Under suitable growth and coercivity conditions on the nonlinear damping operator $g$ which ensure non-resonance, we estimate the ultimate bound of the energy of the general solution to the equation $ddot{u}(t) + Au(t) + g(dot{u}(t))=h(t),quad tinmathbb{R}^+ ,$ where $A$ is a positive selfadjoint operator on a Hilbert space $H$ and $h$ is a bounded forcing term with values in $H$. In general the bound is of the form $ C(1+ ||h||^4)$ where $||h||$ stands for the $L^infty$ norm of $h$ with values in $H$ and the growth of $g$ does not seem to play any role. If $g$ behaves lie a power for large values of the velocity, the ultimate bound has a quadratic growth with respect to $||h||$ and this result is optimal. If $h$ is anti periodic, we obtain a much lower growth bound and again the result is shown to be optimal even for scalar ODEs.
{"title":"On the ultimate energy bound of solutions to some forced second-order evolution equations with a general nonlinear damping operator","authors":"A. Haraux","doi":"10.2140/tunis.2019.1.59","DOIUrl":"https://doi.org/10.2140/tunis.2019.1.59","url":null,"abstract":"Under suitable growth and coercivity conditions on the nonlinear damping operator $g$ which ensure non-resonance, we estimate the ultimate bound of the energy of the general solution to the equation $ddot{u}(t) + Au(t) + g(dot{u}(t))=h(t),quad tinmathbb{R}^+ ,$ where $A$ is a positive selfadjoint operator on a Hilbert space $H$ and $h$ is a bounded forcing term with values in $H$. In general the bound is of the form $ C(1+ ||h||^4)$ where $||h||$ stands for the $L^infty$ norm of $h$ with values in $H$ and the growth of $g$ does not seem to play any role. If $g$ behaves lie a power for large values of the velocity, the ultimate bound has a quadratic growth with respect to $||h||$ and this result is optimal. If $h$ is anti periodic, we obtain a much lower growth bound and again the result is shown to be optimal even for scalar ODEs.","PeriodicalId":36030,"journal":{"name":"Tunisian Journal of Mathematics","volume":" ","pages":""},"PeriodicalIF":0.9,"publicationDate":"2017-08-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.2140/tunis.2019.1.59","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"45191818","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
We derive the hydrodynamic limit of a kinetic equation where the interactions in velocity are modelled by a linear operator (Fokker-Planck or Linear Boltzmann) and the force in the Vlasov term is a stochastic process with high amplitude and short-range correlation. In the scales and the regime we consider, the hydrodynamic equation is a scalar second-order stochastic partial differential equation. Compared to the deterministic case, we also observe a phenomenon of enhanced diffusion.
{"title":"Diffusion-approximation in stochastically forced kinetic equations","authors":"A. Debussche, J. Vovelle","doi":"10.2140/TUNIS.2021.3.1","DOIUrl":"https://doi.org/10.2140/TUNIS.2021.3.1","url":null,"abstract":"We derive the hydrodynamic limit of a kinetic equation where the interactions in velocity are modelled by a linear operator (Fokker-Planck or Linear Boltzmann) and the force in the Vlasov term is a stochastic process with high amplitude and short-range correlation. In the scales and the regime we consider, the hydrodynamic equation is a scalar second-order stochastic partial differential equation. Compared to the deterministic case, we also observe a phenomenon of enhanced diffusion.","PeriodicalId":36030,"journal":{"name":"Tunisian Journal of Mathematics","volume":" ","pages":""},"PeriodicalIF":0.9,"publicationDate":"2017-07-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.2140/TUNIS.2021.3.1","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"47373915","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2017-07-19DOI: 10.2140/tunis.2019.1.151
P. Auscher, S. Bortz, Moritz Egert, Olli Saari
A functional analytic approach to obtaining self-improving properties of solutions to linear non-local elliptic equations is presented. It yields conceptually simple and very short proofs of some previous results due to Kuusi–Mingione–Sire and Bass–Ren. Its flexibility is demonstrated by new applications to non-autonomous parabolic equations with non-local elliptic part and questions related to maximal regularity.
{"title":"Nonlocal self-improving properties: a functional analytic approach","authors":"P. Auscher, S. Bortz, Moritz Egert, Olli Saari","doi":"10.2140/tunis.2019.1.151","DOIUrl":"https://doi.org/10.2140/tunis.2019.1.151","url":null,"abstract":"A functional analytic approach to obtaining self-improving properties of solutions to linear non-local elliptic equations is presented. It yields conceptually simple and very short proofs of some previous results due to Kuusi–Mingione–Sire and Bass–Ren. Its flexibility is demonstrated by new applications to non-autonomous parabolic equations with non-local elliptic part and questions related to maximal regularity.","PeriodicalId":36030,"journal":{"name":"Tunisian Journal of Mathematics","volume":" ","pages":""},"PeriodicalIF":0.9,"publicationDate":"2017-07-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.2140/tunis.2019.1.151","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"47045074","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
We consider the semilinear heat equation begin{eqnarray*} partial_t u = Delta u + |u|^{p-1} u ln ^{alpha}( u^2 +2), end{eqnarray*} in the whole space $mathbb{R}^n$, where $p > 1$ and $ alpha in mathbb{R}$. Unlike the standard case $alpha = 0$, this equation is not scaling invariant. We construct for this equation a solution which blows up in finite time $T$ only at one blowup point $a$, according to the following asymptotic dynamics: begin{eqnarray*} u(x,t) sim psi(t) left(1 + frac{(p-1)|x-a|^2}{4p(T -t)|ln(T -t)|} right)^{-frac{1}{p-1}} text{ as } t to T, end{eqnarray*} where $psi(t)$ is the unique positive solution of the ODE begin{eqnarray*} psi' = psi^p ln^{alpha}(psi^2 +2), quad lim_{tto T}psi(t) = + infty. end{eqnarray*} The construction relies on the reduction of the problem to a finite dimensional one and a topological argument based on the index theory to get the conclusion. By the interpretation of the parameters of the finite dimensional problem in terms of the blowup time and the blowup point, we show the stability of the constructed solution with respect to perturbations in initial data. To our knowledge, this is the first successful construction for a genuinely non-scale invariant PDE of a stable blowup solution with the derivation of the blowup profile. From this point of view, we consider our result as a breakthrough.
{"title":"Construction of a stable blowup solution with a prescribed behavior for a non-scaling-invariant semilinear heat equation","authors":"G. K. Duong, V. T. Nguyen, H. Zaag","doi":"10.2140/tunis.2019.1.13","DOIUrl":"https://doi.org/10.2140/tunis.2019.1.13","url":null,"abstract":"We consider the semilinear heat equation begin{eqnarray*} partial_t u = Delta u + |u|^{p-1} u ln ^{alpha}( u^2 +2), end{eqnarray*} in the whole space $mathbb{R}^n$, where $p > 1$ and $ alpha in mathbb{R}$. Unlike the standard case $alpha = 0$, this equation is not scaling invariant. We construct for this equation a solution which blows up in finite time $T$ only at one blowup point $a$, according to the following asymptotic dynamics: begin{eqnarray*} u(x,t) sim psi(t) left(1 + frac{(p-1)|x-a|^2}{4p(T -t)|ln(T -t)|} right)^{-frac{1}{p-1}} text{ as } t to T, end{eqnarray*} where $psi(t)$ is the unique positive solution of the ODE begin{eqnarray*} psi' = psi^p ln^{alpha}(psi^2 +2), quad lim_{tto T}psi(t) = + infty. end{eqnarray*} The construction relies on the reduction of the problem to a finite dimensional one and a topological argument based on the index theory to get the conclusion. By the interpretation of the parameters of the finite dimensional problem in terms of the blowup time and the blowup point, we show the stability of the constructed solution with respect to perturbations in initial data. To our knowledge, this is the first successful construction for a genuinely non-scale invariant PDE of a stable blowup solution with the derivation of the blowup profile. From this point of view, we consider our result as a breakthrough.","PeriodicalId":36030,"journal":{"name":"Tunisian Journal of Mathematics","volume":" ","pages":""},"PeriodicalIF":0.9,"publicationDate":"2017-04-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.2140/tunis.2019.1.13","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"45901813","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2017-03-01DOI: 10.2140/tunis.2020.2.287
Bruce W. Jordan, Z. Klagsbrun, B. Poonen, C. Skinner, Yevgeny Zaytman
For each odd prime $p$, we conjecture the distribution of the $p$-torsion subgroup of $K_{2n}(mathcal{O}_F)$ as $F$ ranges over real quadratic fields, or over imaginary quadratic fields. We then prove that the average size of the $3$-torsion subgroup of $K_{2n}(mathcal{O}_F)$ is as predicted by this conjecture.
{"title":"Statistics of K-groups modulo p for the ring of\u0000integers of a varying quadratic number field","authors":"Bruce W. Jordan, Z. Klagsbrun, B. Poonen, C. Skinner, Yevgeny Zaytman","doi":"10.2140/tunis.2020.2.287","DOIUrl":"https://doi.org/10.2140/tunis.2020.2.287","url":null,"abstract":"For each odd prime $p$, we conjecture the distribution of the $p$-torsion subgroup of $K_{2n}(mathcal{O}_F)$ as $F$ ranges over real quadratic fields, or over imaginary quadratic fields. We then prove that the average size of the $3$-torsion subgroup of $K_{2n}(mathcal{O}_F)$ is as predicted by this conjecture.","PeriodicalId":36030,"journal":{"name":"Tunisian Journal of Mathematics","volume":" ","pages":""},"PeriodicalIF":0.9,"publicationDate":"2017-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.2140/tunis.2020.2.287","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"48171694","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}