首页 > 最新文献

Journal of Functional Analysis最新文献

英文 中文
The high dimensional Fisher-KPP nonlocal diffusion equation with free boundary and radial symmetry, part 2: Sharp estimates 具有自由边界和径向对称性的高维 Fisher-KPP 非局部扩散方程,第 2 部分:锐利估计
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-08-31 DOI: 10.1016/j.jfa.2024.110649
Yihong Du, Wenjie Ni
<div><p>This is the second part of a two-part series devoted to an in depth understanding of the dynamical behaviour of the radially symmetric Fisher-KPP nonlocal diffusion equation with free boundary <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>=</mo><mi>h</mi><mo>(</mo><mi>t</mi><mo>)</mo></math></span>. In Part 1 <span><span>[19]</span></span>, we have shown that the long-time dynamics of this problem is characterised by a spreading-vanishing dichotomy, and there exists a threshold condition on the diffusion kernel <span><math><mi>J</mi><mo>(</mo><mo>|</mo><mi>x</mi><mo>|</mo><mo>)</mo></math></span> such that the spreading speed is ∞ when this condition is not satisfied, and when it is satisfied, the finite spreading speed <span><math><msub><mrow><mi>c</mi></mrow><mrow><mn>0</mn></mrow></msub></math></span> is determined by an associated semi-wave problem established in <span><span>[15]</span></span>. In Part 2 here, we obtain more precise description of the spreading profile by focusing on some natural classes of kernel functions, including those satisfying <span><math><mi>J</mi><mo>(</mo><mo>|</mo><mi>x</mi><mo>|</mo><mo>)</mo><mo>∼</mo><mo>|</mo><mi>x</mi><msup><mrow><mo>|</mo></mrow><mrow><mo>−</mo><mi>β</mi></mrow></msup></math></span> for <span><math><mo>|</mo><mi>x</mi><mo>|</mo><mo>≫</mo><mn>1</mn></math></span> in <span><math><msup><mrow><mi>R</mi></mrow><mrow><mi>N</mi></mrow></msup></math></span>. Our results for such kernels reveal a striking difference of behaviour from the pattern exhibited in the one dimension case <span><span>[18]</span></span> when <em>β</em> crosses the value <span><math><mi>N</mi><mo>+</mo><mn>2</mn></math></span>. More precisely, (a) when <span><math><mi>β</mi><mo>∈</mo><mo>(</mo><mi>N</mi><mo>,</mo><mi>N</mi><mo>+</mo><mn>1</mn><mo>]</mo></math></span>, we show that for <span><math><mi>t</mi><mo>≫</mo><mn>1</mn></math></span>, <span><math><mi>h</mi><mo>(</mo><mi>t</mi><mo>)</mo><mo>∼</mo><msup><mrow><mi>t</mi></mrow><mrow><mn>1</mn><mo>/</mo><mo>(</mo><mi>β</mi><mo>−</mo><mi>N</mi><mo>)</mo></mrow></msup></math></span> if <span><math><mi>β</mi><mo>∈</mo><mo>(</mo><mi>N</mi><mo>,</mo><mi>N</mi><mo>+</mo><mn>1</mn><mo>)</mo></math></span>, and <span><math><mi>h</mi><mo>(</mo><mi>t</mi><mo>)</mo><mo>∼</mo><mi>t</mi><mi>ln</mi><mo>⁡</mo><mi>t</mi></math></span> if <span><math><mi>β</mi><mo>=</mo><mi>N</mi><mo>+</mo><mn>1</mn></math></span>, which is of the same pattern as in dimension one, namely we recover the result in <span><span>[18]</span></span> by letting <span><math><mi>N</mi><mo>=</mo><mn>1</mn></math></span> in the above statements; (b) when <span><math><mi>β</mi><mo>∈</mo><mo>(</mo><mi>N</mi><mo>+</mo><mn>1</mn><mo>,</mo><mi>N</mi><mo>+</mo><mn>2</mn><mo>]</mo></math></span>, the front has a finite spreading speed <span><math><msub><mrow><mi>c</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>=</mo><msub><mrow><mi>c</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>(</mo><mi>β</mi><mo>)</mo></math></span> i
本文是两部分系列文章的第二部分,致力于深入理解自由边界 |x|=h(t) 的辐射对称 Fisher-KPP 非局部扩散方程的动力学行为。在第一部分[19]中,我们证明了该问题的长时动力学特征是扩散-消失二分法,扩散核 J(|x|) 存在一个阈值条件,当该条件不满足时,扩散速度为∞;当该条件满足时,有限扩散速度 c0 由[15]中建立的相关半波问题决定。在第 2 部分中,我们将重点研究一些自然类核函数,包括 RN 中满足 J(|x|)∼|x|-β for |x|≫1 的核函数,从而获得对传播曲线更精确的描述。当 β 越过 N+2 值时,我们对此类核的结果显示出与一维情况下[18]所表现出的行为模式的惊人差异。更确切地说,(a) 当 β∈(N,N+1]时,我们证明对于 t≫1,如果 β∈(N,N+1),则 h(t)∼t1/(β-N),如果 β=N+1 则 h(t)∼tlnt,这与一维情况下的模式相同,即我们通过在上述陈述中让 N=1 恢复了 [18] 中的结果;(b) 当 β∈(N+1,N+2]时,前沿有一个有限的扩散速度 c0=c0(β),即 limt→∞h(t)/t=c0;(c) 当 β>N+2 时,前沿仍具有有限的扩散速度 c0,但在 N≥2 与 N=1 之间,位移 c0t-h(t) 的阶次发生了显著变化:对于 t≫1,当 N≥2 时,c0t-h(t)∼lnt,但当 N=1 时,c0t-h(t)∼1。
{"title":"The high dimensional Fisher-KPP nonlocal diffusion equation with free boundary and radial symmetry, part 2: Sharp estimates","authors":"Yihong Du,&nbsp;Wenjie Ni","doi":"10.1016/j.jfa.2024.110649","DOIUrl":"10.1016/j.jfa.2024.110649","url":null,"abstract":"&lt;div&gt;&lt;p&gt;This is the second part of a two-part series devoted to an in depth understanding of the dynamical behaviour of the radially symmetric Fisher-KPP nonlocal diffusion equation with free boundary &lt;span&gt;&lt;math&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;h&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;. In Part 1 &lt;span&gt;&lt;span&gt;[19]&lt;/span&gt;&lt;/span&gt;, we have shown that the long-time dynamics of this problem is characterised by a spreading-vanishing dichotomy, and there exists a threshold condition on the diffusion kernel &lt;span&gt;&lt;math&gt;&lt;mi&gt;J&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; such that the spreading speed is ∞ when this condition is not satisfied, and when it is satisfied, the finite spreading speed &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;c&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; is determined by an associated semi-wave problem established in &lt;span&gt;&lt;span&gt;[15]&lt;/span&gt;&lt;/span&gt;. In Part 2 here, we obtain more precise description of the spreading profile by focusing on some natural classes of kernel functions, including those satisfying &lt;span&gt;&lt;math&gt;&lt;mi&gt;J&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;∼&lt;/mo&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;β&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt; for &lt;span&gt;&lt;math&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mo&gt;≫&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt; in &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt;. Our results for such kernels reveal a striking difference of behaviour from the pattern exhibited in the one dimension case &lt;span&gt;&lt;span&gt;[18]&lt;/span&gt;&lt;/span&gt; when &lt;em&gt;β&lt;/em&gt; crosses the value &lt;span&gt;&lt;math&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;. More precisely, (a) when &lt;span&gt;&lt;math&gt;&lt;mi&gt;β&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;]&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;, we show that for &lt;span&gt;&lt;math&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;≫&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;, &lt;span&gt;&lt;math&gt;&lt;mi&gt;h&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;∼&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;/&lt;/mo&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;β&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt; if &lt;span&gt;&lt;math&gt;&lt;mi&gt;β&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;, and &lt;span&gt;&lt;math&gt;&lt;mi&gt;h&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;∼&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mi&gt;ln&lt;/mi&gt;&lt;mo&gt;⁡&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; if &lt;span&gt;&lt;math&gt;&lt;mi&gt;β&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;, which is of the same pattern as in dimension one, namely we recover the result in &lt;span&gt;&lt;span&gt;[18]&lt;/span&gt;&lt;/span&gt; by letting &lt;span&gt;&lt;math&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt; in the above statements; (b) when &lt;span&gt;&lt;math&gt;&lt;mi&gt;β&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mo&gt;]&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;, the front has a finite spreading speed &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;c&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;c&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;β&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; i","PeriodicalId":15750,"journal":{"name":"Journal of Functional Analysis","volume":"287 12","pages":"Article 110649"},"PeriodicalIF":1.7,"publicationDate":"2024-08-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142161638","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}
引用次数: 0
The Widom–Sobolev formula for discontinuous matrix-valued symbols 不连续矩阵值符号的 Widom-Sobolev 公式
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-08-31 DOI: 10.1016/j.jfa.2024.110651
Leon Bollmann, Peter Müller

We prove the Widom–Sobolev formula for the asymptotic behaviour of truncated Wiener–Hopf operators with discontinuous matrix-valued symbols for three different classes of test functions. The symbols may depend on both position and momentum except when closing the asymptotics for twice differentiable test functions with Hölder singularities. The cut-off domains are allowed to have piecewise differentiable boundaries. In contrast to the case where the symbol is smooth in one variable, the resulting coefficient in the enhanced area law we obtain here remains as explicit for matrix-valued symbols as it is for scalar-valued symbols.

我们证明了具有不连续矩阵值符号的截断维纳-霍普夫算子的渐近行为的 Widom-Sobolev 公式,适用于三类不同的检验函数。符号可以同时取决于位置和动量,除非是在对具有霍尔德奇点的二次微分检验函数进行渐近分析时。允许截断域具有片断可变的边界。与符号在一个变量中是平滑的情况相反,我们在这里得到的增强面积定律中的系数对于矩阵值符号和标量值符号一样明确。
{"title":"The Widom–Sobolev formula for discontinuous matrix-valued symbols","authors":"Leon Bollmann,&nbsp;Peter Müller","doi":"10.1016/j.jfa.2024.110651","DOIUrl":"10.1016/j.jfa.2024.110651","url":null,"abstract":"<div><p>We prove the Widom–Sobolev formula for the asymptotic behaviour of truncated Wiener–Hopf operators with discontinuous matrix-valued symbols for three different classes of test functions. The symbols may depend on both position and momentum except when closing the asymptotics for twice differentiable test functions with Hölder singularities. The cut-off domains are allowed to have piecewise differentiable boundaries. In contrast to the case where the symbol is smooth in one variable, the resulting coefficient in the enhanced area law we obtain here remains as explicit for matrix-valued symbols as it is for scalar-valued symbols.</p></div>","PeriodicalId":15750,"journal":{"name":"Journal of Functional Analysis","volume":"287 12","pages":"Article 110651"},"PeriodicalIF":1.7,"publicationDate":"2024-08-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0022123624003392/pdfft?md5=8010699661a21471a1a6bd426ef43d6a&pid=1-s2.0-S0022123624003392-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142161640","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}
引用次数: 0
Porous medium type reaction-diffusion equation: Large time behaviors and regularity of free boundary 多孔介质型反应扩散方程:自由边界的大时间行为和正则性
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-08-31 DOI: 10.1016/j.jfa.2024.110643
Qingyou He
<div><p>We consider the Cauchy problem of the porous medium type reaction-diffusion equation<span><span><span><math><msub><mrow><mo>∂</mo></mrow><mrow><mi>t</mi></mrow></msub><mi>ρ</mi><mo>=</mo><mi>Δ</mi><msup><mrow><mi>ρ</mi></mrow><mrow><mi>m</mi></mrow></msup><mo>+</mo><mi>ρ</mi><mi>g</mi><mo>(</mo><mi>ρ</mi><mo>)</mo><mo>,</mo><mspace></mspace><mo>(</mo><mi>x</mi><mo>,</mo><mi>t</mi><mo>)</mo><mo>∈</mo><msup><mrow><mi>R</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>×</mo><msub><mrow><mi>R</mi></mrow><mrow><mo>+</mo></mrow></msub><mo>,</mo><mspace></mspace><mi>n</mi><mo>≥</mo><mn>2</mn><mo>,</mo><mspace></mspace><mi>m</mi><mo>></mo><mn>1</mn><mo>,</mo></math></span></span></span> where <em>g</em> is the given monotonic decreasing function with the density critical threshold <span><math><msub><mrow><mi>ρ</mi></mrow><mrow><mi>M</mi></mrow></msub><mo>></mo><mn>0</mn></math></span> satisfying <span><math><mi>g</mi><mo>(</mo><msub><mrow><mi>ρ</mi></mrow><mrow><mi>M</mi></mrow></msub><mo>)</mo><mo>=</mo><mn>0</mn></math></span>. We prove that the pressure <span><math><mi>P</mi><mo>:</mo><mo>=</mo><mfrac><mrow><mi>m</mi></mrow><mrow><mi>m</mi><mo>−</mo><mn>1</mn></mrow></mfrac><msup><mrow><mi>ρ</mi></mrow><mrow><mi>m</mi><mo>−</mo><mn>1</mn></mrow></msup></math></span> in <span><math><msubsup><mrow><mi>L</mi></mrow><mrow><mi>l</mi><mi>o</mi><mi>c</mi></mrow><mrow><mo>∞</mo></mrow></msubsup><mo>(</mo><msup><mrow><mi>R</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>)</mo></math></span> tends to the pressure critical threshold <span><math><msub><mrow><mi>P</mi></mrow><mrow><mi>M</mi></mrow></msub><mo>:</mo><mo>=</mo><mfrac><mrow><mi>m</mi></mrow><mrow><mi>m</mi><mo>−</mo><mn>1</mn></mrow></mfrac><msup><mrow><mo>(</mo><msub><mrow><mi>ρ</mi></mrow><mrow><mi>M</mi></mrow></msub><mo>)</mo></mrow><mrow><mi>m</mi><mo>−</mo><mn>1</mn></mrow></msup></math></span> at the time decay rate <span><math><msup><mrow><mo>(</mo><mn>1</mn><mo>+</mo><mi>t</mi><mo>)</mo></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup></math></span>. If the initial density <span><math><mi>ρ</mi><mo>(</mo><mi>x</mi><mo>,</mo><mn>0</mn><mo>)</mo></math></span> is compactly supported, we justify that the support <span><math><mo>{</mo><mi>x</mi><mo>:</mo><mi>ρ</mi><mo>(</mo><mi>x</mi><mo>,</mo><mi>t</mi><mo>)</mo><mo>></mo><mn>0</mn><mo>}</mo></math></span> of the density <em>ρ</em> expands exponentially in time. Furthermore, we show that there exists a time <span><math><msub><mrow><mi>T</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>></mo><mn>0</mn></math></span> such that the pressure <em>P</em> is Lipschitz continuous for <span><math><mi>t</mi><mo>></mo><msub><mrow><mi>T</mi></mrow><mrow><mn>0</mn></mrow></msub></math></span>, which is the optimal (sharp) regularity of the pressure, and the free surface <span><math><mo>∂</mo><mo>{</mo><mo>(</mo><mi>x</mi><mo>,</mo><mi>t</mi><mo>)</mo><mo>:</mo><mi>ρ</mi><mo>(</mo><mi>x</mi><mo>,</mo><mi>t</mi><mo>)</mo><mo>></mo><mn>0</mn><mo>}<
我们考虑多孔介质型反应扩散方程∂tρ=Δρm+ρg(ρ)的考奇问题,(x,t)∈Rn×R+,n≥2,m>1,其中g为给定的单调递减函数,密度临界阈值ρM>0满足g(ρM)=0。我们证明,Lloc∞(Rn) 中的压力 P:=mm-1ρm-1 以时间衰减率 (1+t)-1 趋向于压力临界阈值 PM:=mm-1(ρM)m-1。如果初始密度ρ(x,0)是紧凑支撑的,我们证明密度ρ的支撑{x:ρ(x,t)>0}随时间呈指数扩展。此外,我们证明存在一个时间 T0>0,使得压力 P 在 t>T0 时是 Lipschitz 连续的,这是压力的最优(锐利)正则性,并且自由表面 ∂{(x,t):ρ(x,t)>0}∩{t>T0} 是局部 Lipschitz 连续的。此外,在同样的紧凑支撑初始假设下,我们验证了自由边界∂{(x,t):ρ(x,t)>0}∩{t>T0}是局部 C1,α 曲面。
{"title":"Porous medium type reaction-diffusion equation: Large time behaviors and regularity of free boundary","authors":"Qingyou He","doi":"10.1016/j.jfa.2024.110643","DOIUrl":"10.1016/j.jfa.2024.110643","url":null,"abstract":"&lt;div&gt;&lt;p&gt;We consider the Cauchy problem of the porous medium type reaction-diffusion equation&lt;span&gt;&lt;span&gt;&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mo&gt;∂&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mi&gt;ρ&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;Δ&lt;/mi&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;ρ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;ρ&lt;/mi&gt;&lt;mi&gt;g&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;ρ&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt; where &lt;em&gt;g&lt;/em&gt; is the given monotonic decreasing function with the density critical threshold &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;ρ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;M&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt; satisfying &lt;span&gt;&lt;math&gt;&lt;mi&gt;g&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;ρ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;M&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;. We prove that the pressure &lt;span&gt;&lt;math&gt;&lt;mi&gt;P&lt;/mi&gt;&lt;mo&gt;:&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;ρ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt; in &lt;span&gt;&lt;math&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;L&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;l&lt;/mi&gt;&lt;mi&gt;o&lt;/mi&gt;&lt;mi&gt;c&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;∞&lt;/mo&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; tends to the pressure critical threshold &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;P&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;M&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;:&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;ρ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;M&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt; at the time decay rate &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt;. If the initial density &lt;span&gt;&lt;math&gt;&lt;mi&gt;ρ&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; is compactly supported, we justify that the support &lt;span&gt;&lt;math&gt;&lt;mo&gt;{&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;:&lt;/mo&gt;&lt;mi&gt;ρ&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;}&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; of the density &lt;em&gt;ρ&lt;/em&gt; expands exponentially in time. Furthermore, we show that there exists a time &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt; such that the pressure &lt;em&gt;P&lt;/em&gt; is Lipschitz continuous for &lt;span&gt;&lt;math&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;, which is the optimal (sharp) regularity of the pressure, and the free surface &lt;span&gt;&lt;math&gt;&lt;mo&gt;∂&lt;/mo&gt;&lt;mo&gt;{&lt;/mo&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;:&lt;/mo&gt;&lt;mi&gt;ρ&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;}&lt;","PeriodicalId":15750,"journal":{"name":"Journal of Functional Analysis","volume":"287 12","pages":"Article 110643"},"PeriodicalIF":1.7,"publicationDate":"2024-08-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142151202","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}
引用次数: 0
On the optimal rate for the convergence problem in mean field control 论平均场控制中收敛问题的最佳速率
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-08-31 DOI: 10.1016/j.jfa.2024.110660
Samuel Daudin , François Delarue , Joe Jackson

The goal of this work is to obtain (nearly) optimal rates for the convergence problem in mean field control. Our analysis covers cases where the solutions to the limiting problem may not be unique nor stable. Equivalently the value function of the limiting problem might not be differentiable on the entire space. Our main result is then to derive sharp rates of convergence in two distinct regimes. First, when the data is sufficiently regular, we obtain rates proportional to N1/2, with N being the number of particles, and we verify that N1/2 is indeed optimal in this setting. Second, when the data is merely Lipschitz and semi-concave with respect to the first Wasserstein distance, we obtain rates proportional to N2/(3d+6). We do not expect this second estimate to be optimal, but it improves substantially on the existing literature. Moreover, we construct an example showing that the optimal rate is no faster than N1/d, and we conjecture that the optimal rate should indeed be exactly N1/d (at least when d3). The key argument in our approach consists in mollifying the value function of the limiting problem in order to produce functions that are almost classical sub-solutions to the limiting Hamilton-Jacobi equation (which is a PDE set on the space of probability measures). These sub-solutions can be projected onto finite dimensional spaces and then compared with the value functions associated with the particle systems. In the end, this comparison is used to prove the most demanding bound in the estimates. The key challenge therein is thus to exhibit an appropriate form of mollification. We do so by employing sup-convolution within a convenient functional Hilbert space. To make the whole easier, we limit ourselves to the periodic setting. We also provide some examples to show that our results are sharp up to some extent.

这项工作的目标是获得平均场控制收敛问题的(近)最优率。我们的分析涵盖了极限问题解可能不唯一也不稳定的情况。同样,极限问题的值函数也可能在整个空间上不可微。因此,我们的主要结果是推导出两种不同情况下的急剧收敛速率。首先,当数据足够规则时,我们会得到与 N-1/2 成比例的收敛率,N 是粒子的数量,我们验证了 N-1/2 在这种情况下确实是最优的。其次,当数据仅仅是 Lipschitz 且与第一个 Wasserstein 距离呈半凹时,我们会得到与 N-2/(3d+6)成正比的速率。我们并不指望第二个估计值是最优的,但它大大改进了现有的文献。此外,我们还构建了一个例子,表明最佳速率不会快于 N-1/d,而且我们猜想最佳速率应该正好是 N-1/d(至少当 d≥3 时)。我们的方法的关键论点在于,对极限问题的值函数进行调和,以产生几乎是极限汉密尔顿-雅可比方程(这是概率度量空间上的一个 PDE 集)经典子解的函数。这些子解可以投影到有限维空间,然后与粒子系统相关的值函数进行比较。最后,这种比较被用来证明估计中最苛刻的约束。因此,其中的关键挑战在于展示一种适当的摩尔化形式。为此,我们在方便的函数希尔伯特空间内采用了超卷积。为了简化整个过程,我们将自己限制在周期性的环境中。我们还提供了一些例子来说明我们的结果在一定程度上是锐利的。
{"title":"On the optimal rate for the convergence problem in mean field control","authors":"Samuel Daudin ,&nbsp;François Delarue ,&nbsp;Joe Jackson","doi":"10.1016/j.jfa.2024.110660","DOIUrl":"10.1016/j.jfa.2024.110660","url":null,"abstract":"<div><p>The goal of this work is to obtain (nearly) optimal rates for the convergence problem in mean field control. Our analysis covers cases where the solutions to the limiting problem may not be unique nor stable. Equivalently the value function of the limiting problem might not be differentiable on the entire space. Our main result is then to derive sharp rates of convergence in two distinct regimes. First, when the data is sufficiently regular, we obtain rates proportional to <span><math><msup><mrow><mi>N</mi></mrow><mrow><mo>−</mo><mn>1</mn><mo>/</mo><mn>2</mn></mrow></msup></math></span>, with <em>N</em> being the number of particles, and we verify that <span><math><msup><mrow><mi>N</mi></mrow><mrow><mo>−</mo><mn>1</mn><mo>/</mo><mn>2</mn></mrow></msup></math></span> is indeed optimal in this setting. Second, when the data is merely Lipschitz and semi-concave with respect to the first Wasserstein distance, we obtain rates proportional to <span><math><msup><mrow><mi>N</mi></mrow><mrow><mo>−</mo><mn>2</mn><mo>/</mo><mo>(</mo><mn>3</mn><mi>d</mi><mo>+</mo><mn>6</mn><mo>)</mo></mrow></msup></math></span>. We do not expect this second estimate to be optimal, but it improves substantially on the existing literature. Moreover, we construct an example showing that the optimal rate is no faster than <span><math><msup><mrow><mi>N</mi></mrow><mrow><mo>−</mo><mn>1</mn><mo>/</mo><mi>d</mi></mrow></msup></math></span>, and we conjecture that the optimal rate should indeed be exactly <span><math><msup><mrow><mi>N</mi></mrow><mrow><mo>−</mo><mn>1</mn><mo>/</mo><mi>d</mi></mrow></msup></math></span> (at least when <span><math><mi>d</mi><mo>≥</mo><mn>3</mn></math></span>). The key argument in our approach consists in mollifying the value function of the limiting problem in order to produce functions that are almost classical sub-solutions to the limiting Hamilton-Jacobi equation (which is a PDE set on the space of probability measures). These sub-solutions can be projected onto finite dimensional spaces and then compared with the value functions associated with the particle systems. In the end, this comparison is used to prove the most demanding bound in the estimates. The key challenge therein is thus to exhibit an appropriate form of mollification. We do so by employing sup-convolution within a convenient functional Hilbert space. To make the whole easier, we limit ourselves to the periodic setting. We also provide some examples to show that our results are sharp up to some extent.</p></div>","PeriodicalId":15750,"journal":{"name":"Journal of Functional Analysis","volume":"287 12","pages":"Article 110660"},"PeriodicalIF":1.7,"publicationDate":"2024-08-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0022123624003483/pdfft?md5=5935f79205a900c37dc8ad1a51b88e6a&pid=1-s2.0-S0022123624003483-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142151206","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}
引用次数: 0
Norm convergence rate for multivariate quadratic polynomials of Wigner matrices 维格纳矩阵多元二次多项式的规范收敛率
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-08-31 DOI: 10.1016/j.jfa.2024.110647
Jacob Fronk , Torben Krüger , Yuriy Nemish

We study Hermitian non-commutative quadratic polynomials of multiple independent Wigner matrices. We prove that, with the exception of some specific reducible cases, the limiting spectral density of the polynomials always has a square root growth at its edges and prove an optimal local law around these edges. Combining these two results, we establish that, as the dimension N of the matrices grows to infinity, the operator norm of such polynomials q converges to a deterministic limit with a rate of convergence of N2/3+o(1). Here, the exponent in the rate of convergence is optimal. For the specific reducible cases, we also provide a classification of all possible edge behaviors.

我们研究了多个独立维格纳矩阵的赫米提非交换二次多项式。我们证明,除了一些特定的可还原情况外,多项式的极限谱密度在其边缘总是有平方根增长,并证明了这些边缘周围的最优局部规律。结合这两个结果,我们确定,当矩阵的维数 N 增长到无穷大时,此类多项式 q 的算子规范会收敛到一个确定的极限,收敛速率为 N-2/3+o(1)。这里,收敛速率的指数是最优的。对于特定的可还原情况,我们还提供了所有可能的边缘行为分类。
{"title":"Norm convergence rate for multivariate quadratic polynomials of Wigner matrices","authors":"Jacob Fronk ,&nbsp;Torben Krüger ,&nbsp;Yuriy Nemish","doi":"10.1016/j.jfa.2024.110647","DOIUrl":"10.1016/j.jfa.2024.110647","url":null,"abstract":"<div><p>We study Hermitian non-commutative quadratic polynomials of multiple independent Wigner matrices. We prove that, with the exception of some specific reducible cases, the limiting spectral density of the polynomials always has a square root growth at its edges and prove an optimal local law around these edges. Combining these two results, we establish that, as the dimension <em>N</em> of the matrices grows to infinity, the operator norm of such polynomials <em>q</em> converges to a deterministic limit with a rate of convergence of <span><math><msup><mrow><mi>N</mi></mrow><mrow><mo>−</mo><mn>2</mn><mo>/</mo><mn>3</mn><mo>+</mo><mi>o</mi><mo>(</mo><mn>1</mn><mo>)</mo></mrow></msup></math></span>. Here, the exponent in the rate of convergence is optimal. For the specific reducible cases, we also provide a classification of all possible edge behaviors.</p></div>","PeriodicalId":15750,"journal":{"name":"Journal of Functional Analysis","volume":"287 12","pages":"Article 110647"},"PeriodicalIF":1.7,"publicationDate":"2024-08-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0022123624003355/pdfft?md5=4e27857829ee38213729e119afe883b6&pid=1-s2.0-S0022123624003355-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142161642","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}
引用次数: 0
Small perturbations of polytopes 多边形的小扰动
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-08-30 DOI: 10.1016/j.jfa.2024.110644
Christian Kipp

Motivated by first-order conditions for extremal bodies of geometric functionals, we study a functional analytic notion of infinitesimal perturbations of convex bodies and give a full characterization of the set of realizable perturbations if the perturbed body is a polytope. As an application, we derive a necessary condition for polytopal maximizers of the isotropic constant.

受几何函数极值体的一阶条件的启发,我们研究了凸体无穷小扰动的函数解析概念,并给出了如果被扰动体是多面体,可实现扰动集合的完整特征。作为应用,我们推导出了等向常数多面体最大化的必要条件。
{"title":"Small perturbations of polytopes","authors":"Christian Kipp","doi":"10.1016/j.jfa.2024.110644","DOIUrl":"10.1016/j.jfa.2024.110644","url":null,"abstract":"<div><p>Motivated by first-order conditions for extremal bodies of geometric functionals, we study a functional analytic notion of infinitesimal perturbations of convex bodies and give a full characterization of the set of realizable perturbations if the perturbed body is a polytope. As an application, we derive a necessary condition for polytopal maximizers of the isotropic constant.</p></div>","PeriodicalId":15750,"journal":{"name":"Journal of Functional Analysis","volume":"287 12","pages":"Article 110644"},"PeriodicalIF":1.7,"publicationDate":"2024-08-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S002212362400332X/pdfft?md5=e462643d71502f41002932b5ab067bea&pid=1-s2.0-S002212362400332X-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142151201","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}
引用次数: 0
Locally universal C⁎-algebras with computable presentations 具有可计算呈现的局部通用 C⁎ 矩阵
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-08-30 DOI: 10.1016/j.jfa.2024.110652
Alec Fox , Isaac Goldbring , Bradd Hart

The Kirchberg Embedding Problem (KEP) asks if every C-algebra embeds into an ultrapower of the Cuntz algebra O2. Motivated by the recent refutation of the Connes Embedding Problem, we establish two computability-theoretic consequences of a positive solution to KEP. Both of our results follow from the a priori weaker assumption that there exists a locally universal C-algebra with a computable presentation.

基希贝格嵌入问题(Kirchberg Embedding Problem,KEP)询问是否每个 C⁎-代数都嵌入到 Cuntz 代数 O2 的一个超幂中。受最近反驳康恩嵌入问题的启发,我们建立了 KEP 正解的两个可计算性理论后果。我们的这两个结果都来自一个先验的较弱假设,即存在一个具有可计算呈现的局部普适 C⁎-代数。
{"title":"Locally universal C⁎-algebras with computable presentations","authors":"Alec Fox ,&nbsp;Isaac Goldbring ,&nbsp;Bradd Hart","doi":"10.1016/j.jfa.2024.110652","DOIUrl":"10.1016/j.jfa.2024.110652","url":null,"abstract":"<div><p>The Kirchberg Embedding Problem (KEP) asks if every <span><math><msup><mrow><mi>C</mi></mrow><mrow><mo>⁎</mo></mrow></msup></math></span>-algebra embeds into an ultrapower of the Cuntz algebra <span><math><msub><mrow><mi>O</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span>. Motivated by the recent refutation of the Connes Embedding Problem, we establish two computability-theoretic consequences of a positive solution to KEP. Both of our results follow from the a priori weaker assumption that there exists a locally universal <span><math><msup><mrow><mi>C</mi></mrow><mrow><mo>⁎</mo></mrow></msup></math></span>-algebra with a computable presentation.</p></div>","PeriodicalId":15750,"journal":{"name":"Journal of Functional Analysis","volume":"287 12","pages":"Article 110652"},"PeriodicalIF":1.7,"publicationDate":"2024-08-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142172920","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}
引用次数: 0
Random Carleson sequences for the Hardy space on the polydisc and the unit ball 多圆盘和单位球上哈代空间的随机卡列松序列
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-08-30 DOI: 10.1016/j.jfa.2024.110659
Nikolaos Chalmoukis , Alberto Dayan , Giuseppe Lamberti

We study the Kolmogorov 01 law for a random sequence with prescribed radii so that it generates a Carleson measure almost surely, both for the Hardy space on the polydisc and the Hardy space on the unit ball, thus providing improved versions of previous results of the first two authors and of a separate result of Massaneda. In the polydisc, the geometry of such sequences is not well understood, so we proceed by studying the random Gramians generated by random sequences, using tools from the theory of random matrices. Another result we prove, and that is of its own relevance, is the 01 law for a random sequence to be partitioned into M separated sequences with respect to the pseudo-hyperbolic distance, which is used also to describe the random sequences that are interpolating for the Bloch space on the unit disc almost surely.

我们研究了具有规定半径的随机序列的柯尔莫哥洛夫 0-1 定律,从而使其几乎肯定地产生卡列松度量,这既适用于多圆盘上的哈代空间,也适用于单位球上的哈代空间,从而提供了前两位作者先前结果和马萨内达单独结果的改进版本。在多圆盘上,人们对这类序列的几何结构还不太了解,因此我们利用随机矩阵理论的工具,研究随机序列产生的随机格拉米安。我们证明的另一个结果本身也具有相关性,那就是关于伪双曲距离的随机序列被分割成 M 个分离序列的 0-1 规律,该规律也用于描述几乎肯定插值为单位圆盘上布洛赫空间的随机序列。
{"title":"Random Carleson sequences for the Hardy space on the polydisc and the unit ball","authors":"Nikolaos Chalmoukis ,&nbsp;Alberto Dayan ,&nbsp;Giuseppe Lamberti","doi":"10.1016/j.jfa.2024.110659","DOIUrl":"10.1016/j.jfa.2024.110659","url":null,"abstract":"<div><p>We study the Kolmogorov <span><math><mn>0</mn><mo>−</mo><mn>1</mn></math></span> law for a random sequence with prescribed radii so that it generates a Carleson measure almost surely, both for the Hardy space on the polydisc and the Hardy space on the unit ball, thus providing improved versions of previous results of the first two authors and of a separate result of Massaneda. In the polydisc, the geometry of such sequences is not well understood, so we proceed by studying the random Gramians generated by random sequences, using tools from the theory of random matrices. Another result we prove, and that is of its own relevance, is the <span><math><mn>0</mn><mo>−</mo><mn>1</mn></math></span> law for a random sequence to be partitioned into <em>M</em> separated sequences with respect to the pseudo-hyperbolic distance, which is used also to describe the random sequences that are interpolating for the Bloch space on the unit disc almost surely.</p></div>","PeriodicalId":15750,"journal":{"name":"Journal of Functional Analysis","volume":"287 12","pages":"Article 110659"},"PeriodicalIF":1.7,"publicationDate":"2024-08-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0022123624003471/pdfft?md5=002a3ca282e7fe0e69899ce4b770adcb&pid=1-s2.0-S0022123624003471-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142161637","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}
引用次数: 0
Weak solutions of anisotropic (and crystalline) inverse mean curvature flow as limits of p-capacitary potentials 作为 p 电容势极限的各向异性(和晶体)反平均曲率流的弱解
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-08-28 DOI: 10.1016/j.jfa.2024.110642
Esther Cabezas-Rivas , Salvador Moll , Marcos Solera

We construct weak solutions of the anisotropic inverse mean curvature flow (A-IMCF) under very mild assumptions both on the anisotropy (which is simply a norm in RN with no ellipticity nor smoothness requirements, in order to include the crystalline case) and on the initial data. By means of an approximation procedure introduced by Moser, our solutions are limits of anisotropic p-harmonic functions or p-capacitary functions (after a change of variable), and we get uniqueness both for the approximating solutions (i.e., uniqueness of p-capacitary functions) and the limiting ones. Our notion of weak solution still recovers variational and geometric definitions similar to those introduced by Huisken-Ilmanen, but requires to work within the broader setting of BV-functions. Despite of this, we still reach classical results like the continuity and exponential growth of perimeter, as well as outward minimizing properties of the sublevel sets. Moreover, by assuming the extra regularity given by an interior rolling ball condition (where a sliding Wulff shape plays the role of a ball), the solutions are shown to be continuous and satisfy Harnack inequalities. Finally, examples of explicit solutions are built.

我们在对各向异性(它只是 RN 中的一个规范,没有椭圆性或光滑性的要求,以便包括晶体情况)和初始数据作非常温和的假设下,构建了各向异性反向平均曲率流(A-IMCF)的弱解。通过莫泽引入的近似程序,我们的解是各向异性 p 谐函数或 p 容函数(变量改变后)的极限,我们得到了近似解(即 p 容函数的唯一性)和极限解的唯一性。我们的弱解概念仍然恢复了类似于 Huisken-Ilmanen 引入的变分和几何定义,但需要在更广泛的 BV 函数背景下工作。尽管如此,我们仍然获得了经典结果,如周长的连续性和指数增长,以及子级集的向外最小化特性。此外,通过假设内部滚动球条件(其中滑动的 Wulff 形状扮演球的角色)给出的额外规则性,我们证明了解的连续性并满足哈纳克不等式。最后,还建立了显式解的实例。
{"title":"Weak solutions of anisotropic (and crystalline) inverse mean curvature flow as limits of p-capacitary potentials","authors":"Esther Cabezas-Rivas ,&nbsp;Salvador Moll ,&nbsp;Marcos Solera","doi":"10.1016/j.jfa.2024.110642","DOIUrl":"10.1016/j.jfa.2024.110642","url":null,"abstract":"<div><p>We construct weak solutions of the anisotropic inverse mean curvature flow (A-IMCF) under very mild assumptions both on the anisotropy (which is simply a norm in <span><math><msup><mrow><mi>R</mi></mrow><mrow><mi>N</mi></mrow></msup></math></span> with no ellipticity nor smoothness requirements, in order to include the crystalline case) and on the initial data. By means of an approximation procedure introduced by Moser, our solutions are limits of anisotropic <em>p</em>-harmonic functions or <em>p</em>-capacitary functions (after a change of variable), and we get uniqueness both for the approximating solutions (i.e., uniqueness of <em>p</em>-capacitary functions) and the limiting ones. Our notion of weak solution still recovers variational and geometric definitions similar to those introduced by Huisken-Ilmanen, but requires to work within the broader setting of <em>BV</em>-functions. Despite of this, we still reach classical results like the continuity and exponential growth of perimeter, as well as outward minimizing properties of the sublevel sets. Moreover, by assuming the extra regularity given by an interior rolling ball condition (where a sliding Wulff shape plays the role of a ball), the solutions are shown to be continuous and satisfy Harnack inequalities. Finally, examples of explicit solutions are built.</p></div>","PeriodicalId":15750,"journal":{"name":"Journal of Functional Analysis","volume":"287 11","pages":"Article 110642"},"PeriodicalIF":1.7,"publicationDate":"2024-08-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0022123624003306/pdfft?md5=b8aed4f15cb7f0e5872276ff50c4a2cd&pid=1-s2.0-S0022123624003306-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142130089","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}
引用次数: 0
A geometric Elliott invariant and noncommutative rigidity of mapping tori 映射环的几何埃利奥特不变性和非交换刚性
IF 1.7 2区 数学 Q1 MATHEMATICS Pub Date : 2024-08-13 DOI: 10.1016/j.jfa.2024.110625
Hao Guo , Valerio Proietti , Hang Wang

We prove a rigidity property for mapping tori associated to minimal topological dynamical systems using tools from noncommutative geometry. More precisely, we show that under mild geometric assumptions, a leafwise homotopy equivalence of two mapping tori associated to Zd-actions on a compact space can be lifted to an isomorphism of their foliation C-algebras. This property is a noncommutative analogue of topological rigidity in the context of foliated spaces whose space of leaves is singular, where isomorphism type of the C-algebra replaces homeomorphism type. Our technique is to develop a geometric approach to the Elliott invariant that relies on topological and index-theoretic data from the mapping torus. We also discuss how our construction can be extended to slightly more general homotopy quotients arising from actions of discrete cocompact subgroups of simply connected solvable Lie groups, as well as how the theory can be applied to the magnetic gap-labelling problem for certain Cantor minimal systems.

我们利用非交换几何学的工具证明了与最小拓扑动力系统相关的映射环的刚性属性。更确切地说,我们证明了在温和的几何假设条件下,与紧凑空间上的 Zd 作用相关的两个映射环的叶向同调等价性可以提升为它们的叶状 C⁎-代数的同构性。这一性质是叶子空间奇异的叶状空间中拓扑刚性的非交换类似物,其中 C⁎-代数的同构类型取代了同构类型。我们的技术是利用来自映射环的拓扑和索引理论数据,开发出一种几何方法来实现埃利奥特不变量。我们还讨论了如何将我们的构造扩展到由简单连通的可解李群的离散可紧密子群的作用所产生的稍微更一般的同调商,以及如何将该理论应用于某些康托最小系统的磁隙标注问题。
{"title":"A geometric Elliott invariant and noncommutative rigidity of mapping tori","authors":"Hao Guo ,&nbsp;Valerio Proietti ,&nbsp;Hang Wang","doi":"10.1016/j.jfa.2024.110625","DOIUrl":"10.1016/j.jfa.2024.110625","url":null,"abstract":"<div><p>We prove a rigidity property for mapping tori associated to minimal topological dynamical systems using tools from noncommutative geometry. More precisely, we show that under mild geometric assumptions, a leafwise homotopy equivalence of two mapping tori associated to <span><math><msup><mrow><mi>Z</mi></mrow><mrow><mi>d</mi></mrow></msup></math></span>-actions on a compact space can be lifted to an isomorphism of their foliation <span><math><msup><mrow><mi>C</mi></mrow><mrow><mo>⁎</mo></mrow></msup></math></span>-algebras. This property is a noncommutative analogue of topological rigidity in the context of foliated spaces whose space of leaves is singular, where isomorphism type of the <span><math><msup><mrow><mi>C</mi></mrow><mrow><mo>⁎</mo></mrow></msup></math></span>-algebra replaces homeomorphism type. Our technique is to develop a geometric approach to the Elliott invariant that relies on topological and index-theoretic data from the mapping torus. We also discuss how our construction can be extended to slightly more general homotopy quotients arising from actions of discrete cocompact subgroups of simply connected solvable Lie groups, as well as how the theory can be applied to the magnetic gap-labelling problem for certain Cantor minimal systems.</p></div>","PeriodicalId":15750,"journal":{"name":"Journal of Functional Analysis","volume":"287 11","pages":"Article 110625"},"PeriodicalIF":1.7,"publicationDate":"2024-08-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0022123624003136/pdfft?md5=a1cbbfe5bdbc4ef488f7c160f8a48b02&pid=1-s2.0-S0022123624003136-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142076533","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}
引用次数: 0
期刊
Journal of Functional Analysis
全部 Acc. Chem. Res. ACS Applied Bio Materials ACS Appl. Electron. Mater. ACS Appl. Energy Mater. ACS Appl. Mater. Interfaces ACS Appl. Nano Mater. ACS Appl. Polym. Mater. ACS BIOMATER-SCI ENG ACS Catal. ACS Cent. Sci. ACS Chem. Biol. ACS Chemical Health & Safety ACS Chem. Neurosci. ACS Comb. Sci. ACS Earth Space Chem. ACS Energy Lett. ACS Infect. Dis. ACS Macro Lett. ACS Mater. Lett. ACS Med. Chem. Lett. ACS Nano ACS Omega ACS Photonics ACS Sens. ACS Sustainable Chem. Eng. ACS Synth. Biol. Anal. Chem. BIOCHEMISTRY-US Bioconjugate Chem. BIOMACROMOLECULES Chem. Res. Toxicol. Chem. Rev. Chem. Mater. CRYST GROWTH DES ENERG FUEL Environ. Sci. Technol. Environ. Sci. Technol. Lett. Eur. J. Inorg. Chem. IND ENG CHEM RES Inorg. Chem. J. Agric. Food. Chem. J. Chem. Eng. Data J. Chem. Educ. J. Chem. Inf. Model. J. Chem. Theory Comput. J. Med. Chem. J. Nat. Prod. J PROTEOME RES J. Am. Chem. Soc. LANGMUIR MACROMOLECULES Mol. Pharmaceutics Nano Lett. Org. Lett. ORG PROCESS RES DEV ORGANOMETALLICS J. Org. Chem. J. Phys. Chem. J. Phys. Chem. A J. Phys. Chem. B J. Phys. Chem. C J. Phys. Chem. Lett. Analyst Anal. Methods Biomater. Sci. Catal. Sci. Technol. Chem. Commun. Chem. Soc. Rev. CHEM EDUC RES PRACT CRYSTENGCOMM Dalton Trans. Energy Environ. Sci. ENVIRON SCI-NANO ENVIRON SCI-PROC IMP ENVIRON SCI-WAT RES Faraday Discuss. Food Funct. Green Chem. Inorg. Chem. Front. Integr. Biol. J. Anal. At. Spectrom. J. Mater. Chem. A J. Mater. Chem. B J. Mater. Chem. C Lab Chip Mater. Chem. Front. Mater. Horiz. MEDCHEMCOMM Metallomics Mol. Biosyst. Mol. Syst. Des. Eng. Nanoscale Nanoscale Horiz. Nat. Prod. Rep. New J. Chem. Org. Biomol. Chem. Org. Chem. Front. PHOTOCH PHOTOBIO SCI PCCP Polym. Chem.
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
0
微信
客服QQ
Book学术公众号 扫码关注我们
反馈
×
意见反馈
请填写您的意见或建议
请填写您的手机或邮箱
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
现在去查看 取消
×
提示
确定
Book学术官方微信
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术
文献互助 智能选刊 最新文献 互助须知 联系我们:info@booksci.cn
Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。
Copyright © 2023 Book学术 All rights reserved.
ghs 京公网安备 11010802042870号 京ICP备2023020795号-1