math></span> with <span><math><mi>p</mi><mo>∈</mo><mo>(</mo><mn>1</mn><mo>,</mo><mo>+</mo><mo>∞</mo><mo>)</mo></math></span>, <span><math><msup><mrow><mi>C</mi></mrow><mrow><mn>1</mn><mo>,</mo><mi>μ</mi></mrow></msup></math></span> with <span><math><mi>μ</mi><mo>∈</mo><mo>(</mo><mn>0</mn><mo>,</mo><mn>1</mn><mo>)</mo></math></span>, and <span><math><msup><mrow><mi>C</mi></mrow><mrow><mo>∞</mo></mrow></msup></math></span>) of the viscosity solution to the problem.</p></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-09-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142274259","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 : 2024-09-19DOI: 10.1016/j.jde.2024.09.021
We study a continuous transition from the discrete infinite Kuramoto model to the continuous counterpart in a whole time interval. The discrete infinite Kuramoto model corresponds to the discretization of the infinite Kuramoto model [18] via the first-order Euler discretization algorithm. For the proposed discrete infinite Kuramoto model, we study the emergent dynamics and uniform (-in-time) stability with respect to initial data under a suitable framework which is formulated in terms of system parameters and initial data. For a homogeneous ensemble with the same natural frequencies, we identify sufficient conditions for the existence of “quasi-stationary state” and complete synchronization. In contrast, for a heterogeneous ensemble, we also provide a weak emergent dynamics, namely “practical synchronization”. For the continuous transition in a zero time-step limit, we provide an improved truncation error estimate compared to the error estimate which can be obtained from the general theory for first-order discretized model using the uniform stability and emergent dynamics.
{"title":"Uniform-in-time stability and continuous transition of the time-discrete infinite Kuramoto model","authors":"","doi":"10.1016/j.jde.2024.09.021","DOIUrl":"10.1016/j.jde.2024.09.021","url":null,"abstract":"<div><p>We study a continuous transition from the discrete infinite Kuramoto model to the continuous counterpart in a whole time interval. The discrete infinite Kuramoto model corresponds to the discretization of the infinite Kuramoto model <span><span>[18]</span></span> via the first-order Euler discretization algorithm. For the proposed discrete infinite Kuramoto model, we study the emergent dynamics and uniform (-in-time) stability with respect to initial data under a suitable framework which is formulated in terms of system parameters and initial data. For a homogeneous ensemble with the same natural frequencies, we identify sufficient conditions for the existence of “quasi-stationary state” and complete synchronization. In contrast, for a heterogeneous ensemble, we also provide a weak emergent dynamics, namely “practical synchronization”. For the continuous transition in a zero time-step limit, we provide an improved truncation error estimate compared to the error estimate which can be obtained from the general theory for first-order discretized model using the uniform stability and emergent dynamics.</p></div>","PeriodicalId":15623,"journal":{"name":"Journal of Differential Equations","volume":null,"pages":null},"PeriodicalIF":2.4,"publicationDate":"2024-09-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142274363","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}