非自治Plate方程时间依赖强拉回吸引子的存在性

结合Plinio等人([Plinio D,Duane G S,Temarn R,Time-dependent attractor for the oscillon equation,Discrete Contin Dyn Syst,2011,29(1):141-167.])提出的时间依赖全局吸引子概念,运用压缩函数的方法,证明了带有时间依赖系数的非自治Plate方程时间依赖拉回吸引子在空间H~4(Ω)∩H~2_0(Ω)×H~2_0(Ω)中的存在性.     

三维光滑区域上Navier-Stokes方程的有限元方法

§1.引言设Ω是R~3中的有界区域,且属于C~2.v是正常数.已知:当f∈(L~2(Ω))~3.且||f||0充分小时,Navier—Stokes方程的解存在且唯一.另外,u∈(H~2(Ω)∩H_1~0(Ω))~3,P∈H~1(Ω)\R. 最近,Bernardi讨论三维多面体区域Ω上Stokes方程的有限元解法.有限元空间由分片多项式(关于u为分片特殊三次多项式,关于p为分片常数)构成,进行误差估计时.要求u∈(H~2(Ω)∩H_0~1(Ω))~3,P∈H~1(Ω)\R.当Ω为二维区域上的凸多角形时,Stokes     

三维Brinkman-Forchheimer方程强解的全局吸引子的存在性

研究了三维有界区域上Brinkman-Forchheimer方程■-γ△u+au+b|u|u+c|u|~βu+▽p=f强解的存在唯一性及强解的全局吸引子的存在性.首先证明了当5/2≤β≤4及初始值u_0∈H_0~1(Ω)时强解的存在唯一性.接着对强解进行了一系列一致估计,基于这些一致估计,借助半群理论证明了方程的强解分别在H_1~1(Ω)和H~2(Ω)空间中具有全局吸引子,并证明了H_0~1(Ω)中的全局吸引子实际上便是H~2(Ω)中的全局吸引子.     

边界层的奇性分析

设 λ∈[λ_0,∞)(0<λ_0<<1),H_1=H_0~2(Ω)∩H~3(Ω),H_2=H_0~1(Ω)∩H~3(Ω),H_3=H~3(Ω),k_1=1/4,k_2=1/12,k_3=1/36,J_6(λ)=integral d(x,Γ)≥a~λlog(1+a~(-β) |△▽(u_e-u)|~2dx,α(ε)=1/6×log_ε1/C(C>1).我们考虑问题(?)定理.若 u=f∈H_i,对问题(1),有如下三种情形成立:i)正规区域 当 λ_0≤λ≤1/6-α(ε)时,有J_6(λ)≤C‖f‖_(H~3(Ω))~2;ii)奇性增长区域当1/6-α(ε)<λ<1/6+k_i/6时,有J_6(λ)≤Cε~(-6λ+2k_i)‖f‖_(H~3(Ω))~2;iii)奇性稳定区域当 λ≥1/6+(k_i)/6时,有J_6(λ)≤Cε~(-1+k_i)‖f‖_(H~3(Ω))~2;其中 i=1,2,3,β≥(45)/(32),C 为同 ε 无关的常数(见图1).     

非自治FitzHugh-Nagumo系统拉回吸引子的H~2×H_0~1有界性

研究带奇异扰动非自治FitzHugh-Nagumo系统拉回吸引子的H~3×H_0~1有界性.为此,首先建立关于过程有界不变集的H~2×H_0~1有界性,从而得到原系统拉回吸引子的有界性结果.     

高维广义BBM方程组的初边值问题

本文应用先验估计和Galerkin方法证明了高维广义BBM方程组的初边值问题在L~∞(0,T;H~3(Ω)∩H_0~1(Ω)),(s≥2)中整体解的存在性和正则性,并得到了整体解在||·||_(H~3×L~∞)范数下的稳定性和光滑解的唯一性。     

带衰退记忆的经典反应扩散方程的全局吸引子

当非线性项满足任意阶多项式增长且外力项仅属于H~(-1)(Ω)时,研究了带衰退记忆的经典反应扩散方程的长时间动力学行为.应用抽象函数理论、半群理论以及新的估计技巧,在空间L~2(Ω)×L_μ~2(R~+;H_0~1(Ω))上证明了全局吸引子的存在性.该结果改进和推广了Chepyzhov等人(2006)及Zhong等人(2006)的相应结果.     

带衰退记忆的经典反应扩散方程的强全局吸引子

当任意阶多项式增长的非线性项为耗散,且外力项仅属于L~2(Ω)时,研究了带衰退记忆的经典反应扩散方程的解在强拓扑空间H_0~1(Ω)×L_μ~2(R~+;D(A))的长时间行为.应用抽象函数理论、半群理论以及新的估计技巧,在拓扑空间H_0~1(Ω)×L_μ~2(R~+;D(A))上,验证了强解半群的渐近紧性并且证明了强全局吸引子的存在性.     

非线性Sobolev-Galpern方程的有限维整体吸引子

本文研究非线性Sobolev-Galpern方程解的渐近性态．首先证明了该方程在H^2(Ω)∩H0^1(Ω)中整体弱吸引子的存在性，然后利用一个能量方程证明了整体弱吸引子实际上是整体强吸引子，建立了整体吸引子的有限维性．     

Finite Dimensional Behavior for Forced Nonlinear Sobolev-Galpern Equations

This paper deals with the asymptotic behavior of solutions for the nonlinear Sobolev-Galpernequations.We first show the existence of the global weak attractor in H~2(Ω)∩H_0~1(Ω) for the equations.Andthen by an energy equation we prove that the global weak attractor is actually the global strong attractor.Thefinite-dimensionality of the global attractor is also established.     

退化抛物型方程弱解的存在性

讨论初值为u_0,v_0∈L_+~4(Ω),w∈W~(1,p)(Ω)(p≥2)时退化抛物型方程弱解的存在性.首先利用截断的方法将原问题正则化,化为u_0,v_0∈L_+~∞(Ω)的退化问题,接着对正则化问题的解做估计(这里的估计与具体的截断无关),最后利用弱收敛性,通过取极限的方法证明了原问题解的存在性.     

Convergence to strong nonlinear diffusion waves for solutions to p-system with damping on quadrant

In this paper, we consider the so-called p-system with linear damping on quadrant. We show that for a certain class of given large initial data (v₀(x),u₀(x)), the corresponding initial-boundary value problem admits a unique global smooth solution (v(x,t),u(x,t)) and such a solution tends time-asymptotically, at the Lp (2?p?∞) optimal decay rates, to the corresponding nonlinear diffusion wave which satisfies (1.9) provided the corresponding prescribed initial error function (V₀(x),U₀(x)) lies in (H³(R⁺)∩L¹(R⁺))×(H²(R⁺)∩L¹(R⁺)).     

Heat Flow and Perimeter in \boldsymbol{{\mathbb{R}}^m}

Let Ω be an open set in Euclidean space ? ^m with finite perimeter ${\mathcal{P}}(\Omega),$ and with m-dimensional Lebesgue measure |Ω|. It was shown by M. Preunkert that if T(t) is the heat semigroup on L ²(? ^m ) then $H_{\Omega}(t):=\int_{\Omega}T(t)\textbf{1}_{\Omega}(x)dx=|\Omega|-\pi^{-1/2}{\mathcal{P}}(\Omega)t^{1/2}+o(t^{1/2}), \ t\downarrow 0$ . H _Ω(t) represents the amount of heat in Ω if Ω is at initial temperature 1 and if ? ^m ???Ω is at initial temperature 0. In this paper we will compare the quantitative behaviour of H _Ω(t) with the usual heat content Q _Ω(t) associated to the Dirichlet heat semigroup on Ω. We analyse the heat content for horn-shaped open sets of the form Ω(α, Σ)?=?{(x, x′)?∈?? ^m : x′?∈?(1?+?x)^???α Σ, x?>?0}, where α?>?0, and where Σ is an open set in ? ^m???1 with finite perimeter in ? ^m???1, which is star-shaped with respect to 0. For m?≥?3 we find that there are four regimes with very different behaviour depending on α, and a further two limiting cases where logarithmic corrections appear.     

Convergence to strong nonlinear diffusion waves for solutions to p-system with damping

In this paper we consider the so-called p-system with linear damping, and we will prove an optimal decay estimates without any smallness conditions on the initial error. More precisely, if we restrict the initial data (V₀,U₀) in the space H³(R⁺)∩L1,γ(R⁺)×H²(R⁺)∩L1,γ(R⁺), then we can derive faster decay estimates than those given in [P. Marcati, M. Mei, B. Rubino, Optimal convergence rates to diffusion waves for solutions of the hyperbolic conservation laws with damping, J. Math. Fluid Mech. 7 (2) (2005) 224-240; H. Zhao, Convergence to strong nonlinear diffusion waves for solutions of p-system with damping, J. Differential Equations 174 (1) (2001) 200-236] and [M. Jian, C. Zhu, Convergence to strong nonlinear diffusion waves for solutions to p-system with damping on quadrant, J. Differential Equations 246 (1) (2009) 50-77].     

Existence results for nonlinear parabolic equations via strong convergence of truncations

Summary  We prove existence results for the initial-boundary value problem for parabolic equations of the type

Bergman-Hartogs型域的全纯自同构群

我们考虑一类以有界对称域D为底的Bergman-Hartogs型域Ω={(wm(1),...,w(r),z)∈C1×···×Cmr×D:∥w(1)∥2p1+···+∥w(r)∥2prKD(z,z)-q},其中KD(z,z)是D上的Bergman核函数,r 1且为正整数,参数p1,...,pr1和q0为实数.我们给出它的全纯自同构群,并且证明当r=1时此自同构群为最大全纯自同构群;当r1时,若Ω的全纯自同构变换F将(0,z)∈{0}×D映到(0,z*)∈{0}×D,则F在我们给出的全纯自同构群中.     

Long-time behavior of reaction-diffusion equations with dynamical boundary condition

In this paper, we study the long-time behavior of the reaction-diffusion equation with dynamical boundary condition, where the nonlinear terms f and g satisfy the polynomial growth condition of arbitrary order. Some asymptotic regularity of the solution has been proved. As an application of the asymptotic regularity results, we can not only obtain the existence of a global attractor A in (H¹(Ω)∩L^p(Ω))×L^q(Γ) immediately, but also can show further that A attracts every L²(Ω)×L²(Γ)-bounded subset with (H¹(Ω)∩L^p+δ(Ω))×L^q+κ(Γ)-norm for any δ,κ∈[0,∞).     

On ideals in the bidual of the Fourier algebra and related algebras

Let G be a compact nonmetrizable topological group whose local weight b(G) has uncountable cofinality. Let H be an amenable locally compact group, A(G×H) the Fourier algebra of G×H, and UC₂(G×H) the space of uniformly continuous functionals in VN(G×H)=A^∗(G×H). We use weak factorization of operators in the group von Neumann algebra VN(G×H) to prove that there exist at least ²b(G)² left ideals of dimensions at least ²b(G)² in A(G×H)^∗∗ and in UC₂^∗(G×H). We show that every nontrivial right ideal in A(G×H)^∗∗ and in UC₂^∗(G×H) has dimension at least ²b(G)².     

Friedrichs extensions of Schrödinger operators with singular potentials

The Friedrichs extension for the generalized spiked harmonic oscillator given by the singular differential operator −d²/dx²+Bx²+Ax⁻²+λx^−α (B>0, A?0) in L₂(0,∞) is studied. We look at two different domains of definition for each of these differential operators in L₂(0,∞), namely C₀^∞(0,∞) and D(T_2,F)∩D(M_λ,α), where the latter is a subspace of the Sobolev space W_2,2(0,∞). Adjoints of these differential operators on C₀^∞(0,∞) exist as result of the null-space properties of functionals. For the other domain, convolutions and Jensen and Minkowski integral inequalities, density of C₀^∞(0,∞) in D(T_2,F)∩D(M_λ,α) in L₂(0,∞) lead to the other adjoints. Further density properties C₀^∞(0,∞) in D(T_2,F)∩D(M_λ,α) yield the Friedrichs extension of these differential operators with domains of definition D(T_2,F)∩D(M_λ,α).     

Model problem for the motion of a compressible, viscous flow with the no-slip boundary condition

We consider the Navier–Stokes equations for the motion of a compressible, viscous, pressureless fluid in the domain W = \mathbbR³₊{\Omega = \mathbb{R}^3_+} with the no-slip boundary conditions. We construct a global in time, regular weak solution, provided that initial density ρ ₀ is bounded and the magnitude of the initial velocity u ₀ is suitably restricted in the norm ||?{r₀(·)}u₀(·)||_L²(W) + ||?u₀(·)||_L²(W){\|\sqrt{\rho_0(\cdot)}{\bf u}_0(\cdot)\|_{L^2(\Omega)} + \|\nabla{\bf u}_0(\cdot)\|_{L^2(\Omega)}}.