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Some aspects of the Floquet theory for the heat equation in a periodic domain 周期域中热方程的 Floquet 理论的某些方面
IF 1.4 3区 数学 Q1 MATHEMATICS Pub Date : 2024-03-15 DOI: 10.1007/s00028-024-00951-0
Marcus Rosenberg, Jari Taskinen

We treat the linear heat equation in a periodic waveguide (Pi subset {{mathbb {R}}}^d), with a regular enough boundary, by using the Floquet transform methods. Applying the Floquet transform ({{textsf{F}}}) to the equation yields a heat equation with mixed boundary conditions on the periodic cell (varpi ) of (Pi ), and we analyse the connection between the solutions of the two problems. The considerations involve a description of the spectral projections onto subspaces ({{mathcal {H}}}_S subset L^2(Pi )) corresponding certain spectral components. We also show that the translated Wannier functions form an orthonormal basis in ({{mathcal {H}}}_S).

我们使用弗洛克特变换方法来处理具有足够规则边界的周期波导 (Pi 子集 {{mathbb {R}}^d) 中的线性热方程。将 Floquet 变换 ({{textsf{F}}})应用于方程,可以得到一个在 (Pi )的周期单元 (varpi )上具有混合边界条件的热方程,我们分析了这两个问题的解之间的联系。这些考虑涉及到对子空间 ({{mathcal {H}}_S subset L^2(Pi )) 对应于某些谱成分的谱投影的描述。我们还证明了平移的万尼尔函数在 ({{mathcal {H}}_S) 中形成了一个正交基。)
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引用次数: 0
On the separation property and the global attractor for the nonlocal Cahn-Hilliard equation in three dimensions 论三维非局部卡恩-希利亚德方程的分离特性和全局吸引子
IF 1.4 3区 数学 Q1 MATHEMATICS Pub Date : 2024-03-15 DOI: 10.1007/s00028-024-00953-y
Andrea Giorgini

We consider the nonlocal Cahn-Hilliard equation with constant mobility and singular potential in three dimensional bounded and smooth domains. This model describes phase separation in binary fluid mixtures. Given any global solution (whose existence and uniqueness are already known), we prove the so-called instantaneous and uniform separation property: any global solution with initial finite energy is globally confined (in the (L^infty ) metric) in the interval ([-1+delta ,1-delta ]) on the time interval ([tau ,infty )) for any (tau >0), where (delta ) only depends on the norms of the initial datum, (tau ) and the parameters of the system. We then exploit such result to improve the regularity of the global attractor for the dynamical system associated to the problem.

我们考虑了三维有界光滑域中具有恒定流动性和奇异势能的非局部卡恩-希利亚德方程。该模型描述了二元流体混合物中的相分离。给定任何全局解(其存在性和唯一性已经已知),我们证明了所谓的瞬时均匀分离特性:对于任意(tau >;0), 其中 (delta ) 只取决于初始基准的规范、 (tau ) 和系统的参数。然后,我们利用这一结果来改善与问题相关的动力系统的全局吸引子的正则性。
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引用次数: 0
Bi-objective and hierarchical control for the Burgers equation 布尔格斯方程的双目标和分层控制
IF 1.4 3区 数学 Q1 MATHEMATICS Pub Date : 2024-03-15 DOI: 10.1007/s00028-024-00952-z
F. D. Araruna, E. Fernández-Cara, L. C. da Silva

We present some results concerning the control of the Burgers equation. We analyze a bi-objective optimal control problem and then the hierarchical null controllability through a Stackelberg–Nash strategy, with one leader and two followers. The results may be viewed as an extension to this nonlinear setting of a previous analysis performed for linear and semilinear heat equations. They can also be regarded as a first step in the solution of control problems of this kind for the Navier–Stokes equations.

我们介绍了有关布尔格斯方程控制的一些结果。我们分析了一个双目标最优控制问题,然后通过一个领导者和两个跟随者的 Stackelberg-Nash 策略分析了分层空可控性。这些结果可以看作是之前对线性和半线性热方程分析在非线性环境下的扩展。这些结果也可视为解决 Navier-Stokes 方程中此类控制问题的第一步。
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引用次数: 0
Strong solutions and attractor dimension for 2D NSE with dynamic boundary conditions 具有动态边界条件的二维 NSE 的强解和吸引子维度
IF 1.4 3区 数学 Q1 MATHEMATICS Pub Date : 2024-03-15 DOI: 10.1007/s00028-024-00948-9

Abstract

We consider incompressible Navier–Stokes equations in a bounded 2D domain, complete with the so-called dynamic slip boundary conditions. Assuming that the data are regular, we show that weak solutions are strong. As an application, we provide an explicit upper bound of the fractal dimension of the global attractor in terms of the physical parameters. These estimates comply with analogous results in the case of Dirichlet boundary condition.

摘要 我们考虑了有界二维域中的不可压缩纳维-斯托克斯方程,其中包含所谓的动态滑移边界条件。假设数据是规则的,我们证明弱解是强解。作为一种应用,我们根据物理参数提供了全局吸引子分形维度的明确上限。这些估计值与 Dirichlet 边界条件情况下的类似结果一致。
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引用次数: 0
Remarks on uniqueness and energy conservation for electron-MHD system 关于电子-MHD 系统唯一性和能量守恒的评论
IF 1.4 3区 数学 Q1 MATHEMATICS Pub Date : 2024-03-15 DOI: 10.1007/s00028-024-00955-w
Fan Wu

This paper is concerned with the uniqueness and energy conservation of weak solutions for Electron-MHD system. Under suitable assumptions, we first show that the Electron-MHD system has a unique weak solution. In addition, we show that weak solution conserves energy if (nabla times bin L^2(0, T; L^4({mathbb {R}}^d))(dge 2)) or ( nabla times b in L^{frac{4d+8}{d+4}}left( 0, T; L^{frac{4d+8}{d+4}}({mathbb {R}}^{d})right) (d=2, 3, 4)).

本文主要研究电子-MHD 系统弱解的唯一性和能量守恒问题。在合适的假设条件下,我们首先证明了电子-MHD系统有唯一的弱解。此外,我们还证明了如果在 L^2(0,T.)中 (nabla times bin L^2(0, T.), 则弱解能量守恒;L^4({mathbb {R}}^d))(dge 2))或者(( nabla times b in L^{frac{4d+8}{d+4}}left( 0, T; L^{frac{4d+8}{d+4}}({mathbb {R}}^{d})right) (d=2, 3, 4))。
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引用次数: 0
Stability estimates for semigroups in the Banach case 巴拿赫半群的稳定性估计
IF 1.4 3区 数学 Q1 MATHEMATICS Pub Date : 2024-03-15 DOI: 10.1007/s00028-024-00958-7

Abstract

The purpose of this paper is to revisit previous works of the author with Helffer and Sjöstrand (arXiv:1001.4171v1. 2010; Int Equ Op Theory 93(3):36, 2021) on the stability of semigroups which were proved in the Hilbert case by considering the Banach case at the light of a paper by Latushkin and Yurov (Discrete Contin Dyn Syst 33:5203–5216, 2013).

摘要 本文的目的是重温作者与 Helffer 和 Sjöstrand (arXiv:1001.4171v1. 2010; Int Equ Op Theory 93(3:36, 2021) 以前关于半群稳定性的工作。2010;Int Equ Op Theory 93(3):36, 2021)关于半群稳定性的研究,这些研究是根据拉图什金和尤罗夫的论文(Discrete Contin Dyn Syst 33:5203-5216, 2013),通过考虑巴纳赫情况,在希尔伯特情况下证明的。
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引用次数: 0
A critical exponent in a quasilinear Keller–Segel system with arbitrarily fast decaying diffusivities accounting for volume-filling effects 具有任意快速衰减扩散量的准线性凯勒-西格尔系统中的临界指数,考虑到体积填充效应
IF 1.4 3区 数学 Q1 MATHEMATICS Pub Date : 2024-03-15 DOI: 10.1007/s00028-024-00954-x
Christian Stinner, Michael Winkler

The quasilinear Keller–Segel system

$$begin{aligned} left{ begin{array}{l} u_t=nabla cdot (D(u)nabla u) - nabla cdot (S(u)nabla v), v_t=Delta v-v+u, end{array}right. end{aligned}$$

endowed with homogeneous Neumann boundary conditions is considered in a bounded domain (Omega subset {mathbb {R}}^n), (n ge 3), with smooth boundary for sufficiently regular functions D and S satisfying (D>0) on ([0,infty )), (S>0) on ((0,infty )) and (S(0)=0). On the one hand, it is shown that if (frac{S}{D}) satisfies the subcritical growth condition

$$begin{aligned} frac{S(s)}{D(s)} le C s^alpha qquad text{ for } text{ all } sge 1 qquad text{ with } text{ some } alpha < frac{2}{n} end{aligned}$$

and (C>0), then for any sufficiently regular initial data there exists a global weak energy solution such that ({ mathrm{{ess}}} sup _{t>0} Vert u(t) Vert _{L^p(Omega )}<infty ) for some (p > frac{2n}{n+2}). On the other hand, if (frac{S}{D}) satisfies the supercritical growth condition

$$begin{aligned} frac{S(s)}{D(s)} ge c s^alpha qquad text{ for } text{ all } sge 1 qquad text{ with } text{ some } alpha > frac{2}{n} end{aligned}$$

and (c>0), then the nonexistence of a global weak energy solution having the boundedness property stated above is shown for some initial data in the radial setting. This establishes some criticality of the value (alpha = frac{2}{n}) for (n ge 3), without any additional assumption on the behavior of D(s) as (s rightarrow infty ), in particular without requiring any algebraic lower bound for D. When applied to the Keller–Segel system with volume-filling effect for probability distribution functions of the type (Q(s) = exp (-s^beta )), (s ge 0), for global solvability the exponent (beta = frac{n-2}{n}) is seen to be critical.

准线性凯勒-西格尔系统 $$begin{aligned}u_t=nabla cdot (D(u)nabla u) -nabla cdot (S(u)nabla v), v_t=Delta v-v+u, end{array}right.end{aligned}$$endowed with homogeneous Neumann boundary conditions is considered in a bounded domain (Omega subset {mathbb {R}}^n), (n ge 3), with smooth boundary for sufficiently regular functions D and S satisfying (D>;0) on ([0,infty )),(S>0) on ((0,infty )) and(S(0)=0).一方面,可以证明如果(frac{S}{D})满足次临界增长条件$$begin{aligned}.frac{S(s)}{D(s)} le C s^alpha qquad text{ for }sge 1 *qquad *text{ with }(text{ some }#alpha < #frac{2}{n}end{aligned}$$和 (C>0),那么对于任何足够规则的初始数据,存在一个全局弱能量解,使得 ({ mathrm{{ess}}sup _{t>0}Vert u(t) Vert _{L^p(Omega )}<infty ) for some (p > frac{2n}{n+2}).另一方面,如果 (frac{S}{D})满足超临界增长条件 $$begin{aligned}frac{S(s)}{D(s)} ge c s^alpha qquad text{ for }1 *qquad *text{ with }(text{ some }alpha > frac{2}{n}end{aligned}$$和 (c>0),那么对于径向设置中的一些初始数据来说,具有上述有界性的全局弱能解不存在。这为 (n ge 3) 的值(α= frac{2}{n}) 确定了一些临界性,而不需要对 D(s) 作为 (s rightarrow infty ) 的行为做任何额外的假设,特别是不需要 D 的任何代数下限。当应用于具有体积填充效应的凯勒-西格尔系统时,对于类型为 (Q(s) = exp (-s^beta )), (s ge 0) 的概率分布函数来说,对于全局可解性来说,指数 (beta = frac{n-2}{n}) 是至关重要的。
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引用次数: 0
Nonlinear partial differential equations on noncommutative Euclidean spaces 非交换欧几里得空间上的非线性偏微分方程
IF 1.4 3区 数学 Q1 MATHEMATICS Pub Date : 2024-02-26 DOI: 10.1007/s00028-023-00928-5

Abstract

Noncommutative Euclidean spaces—otherwise known as Moyal spaces or quantum Euclidean spaces—are a standard example of a non-compact noncommutative geometry. Recent progress in the harmonic analysis of these spaces gives us the opportunity to highlight some of their peculiar features. For example, the theory of nonlinear partial differential equations has unexpected properties in this noncommutative setting. We develop elementary aspects of paradifferential calculus for noncommutative Euclidean spaces and give some applications to nonlinear evolution equations. We demonstrate how the analysis of some equations radically simplifies in the strictly noncommutative setting.

摘要 非交换欧几里得空间--又称莫亚尔空间或量子欧几里得空间--是非紧凑非交换几何的一个标准例子。对这些空间进行调和分析的最新进展使我们有机会强调它们的一些特殊性。例如,非线性偏微分方程理论在这种非交换环境中具有意想不到的特性。我们发展了非交换欧几里得空间的范差分微积分的基本方面,并给出了非线性演化方程的一些应用。我们展示了某些方程的分析是如何在严格的非交换环境中从根本上简化的。
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引用次数: 0
Well-posedness and longtime dynamics for the finitely degenerate parabolic and pseudo-parabolic equations 有限退化抛物和伪抛物方程的好求和长时间动力学
IF 1.4 3区 数学 Q1 MATHEMATICS Pub Date : 2024-02-26 DOI: 10.1007/s00028-024-00945-y
Gongwei Liu, Shuying Tian

We consider the initial-boundary value problem for degenerate parabolic and pseudo-parabolic equations associated with Hörmander-type operator. Under the subcritical growth restrictions on the nonlinearity f(u), which are determined by the generalized Métivier index, we establish the global existence of solutions and the corresponding attractors. Finally, we show the upper semicontinuity of the attractors in the topology of (H_{X,0}^1(Omega )).

我们考虑了与赫曼德型算子相关的退化抛物和伪抛物方程的初始边界值问题。在由广义梅蒂维尔指数决定的非线性 f(u) 的次临界增长限制下,我们确定了解的全局存在性和相应的吸引子。最后,我们证明了吸引子在(H_{X,0}^1(Omega ))拓扑中的上半连续性。
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引用次数: 0
Homogeneous Sobolev global-in-time maximal regularity and related trace estimates 同质索波列夫全局-时间最大正则性及相关痕量估计
IF 1.4 3区 数学 Q1 MATHEMATICS Pub Date : 2024-02-12 DOI: 10.1007/s00028-024-00946-x
Anatole Gaudin

In this paper, we prove global-in-time (dot{textrm{H}}^{alpha ,q})-maximal regularity for a class of injective, but not invertible, sectorial operators on a UMD Banach space X, provided (qin (1,+infty )), (alpha in (-1+1/q,1/q)). We also prove the corresponding trace estimate, so that the solution to the canonical abstract Cauchy problem is continuous with values in a not necessarily complete trace space. In order to put our result in perspective, we also provide a short review on (textrm{L}^q)-maximal regularity which includes some recent advances such as the revisited homogeneous operator and interpolation theory by Danchin, Hieber, Mucha and Tolksdorf. This theory will be used to build the appropriate trace space, from which we want to choose the initial data, and the solution of our abstract Cauchy problem to fall in.

在本文中,我们证明了在UMD巴纳赫空间X上一类可注入但不可反转的扇形算子的全局-时间-最大正则性,条件是(qin (1,+infty )),(alpha in(-1+1/q,1/q))。我们还证明了相应的迹估计,因此,典型抽象考奇问题的解是连续的,其值在不一定完整的迹空间中。为了使我们的结果更有说服力,我们还对(textrm{L}^q)-最大正则性做了简短回顾,其中包括一些最新进展,如丹钦、希伯、穆查和托克斯多夫重新审视的同质算子和插值理论。我们将利用这一理论来建立适当的迹空间,并从中选择初始数据和抽象考奇问题的解。
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引用次数: 0
期刊
Journal of Evolution Equations
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