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1.
In this paper, we study the existence and nonexistence of multiple positive solutions for the following problem involving Hardy–Sobolev–Maz'ya term:-Δu- λu/|y|2=|u|pt-1u/|y|t+ μf(x), x ∈Ω,where Ω is a bounded domain in RN(N ≥ 2), 0 ∈Ω, x =(y, z) ∈ Rk× RN-kand pt =N +2-2t N-2(0 ≤ t ≤2). For f(x) ∈ C1(Ω)\{0}, we show that there exists a constant μ* 0 such that the problem possessesat least two positive solutions if μ∈(0, μ*) and at least one positive solution if μ = μ*. Furthermore,there are no positive solutions if μ∈(μ*, +∞).  相似文献   

2.
Given a domain Ω ? R~n, let λ 0 be an eigenvalue of the elliptic operator L :=Σ!(i,j)~n =1?/?xi(a~(ij0 ?/?xj) on Ω for Dirichlet condition. For a function f ∈ L~2(Ω), it is known that the linear resonance equation Lu + λu = f in Ω with Dirichlet boundary condition is not always solvable.We give a new boundary condition P_λ(u|? Ω) = g, called to be pro jective Dirichlet condition, such that the linear resonance equation always admits a unique solution u being orthogonal to all of the eigenfunctions corresponding to λ which satisfies ||u||2,2 ≤ C(||f ||_2 +|| g||_(2,2)) under suitable regularity assumptions on ?Ω and L, where C is a constant depends only on n, Ω, and L. More a priori estimates,such as W~(2,p)-estimates and the C~(2,α)-estimates etc., are given also. This boundary condition can be viewed as a generalization of the Dirichlet condition to resonance equations and shows its advantage when applying to nonlinear resonance equations. In particular, this enables us to find the new indicatrices with vanishing mean(Cartan) torsion in Minkowski geometry. It is known that the geometry of indicatries is the foundation of Finsler geometry.  相似文献   

3.
任洁 《数学学报》2018,61(3):383-402
在非Lipschitz条件下得到随机微分方程同胚流的大偏差原理.作为应用,本文同时给出了随机Hamilton系统同胚流的大偏差原理.特别地,以下二阶非线性随机振荡方程同胚流的大偏差原理也同样成立:Z_t=C_0Z_t-Z_t~3+Θ(Z_t)W_t,(Z_0,Z_0)=(z,u)∈R~2,其中C_0为任意常数,Θ为一阶导数有界的二阶连续可微函数,W_t是一维Brown白噪声.  相似文献   

4.
黄强  王正 《数学学报》2018,61(2):309-316
设T_Ω是带粗糙核的Calderón-Zygmund奇异积分算子,I为任意真包含在单位圆周S~1上的闭圆弧.本文证明,若Ω支在I上并在I上单调,那么T_Ω是从Hardy空间H~1(R~2)到L~1(R~2)的有界算子当且仅当‖Ω‖_(LlogL(S~1))∞.  相似文献   

5.
In this article,we show the existence of infinitely many solutions for the fractional pLaplacian equations of Schr?dinger-Kirchhoff type equation ■ ,where(-△)_p~s is the fractional p-Laplacian operator,[u]_(s,p) is the Gagliardo p-seminorm,0 s 1 q p N/s,α∈(0,N),M and V are continuous and positive functions,and k(x) is a non-negative function in an appropriate Lebesgue space.Combining the concentration-compactness principle in fractional Sobolev space and Kajikiya's new version of the symmetric mountain pass lemma,we obtain the existence of infinitely many solutions which tend to zero for suitable positive parameters λ and β.  相似文献   

6.
陈志红  李东升 《数学学报》2019,62(3):381-390
本文研究了R~3中有界区域Ω上的电磁场方程组弱解的W~(1,p)估计.该方程组来自于磁场所满足的稳态麦克斯韦方程组.在假定系数矩阵的逆属于VMO空间的条件下,利用R~3中向量场的旋度和散度的性质,将该方程组转化为标量椭圆型方程组,从而根据椭圆型方程组的正则性理论,得到解的W~(1,p)估计,其中1

相似文献   


7.
假定T_σ是关于乘子σ的双线性Fourier乘子算子,其中σ满足如下Sobolev正则条件:对某个s∈(n,2n],有sup_(κ∈Z)‖σ_k‖W~s(R~(2m))∞.对于p_1,p_2,p∈(1,∞)且满足1/p=1/p_1+1/p_2和ω=(ω_1,ω_2)∈A_(p/t)(R~(2n)),建立了T_σ及其与函数b=(b_1,b_2)∈(BMO(R~n))~2生成的交换子T_(σ,b)由L~(p_1,λ)(ω_1)×L~(p_2,λ)(ω_2)到L~(p,λ)(v_w)的有界性;同时,在b_1,b_2∈CMO(R~n)(C_c~∞(R~n)在BMO拓扑下的闭包)的条件下,证明交换子T_(σ,b)是L~(p_1,λ)(ω_1)×L~(p_2,λ)(ω_2)到L~(p,λ)(v_w)的紧算子.为了得到主要结果,我们先后建立了几个双(次)线性极大函数在加多权Morrey空间上的有界性以及该空间中准紧集的判定.  相似文献   

8.
We study local properties of solutions and their asymptotic extinction behavior for the fourth-order semilinear parabolic equation of diffusion–absorption type where p < 1, so that the absorption term is not Lipschitz continuous at u = 0. The Cauchy problem with bounded compactly supported initial data possesses solutions with finite interfaces, and we describe their oscillatory, sign changing properties for     . For p ∈ (0, 1), we also study positive solutions of the free-boundary problem with zero contact angle and zero-flux conditions. Finally, we describe families { fk } of similarity extinction patterns   uS ( x , t ) = ( T − t )1/(1− p ) f ( y )  , where   y = x /( T − t )1/4  , that vanish in finite time, as   t → T ∈ (0, ∞)  . Similar local and asymptotic properties are indicated for the sixth-order equation with source   相似文献   

9.
In this paper, we study the nonperiodic first-order Hamiltonian system ù = J L(t)u +J H(t, u), where H ∈ C1(R × R2n). With some assumptions on L, the corresponding Hamiltonian operator has only discrete spectrum. By using the index theory for self-adjoint operator equation,we establish the existence of multiple homoclinic orbits for the asymptotically quadratic nonlinearty satisfying some twist conditions between infinity and origin.  相似文献   

10.
林海波  王宸雁 《数学学报》1936,63(5):443-464
令(X,d,μ)为满足所谓上倍双倍条件和几何双倍条件的度量测度空间.设Mβ,ρ,q为(X,d,μ)上的分数型Marcinkiewicz积分算子.在本文中,作者证明了若β ∈[0,∞),ρ ∈(0,∞),q ∈(1,∞)且Mβ,ρ,q在L2(μ)上有界,则Mβ,ρ,q是从加权Lebesgue空间Lp(w)到加权弱Lebesgue空间Lp,∞(w)上有界和从加权Morrey空间Lp,κ,η(ω)到加权弱Morrey空间WLp,κ,η(ω)上有界.  相似文献   

11.
Consider the nonlinear wave equation
utt − γ 2 uxx + f(u) = 0
with the initial conditions
u ( x ,0) = εφ ( x ), u t( x ,0) = εψ ( x ),
where f ( u ) is either of the form f ( u )= c 2 u −σ u 2 s +1, s =1, 2,…, or an odd smooth function with f '(0)>0 and | f '( u )|≤ C 02.The initial data φ( x )∈ C 2 and ψ( x )∈ C 1 are odd periodic functions that have the same period. We establish the global existence and uniqueness of the solution u ( x ,  t ; ɛ), and prove its boundedness in x ∈ R and t >0 for all sufficiently small ɛ>0. Furthermore, we show that the error between the solution u ( x ,  t ; ɛ) and the leading term approximation obtained by the multiple scale method is of the order ɛ3 uniformly for x ∈ R and 0≤ t ≤ T /ɛ2, as long as ɛ is sufficiently small, T being an arbitrary positive number.  相似文献   

12.
汪成咏  渠刚荣 《数学学报》2016,59(4):489-504
对于1r∞与巴拿哈空间B=L~r(Ω,F,μ),我们研究了欧几里得空间R~n上B-值缓分布构成的哈代-洛伦茨空间H~(p,q)(R~n,B)及哈代-洛伦茨空间之间的内插,其中0p∞和0q≤∞,获得了H~(p,q)(R~n,B)的一系列等价的刻画及其原子分解.若Ω={1},则H~(p,q)(R~n,B)=H~(p,q)(R~n)是经典的情形;若Ω=Z是整数集且μ是Z上的计数测度并且r=2,0p∞及q=∞,则H~(p,q)(R~n,B)=H~(p,∞)(R~n,e~2)转化为Grafakos和He在文[Weak Hardy spaces,Preprint,2014]中讨论的情形.  相似文献   

13.
首先,在并半格中引入了上覆盖关系的概念,并以此为基础引入强并半格以及强并半格中上覆盖和C-滤子的概念,证明了强并半格S中全体C-滤子之族C Fil(S)是余Frame,讨论了简单上集值映射u:S→C Fil(S)的相关并半格同态性质;其次,证明了由一族余Frame{A_λ|λ∈Γ}的直积Π_(λ∈Γ)A_λ中只有有限个坐标非零的元素构成的子集A是强并半格,还证明了A是余Frame族{A_λ|λ∈Γ}在并半格范畴中的余积对象;最后,通过各个坐标集中的上覆盖关系在A中定义了上覆盖C~*,再结合简单上集值映射u:A→C~*Fil(A)和标准入射qλ:Aλ→Π_(λ∈Γ)A_λ(λ∈Γ),证明了强并半格A中由上覆盖C~*诱导的余Frame C~*Fil(A)是余Frame族{A_λ|λ∈Γ}在余Frame范畴中的余积对象.  相似文献   

14.
Suppose A is a unital C*-algebra and r 1.In this paper,we define a unital C*-algebra C_(cb)*(A,r) and a completely bounded unital homomorphism α_r:A → C_(cb)*(A,r)with the property that C_(cb)*(A,r)=C*(α_r(A))and,for every unital C*-algebra B and every unital completely bounded homomorphism φ:A→ B,there is a(unique)unital *-homomorphism π:C_(cb)*(A,r)→B such thatφ=πoα_r.We prove that,if A is generated by a normal set {t_λ:λ∈Λ},then C_(cb)*(A,r)is generated by the set {α_r(t_λ):λ∈Λ}.By proving an equation of the norms of elements in a dense subset of C_(cb)*(A,r)we obtain that,if Β is a unital C*-algebra that can be embedded into A,then C_(cb)*(B,r)can be naturally embedded into C(cb)*(A,r).We give characterizations of C_(cb)*(A,r)for some special situations and we conclude that C_(cb)*(A,r)will be "nice" when dim(A)≤ 2 and "quite complicated" when dim(A)≥ 3.We give a characterization of the relation between K-groups of A and K-groups of C_(cb)*(A,r).We also define and study some analogous of C_(cb)*(A,r).  相似文献   

15.
Zygmund空间上的微分复合算子   总被引:2,自引:1,他引:1  
讨论Zygmund空间E={f∈H(D):sup_(z∈D)(l-|z|~2)|f″(z)|∞}上的微分复合算子DC_φ,这里C_φ是复合算子,D是微分算子.得到了DC_φ在Zygmund空间E和小Zygmund空间E_0上是有界算子与紧算子的充分必要条件.  相似文献   

16.
The Stokes and Krasovskii Conjectures for the Wave of Greatest Height   总被引:1,自引:0,他引:1  
The integral equation:
φμ(s) = (1/3 π)∫π 0((sin φμ(t))/(μ −1+ ∫t 0sin φμ(u) d u )) (log((sin½( s + t ))/ (sin½( s − t )))d t
was derived by Nekrasov to describe waves of permanent form on the surface of a nonviscous, irrotational, infinitely deep flow, the function φμ giving the angle that the wave surface makes with the horizontal. The wave of greatest height is the singular case μ=∞, and it is shown that there exists a solution φ to the equation in this case and that it can be obtained as the limit (in a specified sense) as μ→∞ of solutions for finite μ. Stokes conjectured that φ( s )→⅙π as s ↓0, so that the wave is sharply crested in the limit case; and Krasovskii conjectured that sup s ∈[0,π]φμ( s )≤⅙π for all finite μ. Stokes' conjecture was finally proved by Amick, Fraenkel, and Toland, and the present article shows Krasovskii's conjecture to be false for sufficiently large μ, the angle exceeding ⅙π in what is a boundary layer.  相似文献   

17.
给出C~*-代数α-比较性的等价刻画:对于单的含单位元的稳定有限的C~*-代数A而言,A具有α-比较性,当且仅当对于任意的a,b∈W(A),若α·d_r(a)d_τ(b)(_τ∈QT(A)),则a≤b在Cuntz半群W(A)中成立.利用此刻画,证明了具有α-比较性的C~*-代数一定具有弱比较性;若A具有α-比较性,其中α=m+1,则A具有正元的强迹m-比较性;对于满足Kirchberg-R?rdam条件的C~*-代数,E-稳定、严格比较、α-比较性(α=m+1)、强迹m-比较性、弱比较性以及局部弱比较性彼此等价;若α:=inf{α′∈(1,∞)|A具有α′-比较}∞,则A具有α-比较性.  相似文献   

18.
Through both analytical and numerical methods, we solve the eigenproblem uzz >+(1/ z −λ−( z −1/ε)2) u =0 on the unbounded interval z ∈[−∞, ∞], where λ is the eigenvalue and u ( z )→0 as | z |→∞. This models an equatorially trapped Rossby wave in a shear flow in the ocean or atmosphere. It is the usual parabolic cylinder equation with Hermite functions as the eigenfunctions except for the addition of an extra term, which is a simple pole. The pole, which is on the interior of the interval, is interpreted as the limit δ→0 of 1/( z − i δ). The eigenfunction has a branch point of the form z  log( z ) at z =0, where the branch cut is on the upper imaginary axis. The eigenvalue is complex valued with an imaginary part, which we show, through matched asymptotics, to be approximately √ π exp(−1/ε2){1−2ε log ε+ε log 2+γε}. Because T ( λ ) is transcendentally small in the small parameter ε, it lies "beyond all orders" in the usual Rayleigh–Schrödinger power series in ε. Nonetheless, we develop special numerical algorithms that are effective in computing T ( λ ) for ε as small as 1/100.  相似文献   

19.
We consider a singularly perturbed convection–diffusion equation,     , defined on two domains: a quarter plane,  ( x , y ) ∈ (0, ∞) × (0, ∞)  , and an infinite strip,  ( x , y ) ∈ (−∞, ∞) × (0, 1)  . We consider for both problems discontinuous Dirichlet boundary conditions:   u ( x , 0) = 0  and   u (0, y ) = 1  for the first one and   u ( x , 0) =χ[ a , b ]( x )  and   u ( x , 1) = 0  for the second. For each problem, asymptotic expansions of the solution are obtained from an integral representation in two limits: (a) when the singular parameter  ε→ 0+  (with fixed distance r to the discontinuity points of the boundary condition) and (b) when that distance   r → 0+  (with fixed ε). It is shown that in both problems, the first term of the expansion at  ε= 0  is an error function or a combination of error functions. This term characterizes the effect of the discontinuities on the ε-behavior of the solution and its derivatives in the boundary or internal layers. On the other hand, near the discontinuities of the boundary condition, the solution u ( x , y ) of both problems is approximated by a linear function of the polar angle at the discontinuity points.  相似文献   

20.
Let Gi be closed Lie groups of U (n), Ω i be bounded Gi-invariant domains in C^n which contains 0, and O(C^n)^Gi = C, for i = 1, 2. It is known that if f : Ω 1 → Ω 2 is a proper holomorphic mapping, and f^-1{0} = {0}, then f is a polynomial mapping. In this paper, we provide an upper bound for the degree of such a polynomial mapping using the multiplicity of f .  相似文献   

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