Processing math: 21%

数学物理学报, 2020, 40(2): 379-394 doi:

论文

自然增长条件下的非齐次A-调和方程弱解的梯度估计

张雅楠, 闫硕, 佟玉霞,

Gradient Estimates for Weak Solutions to Non-Homogeneous A-Harmonic Equations Under Natural Growth

Zhang Yanan, Yan Shuo, Tong Yuxia,

通讯作者: 佟玉霞, E-mail:tongyuxia@126.com

收稿日期: 2018-12-28  

基金资助: 河北省社会科学基金.  HB17YJ094

Received: 2018-12-28  

Fund supported: the Social Science Fund of Hebei Province.  HB17YJ094

摘要

该文主要研究一类自然增长条件下的非齐次A-调和方程弱解的梯度估计,首先获得自然增长条件下的非齐次A-调和方程弱解的Lp估计,然后使用迭代覆盖逼近等方法,将其推广到Orlicz空间.

关键词: A-调和方程 ; 弱解 ; 梯度估计

Abstract

The gradient estimates for weak solutions to non-homogeneous A-harmonic equations under natural growth is obtained. The Lp-type estimates for such equation is derived under natural growth, and then the Lφ-type estimate in Orlicz space is derived by a new iteration-covering approach.

Keywords: A-Harmonic equation ; Weak solution ; Gradient estimate

PDF (397KB) 元数据 多维度评价 相关文章 导出 EndNote| Ris| Bibtex  收藏本文

本文引用格式

张雅楠, 闫硕, 佟玉霞. 自然增长条件下的非齐次A-调和方程弱解的梯度估计. 数学物理学报[J], 2020, 40(2): 379-394 doi:

Zhang Yanan, Yan Shuo, Tong Yuxia. Gradient Estimates for Weak Solutions to Non-Homogeneous A-Harmonic Equations Under Natural Growth. Acta Mathematica Scientia[J], 2020, 40(2): 379-394 doi:

1 引言

1<p<+, ΩRn中的有界域,本文考虑如下非齐次椭圆方程

divA(x,u)=B(x,u),
(1.1)

其中算子A=A(x,ξ):Rn×RnRn,满足通常的可测性条件(Carathéodory条件),并且对几乎所有的x,yΩ和所有的ξ,ηRn满足下列条件

A(x,0)=0;
(1.2)

|A(x,ξ)|C1|ξ|p1;
(1.3)

A(x,ξ)A(x,η),ξηC2|ξη|p;
(1.4)

|A(x,ξ)A(y,ξ)|C3ω(|xy|)|ξ|p1;
(1.5)

算子B=B(x,ξ):Rn×RnR满足自然增长条件

|B(x,ξ)|C4|ξ|p;
(1.6)

其中Ci>0,i=1,2,3,4为正常数.这里的连续模ω(x):R+R+非减,而且满足

ω(r)0r0.
(1.7)

考虑自然增长条件下的非齐次A -调和方程(1.1)的弱解,给出如下定义.

定义1.1   设算子A,B满足条件(1.2)–(1.6)式,称uW1,ploc(Ω)L(Ω)是方程(1.1)的局部弱解,若

ΩA(x,u),φdx=ΩB(x,u)φdx,
(1.8)

对于任意的φW1,p0(Ω)都成立.

Dibenedetto等[1]和Iwaniec[2]获得了Lq空间(qp)p-Laplace型拟线性椭圆方程

div(|Du|p2Du)=div(|F|p2F)

弱解的梯度估计; Acerbi和Mingione[3]研究了上述方程在变指数空间中的情况;之后Byun, Kinnunen等[4-5]在不同假设条件下,获得了p-Laplace型拟线性椭圆方程

div((ADuDu)(p2)/2ADu)=div(|F|p2F)

弱解的梯度估计; Byun和Wang[7]获得了非线性椭圆方程

diva(u,x)=divf

的弱解的W1,p (2p<)正则性; Jia等[8]基于标准的W2,p估计方法及Hardy-Littlewood极大函数,建立了泊松方程

Δu=f

在Orlicz空间中的正则性理论; Yao[7]研究了一类非线性椭圆方程

divA(u,x)=div(|f|p2f),

通过假设算子A满足一些合适条件和向量f满足适当增长条件,得到了其在Orlicz空间弱解的梯度估计;后来又获得了抛物型A -调和方程

utdivA(u,x,t)=div(|f|p2f)

的弱解在Sobolev空间和Orlicz空间的梯度估计[9];最近李慧珍和郑神州[10]研究了具有小的部分BMO系数的非散度型线性椭圆方程

aij(x)Diju=f(x),a.e.xΩ

强解的Hesssian矩阵在Orlicz空间的内部估计; Liang和Zheng[11]得到了具有部分BMO系数的非线性椭圆型障碍问题在Orlicz空间中的梯度估计.

Zheng等[12]2008年获得了右端为非散度型的自然增长条件下椭圆方程弱解的Lp估计,其研究成果中关于自然增长条件下的处理方法,对本文研究的A -调和方程的Lp估计具有很强的参考价值.另外,由于经典的Lϕ空间中的极大函数比较繁琐,本文采用了文献[8]中的迭代覆盖逼近方法,将Lp估计推广到Orlicz空间,避免了使用极大函数算子.

另外,关于A -调和方程及其相关问题的结论,可参见文献[13-16].

本文首先得到自然增长条件下非齐次A -调和方程(1.1)Lp估计,再将其扩展到Orlicz空间.

下面是本文主要结论.

定理1.1  假设ϕ22,如果uW1,ploc(Ω)L(Ω)是方程(1.1)的局部弱解,算子AB满足(1.2)–(1.6)式,那么

|u|pLϕloc(Ω),
(1.9)

且有估计式

BRϕ(|u|p)dxC{ϕ(B2R|uu2R|pdx)+1},
(1.10)

其中B2RΩ,且C是独立于u的常数.

本文具体内容组织如下:在第二节给出预备知识和迭代覆盖方法;在第三节给出主要结论的证明.

2 预备知识

Orlicz空间是Lp空间的推广,自1932年波兰著名数学大师Orlicz引进以来, Orlicz空间理论已应用于诸多领域.下面简单介绍Orlicz空间中的基本定义和一些相关的重要结论.

Φ表示所有函数ϕ:[0,+)[0,+)组成的函数类,其中ϕ是递增的凸函数.

定义2.1[7-8, 17]  如果存在一个正常数K,使得对于任意的t>0,都有

ϕ(2t)Kϕ(t);
(2.1)

那么,函数ϕΦ满足全局2条件,表示为ϕ2.同时,如果存在一个常数a>1,使得对于任意的t>0,都有

ϕ(t)ϕ(at)2a;
(2.2)

那么,函数ϕΦ满足全局2条件,表示为ϕ2.

注2.1   (1)注意到全局22条件使函数适当增长.例如, ϕ(t)=|t|α(1+|log|t||)22,α>1.tlog(1+t)这样的例子不满足2条件,而像exp(t2)这样的例子不满足2条件.

(2)事实上,如果ϕ22,那么ϕ满足对于0<θ21θ1<,都有

ϕ(θ1t)Kθα11ϕ(t),ϕ(θ2t)2aθα22ϕ(t),
(2.3)

其中α1=log2K,α2=loga2+1.

(3)在条件(2.3)式下,很容易得到ϕΦ,且满足ϕ(0)=0以及

lim
(2.4)

定义2.2[7-8, 17]    令 \phi \in \Phi ,则 \rm Orlicz K^{\phi }(\Omega ) 是满足

\begin{equation} \int _{\Omega }\phi (\left | g \right |){\rm d}x< \infty \end{equation}
(2.5)

的所有可测函数 g:\Omega \rightarrow {{\Bbb R}} 组成的集合.

Orlicz空间 L^{\phi }(\Omega ) K^{\phi }(\Omega ) 的线性闭包.

注2.2  注意到, \rm Orlicz 空间 L^{\phi }(\Omega ) L^{q } 空间的推广形式.如果 \phi (t) = t^{q}, t\geq 0 ,那么 \phi \in \triangle _{2}\cap \triangledown _{2} ,于是得到一个特例

\begin{equation} L^{\phi }(\Omega ) = L^{q}(\Omega ). \end{equation}
(2.6)

关于Orlicz空间有如下重要引理.

引理2.1[7, 18-19]   假设 \phi \in\triangle _{2}\cap \triangledown _{2} 以及 g \in L^{\phi }(\Omega ) ,那么

(1) K^{\phi } = L^{\phi } ,且 C_{0}^{\infty } L^{\phi } 中稠密;

(2) L^{\alpha _{1}}(\Omega )\subset L^{\phi }(\Omega )\subset L^{\alpha _{2}} (\Omega )\subset L^{1}(\Omega ) ,其中 \alpha _{1}, \alpha _{2} 取自(2.3)式;

(3)

\begin{equation} \int _{\Omega }\phi (\left | g \right |){\rm d}x = \int_{0}^{\infty }\left | \left \{ x \in \Omega :\left | g \right |> \lambda \right \} \right |{\rm d}\left [ \phi (\lambda ) \right ]; \end{equation}
(2.7)

(4)

\begin{equation} \int_{0}^{\infty }\frac{1}{\mu }\int _{\left \{ x \in \Omega :\left | g \right | > a\mu \right \}}\left | g \right |{\rm d}x{\rm d}\left [ \phi (b\mu ) \right ]\leq C\int _{\Omega }\phi (\left | g \right |){\rm d}x, \end{equation}
(2.8)

其中 a, b>0, C = C(a, b, \phi ) .

u 为方程 (1.1) 的局部弱解.先考虑定理1.1中在 R = 1 的情况,然后可通过缩放论证得到(1.10)式.设

\begin{equation} \lambda _{0} = : \left [-\!\!\!\!\!\!\int_{B_{1}} \left | \nabla u \right |^{p}{\rm d}x\right ]^{\frac{1}{p}}; \end{equation}
(2.9)

对于任意的 x \in \Omega \rho > 0 ,令

\begin{equation} J\left [ B_{\rho } (x)\right ] = : -\!\!\!\!\!\!\int _{B_{\rho } (x)}\left | \nabla u \right |^{p}{\rm d}y. \end{equation}
(2.10)

\begin{equation} E(1) = :\left \{ x \in B_{1}:\left | \nabla u \right | ^{p}> \lambda ^{p}\right \}. \end{equation}
(2.11)

由(7)式,选择合适的常数 R_{0} = R_{0}(\epsilon ) \in (0, 1) 使得

\begin{equation} \omega (R_{0})\leq \epsilon . \end{equation}
(2.12)

不妨限定 \epsilon \in (0, 1) ,且由(3.48)式决定.

下面借鉴文献[8],给出迭代覆盖逼近引理.

引理2.2  令 \lambda \geq \lambda _{*} = :(\frac{10}{R_{0}})^{n/p}\lambda _{0}+1 ,则存在一族不相交的球 \left \{ B_{\rho _{i}}(x_{i}) \right \} , x_{i} \in E(1) ,使得 0< \rho _{i} = \rho (x_{i})\leq R_{0}/10 ,且

\begin{equation} J\left [ B_{\rho _{i}} (x_{i})\right ] = \lambda ^{p}, J\left [ B_{\rho } (x_{i})\right ] < \lambda ^{p} \; \mbox{对任意} \; \rho > \rho _{i} \;\mbox{成立}. \end{equation}
(2.13)

而且,有

\begin{equation} E(1)\subset \bigcup\limits_{i \in {\Bbb N}}B_{5\rho _{i}}(x_{i})\cup \mbox{可略集}; \end{equation}
(2.14)

\begin{equation} \left | B_{\rho _{i}} (x_{i})\right |\leq \frac{2}{\lambda ^{p}} \int _{\left \{ x\in B_{\rho _{i}}(x_{i}):\left | \nabla u \right | ^{p}> \frac{\lambda ^{p}}{2}\right \}}\left | \nabla u \right |^{p}{\rm d}x. \end{equation}
(2.15)

   (1) 首先需证

\begin{equation} \sup _{\omega \in B_{1}} \sup _{\frac{R_{0}}{10}\leq \rho \leq R_{0}}J\left [ B_{\rho }(\omega ) \right ]\leq \lambda ^{p}. \end{equation}
(2.16)

为证明上式,给定任意的 \omega \in B_{1} \frac{R_{0}}{10}\leq \rho \leq R_{0} ,令 \lambda \geq \lambda _{*} = :(\frac{10}{R_{0}})^{n/p}\lambda _{0}+1 ,则有

\begin{eqnarray} J\left [ B_{\rho }(\omega ) \right ] = -\!\!\!\!\!\!\int _{B_{\rho }(\omega)}\left |\nabla u \right |^{p}{\rm d}x &\leq& \frac{\left | B_{1} \right |}{\left | B_{\rho }(\omega ) \right |}-\!\!\!\!\!\!\int _{B_{1}}\left | \nabla u \right |^{p}{\rm d}x \\ &\leq& (\frac{10}{R_{0}})^{n}-\!\!\!\!\!\!\int _{B_{1}}\left | \nabla u \right |^{p}{\rm d}x \\ &\leq& (\frac{10}{R_{0}})^{n}\lambda _{0}^{p}+1 \\ &\leq& \lambda ^{p }. \end{eqnarray}
(2.17)

即对任意的 \omega \in B_{1} R_{0}/10\leq \rho \leq R_{0} , (2.16)式成立.

(2) 对几乎处处 \omega \in E(1) ,由Lebesgue微分定理得

\begin{equation} \lim _{\rho \rightarrow 0}J\left [ B_{\rho }(\omega ) \right ]> \lambda ^{p}, \end{equation}
(2.18)

则存在 \rho > 0 ,满足

\begin{equation} J\left [ B_{\rho }(\omega ) \right ]> \lambda ^{p}; \end{equation}
(2.19)

由(2.16)式,选择半径 \rho _{\omega } \in (0, \frac{R_{0}}{10}] 使得

\begin{equation} \rho _{\omega } = :\max \left \{ \rho |J\left [ B_{\rho } (\omega )\right ] = \lambda ^{p} , 0< \rho \leq \frac{R_{0}}{10}\right \}. \end{equation}
(2.20)

由于 J\left [ B_{\rho } (\omega )\right ] 是关于 \rho 的连续函数,则

\begin{equation} J\left [ B_{\rho_{\omega } } (\omega )\right ] = \lambda ^{p}, \end{equation}
(2.21)

于是,对 \rho _{\omega }< \rho \leq R_{0}

\begin{equation} J\left [ B_{\rho } (\omega )\right ]<\lambda ^{p}. \end{equation}
(2.22)

对于几乎处处 \omega \in E(1) ,存在一个球 B_{\rho _{\omega }}(\omega ) 满足上述论证.因此,应用Vitali覆盖引理,有一族互不相交的球 \left \{ B_{\rho _{i }}(x_{i}) \right \}_{i \in {\Bbb N}} ,其中 x_{i} \in E(1), \rho _{i} = \rho (x_{i})\in (0, R_{0}/10] ,使得(2.13)式和(2.14)式成立.

(3) 由(2.13)式有

\begin{equation} J\left [ B_{\rho _{i}}(x_{i}) \right ] = -\!\!\!\!\!\!\int _{B_{\rho _{i}}(x_{i})}\left | \nabla u \right |^{p}{\rm d}x = \lambda ^{p}, \end{equation}
(2.23)

\begin{equation} \lambda ^{p}\left | B_{\rho _{i}}(x_{i})\right | = \int _{B_{\rho _{i}}(x_{i})}\left | \nabla u \right |^{p}{\rm d}x. \end{equation}
(2.24)

于是将(2.24)式进行积分区域分割,得

\begin{equation} \lambda ^{p}\left | B_{\rho _{i}}(x_{i})\right |\leq \int _{\left \{ x \in B_{\rho _{i}}(x_{i}):\left | \nabla u \right |^{p} > \frac{\lambda ^{p}}{2}\right \}}\left | \nabla u \right |^{p}{\rm d}x+\frac{\lambda ^{p}}{2}\left | B_{\rho _{i}}(x_{i})\right |, \end{equation}
(2.25)

移项整理得

\begin{equation} \left | B_{\rho _{i}}(x_{i})\right |\leq \frac{2}{\lambda ^{p}}\int _{\left \{ x \in B_{\rho _{i}}(x_{i}):\left | \nabla u \right |^{p} > \frac{\lambda ^{p}}{2}\right \}}\left | \nabla u \right |^{p}{\rm d}x. \end{equation}
(2.26)

引理2.2证毕.

下面的引理来自文献[20-21].

引理2.3  设 f (\tau ) 是定义在 0\leq R_{0}\leq t\leq R_{1} 上的非负有界函数,若对 R_{0}\leq \tau < t\leq R_{1}

\begin{equation} f(\tau )\leq A(t-\tau )^{-\alpha }+B+\theta f(t), \end{equation}
(2.27)

这里 A, B, \alpha, \theta 为非负常数且 \theta < 1 ,则存在只依赖于 \alpha \theta 的常数 C ,使得对于每个 \rho , R, R_{0}\leq \rho < R\leq R_{1} ,有

\begin{equation} f(\rho )\leq C\left [ A(R-\rho )^{-\alpha } +B \right ]. \end{equation}
(2.28)

3 主要定理的证明

本节内容组织如下:在3.1小节,通过添加假设条件 \left | \nabla u \right |^{p} \in L_{loc}^{\infty }(\Omega ) \subset L_{loc}^{\phi}(\Omega) 给出定理 1.1 的证明;在3.2小节,利用逼近方法将上述添加的假设条件移除.

3.1 假设条件下定理1.1的证明

本小节在假设 \left | \nabla u \right |^{p} \in L_{loc}^{\infty }(\Omega )\subset L_{loc}^{\phi}(\Omega) 的条件下,考虑定理 1.1 的证明.首先建立自然增长条件下方程 (1.1) 的局部 L^{p} 估计.

引理3.1   假设 B_{2R}\subset \Omega ,令 u \in W_{loc}^{1, p}(\Omega) \cap L^{\infty }(\Omega ) 为方程 (1.1) 的局部弱解,算子 A B 满足(1.2)–(1.6)式,则

\begin{equation} \int _{B_{R}}\left | \nabla u \right |^{p}{\rm d}x\leq \frac{C}{R^{p}} \int _{B_{2R}}\left | u-u_{2R} \right |^{p}{\rm d}x. \end{equation}
(3.1)

  选取适当的检验函数 \varphi = (u-u_{2R})e^{\beta \left |u-u_{2R} \right |}\eta ^{p} ,其中 \beta 为待定常数, u_{2R} = \frac{1}{|B_{2R}|}\int _{B_{2R}}u{\rm d}x , \eta \in C_{0}^{\infty }(\Omega) 为截断函数,满足

\begin{equation} 0\leq \eta \leq 1, \eta \equiv 1 \; in \;B_{R}, \eta \equiv 0 \; in \;\Omega \setminus B_{2R}, \left | \nabla \eta \right | \leq \frac{C}{R}. \end{equation}
(3.2)

将检验函数代入定义1.1,得

\begin{equation} \int _{\Omega }\left \langle A(x, \nabla u), \nabla \varphi \right \rangle {\rm d}x = \int _{\Omega }B(x, \nabla u)\varphi {\rm d}x, \end{equation}
(3.3)

并移项整理得

\begin{eqnarray} &&\int _{\Omega }\left \langle A(x, \nabla u), e^{\beta \left | u-u_{2R} \right |}\eta ^{p} \nabla u +\beta \eta ^{p}\left | u-u_{2R} \right | e^{\beta \left | u-u_{2R} \right |} \nabla u \right \rangle {\rm d}x \\ & = & -p\int _{\Omega }\left \langle A(x, \nabla u), \eta ^{p-1} ( u-u_{2R} ) e^{\beta \left | u-u_{2R} \right |} \nabla \eta \right \rangle {\rm d}x +\int _{\Omega }B(x, \nabla u)\varphi {\rm d}x. \end{eqnarray}
(3.4)

上述等式左边利用(1.2)及(1.4)式得

\begin{eqnarray} &&\int _{\Omega }\left \langle A(x, \nabla u), e^{\beta \left | u-u_{2R} \right |}\eta ^{p} \nabla u +\beta \eta ^{p}\left | u-u_{2R} \right | e^{\beta \left | u-u_{2R} \right |} \nabla u \right \rangle {\rm d}x \\ &\geq & C_{2}\int _{\Omega }e^{\beta \left | u-u_{2R} \right |}\left | \eta \nabla u \right |^{p}{\rm d}x +C_{2}\beta \int _{\Omega }\left | \eta \nabla u \right |^{p} \left | u-u_{2R} \right |e^{\beta \left | u-u_{2R} \right |}{\rm d}x. \end{eqnarray}
(3.5)

将(3.4)式右边利用(1.3)式和(1.6)式得

\begin{eqnarray} &&-p\int _{\Omega }\left \langle A(x, \nabla u), \eta ^{p-1} ( u-u_{2R} ) e^{\beta \left | u-u_{2R} \right |} \nabla \eta \right \rangle {\rm d}x +\int _{\Omega }B(x, \nabla u)\varphi {\rm d}x \\ &\leq & pC_{1}\int _{\Omega }\left | \eta \nabla u \right | ^{p-1}\left | \nabla \eta \right |\left | u-u_{2R} \right |e^{\beta \left | u-u_{2R} \right |} {\rm d}x+ C_{4}\int _{\Omega }\left | \eta \nabla u \right |^{p}\left | u-u_{2R} \right |e^{\beta \left | u-u_{2R} \right |} {\rm d}x \\ & = & I_{1}+I_{2}. \end{eqnarray}
(3.6)

估计 I_{1} .由Young不等式得

\begin{eqnarray} I_{1} \leq pC_{1}\tau \int _{\Omega }e^{\beta \left | u-u_{2R} \right |}\left | \eta \nabla u \right |^{p}{\rm d}x +pC_{1}C(\tau )\int _{\Omega }e^{\beta \left | u-u_{2R} \right |} \left | (u-u_{2R}) \nabla \eta \right |^{p}{\rm d}x. \end{eqnarray}
(3.7)

综合(3.4), (3.5), (3.6)及(3.7)式,得

\begin{eqnarray} && C_{2}\int _{\Omega }e^{\beta \left | u-u_{2R} \right |}\left | \eta \nabla u \right |^{p}{\rm d}x +C_{2}\beta \int _{\Omega }\left | \eta \nabla u \right |^{p} \left | u-u_{2R} \right |e^{\beta \left | u-u_{2R} \right |}{\rm d}x \\ &\leq & pC_{1}\tau \int _{\Omega }e^{\beta \left | u-u_{2R} \right |}\left | \eta \nabla u \right |^{p}{\rm d}x +pC_{1}C(\tau)\int _{\Omega }e^{\beta \left | u-u_{2R} \right |} \left | (u-u_{2R}) \nabla \eta \right |^{p}{\rm d}x \\ & & +C_{4}\int _{\Omega }\left | \eta \nabla u \right |^{p}\left | u-u_{2R} \right |e^{\beta \left | u-u_{2R} \right |} {\rm d}x. \end{eqnarray}
(3.8)

\beta 满足 C_{2} \beta > C_{4} ,将上式移项整理得

\begin{eqnarray} && C_{2}\int _{\Omega }e^{\beta \left | u-u_{2R} \right |}\left | \eta \nabla u \right |^{p}{\rm d}x \\ &\leq & pC_{1}\tau \int _{\Omega }e^{\beta \left | u-u_{2R} \right |}\left | \eta \nabla u \right |^{p}{\rm d}x +pC_{1}C(\tau )\int _{\Omega }e^{\beta \left | u-u_{2R} \right |} \left | (u-u_{2R}) \nabla \eta \right |^{p}{\rm d}x. \end{eqnarray}
(3.9)

\tau >0 且满足 C_{2} - p C_{1}\tau > 0 .上式利用(3.2)式得

\begin{eqnarray} \int _{B_{R}}e^{\beta \left | u-u_{2R} \right |}\left | \nabla u \right |^{p}{\rm d}x \leq \frac{C}{R^{p}}\int _{B_{2R}}e^{\beta \left | u-u_{2R} \right |} \left | u-u_{2R} \right |^{p}{\rm d}x. \end{eqnarray}
(3.10)

由于 u \in L^{\infty }(\Omega ), 故存在充分大的正常数 M ,使得 \left | u \right |\leq M .代入上式,得

\begin{eqnarray} \int _{B_{R}}\left | \nabla u \right |^{p}{\rm d}x \leq \frac{C}{R^{p}}\int _{B_{2R}}\left | u-u_{2R} \right |^{p}{\rm d}x, \end{eqnarray}
(3.11)

其中 C = C(C_{1}, C_{2}, C_{4}, p, M) ,引理3.1证毕.

v 是下列边值问题的弱解:

\begin{eqnarray} \left\{\begin{array}{ll} {\rm div} A(x^{*}, \nabla v) = 0 &in \;B_{\widetilde{R}}, \\ v = u \; \, & on \; \partial B_{\widetilde{R}}, \end{array}\right. \end{eqnarray}
(3.12)

其中 x^{*} \in B_{\widetilde{R}} 为定点,且 B_{\widetilde{R}} = B_{10\rho_{i}}(x_{i}) .

下面给出全局弱解的定义.

定义3.1  假设 v \in W^{1, p}(B_{\widetilde{R}}), 于是 v-u \in W_{0}^{1, p}(B_{\widetilde{R}}) ,则称 v \in W^{1, p}(B_{\widetilde{R}}) 是边值问题(3.12)在 B_{\widetilde{R}} 中的弱解,如果有

\begin{equation} \int _{B_{\widetilde{R}}}\left \langle A(x^{*}, \nabla v), \nabla \varphi \right \rangle {\rm d}x = 0 \end{equation}
(3.13)

对于任意的 \varphi \in W_{0}^{1, p}(B_{\widetilde{R}} ) 成立.

下面借鉴文献[12],给出 v 的有界性引理.

引理3.2  令 v \in W^{1, p}(B_{\widetilde{R}}) 是边值问题(3.12)的弱解,则有

\begin{equation} \sup _{ B_{\widetilde{R}}}\left | v \right |\leq \sup _{\partial B_{\widetilde{R}}}\left | u \right |\leq M. \end{equation}
(3.14)

  设 { } M = \sup _{\partial B_{\widetilde{R}}}u , { } m = \inf _{\partial B_{\widetilde{R}}}u ,则 s = \min \left \{ v, M \right \} 是边值问题(3.12)的弱上解.取非负函数 \varphi _{1} = v- s \in W_{0}^{1, p}(B_{\widetilde{R}}) 为检验函数,代入边值问题(3.12),结合 (1.4) 式得

\begin{eqnarray*} 0 &\leq & \int _{B_{\widetilde{R}}}\left \langle A(x^{*}, \nabla s ), \nabla \varphi _{1} \right \rangle {\rm d}x \nonumber\\ & = & \int _{B_{\widetilde{R}}}\left \langle A(x^{*}, \nabla s )- A(x^{*}, \nabla v ) , \nabla (v-s) \right \rangle {\rm d}x \nonumber\\ &\leq & -C_{2}\int _{B_{\widetilde{R}}}\left | \nabla s - \nabla v \right |^{p} {\rm d}x\leq 0. \end{eqnarray*}

于是有

\nabla v = \nabla s a.e. in\, B_{\widetilde{R}}.

由于 \varphi _{1} = v- \min \left \{ v, M \right \} \in W_{0}^{1, p}(B_{\widetilde{R}}) ,则 v = \min \left \{ v, M \right \} ,于是

v\leq M = \sup _{\partial B_{\widetilde{R}}}u.

同理可证得 v\geq m = \inf _{\partial B_{\widetilde{R}}}u .引理3.2得证.

由定义3.1很容易获得如下引理.

引理3.3  若 v \in W^{1, p}(B_{10\rho _{i}}(x_{i})) 是边值问题(3.12)在 B_{10\rho _{i}}(x_{i}) 中的弱解,其中 x_{i} \in E(1) , \rho _{i} 与在引理 2.2 中的定义相同,则有

\begin{equation} -\!\!\!\!\!\!\int _{B_{10\rho _{i}}(x_{i})}\left | \nabla v \right |^{p}{\rm d}x \leq C -\!\!\!\!\!\!\int _{B_{10\rho _{i}}(x_{i})}\left | \nabla u \right |^{p}{\rm d}x. \end{equation}
(3.15)

  取检验函数 \phi = u-v \in W_{0}^{1, p}(B_{10\rho _{i}}(x_{i})) ,由定义3.1,得

\begin{equation} \int _{B_{10\rho _{i}}(x_{i})}\left \langle A(x^{*}, \nabla v) , \nabla (u- v)\right \rangle {\rm d}x = 0. \end{equation}
(3.16)

\begin{equation} \int _{B_{10\rho _{i}}(x_{i})}\left \langle A(x^{*}, \nabla v) , \nabla v\right \rangle {\rm d}x = \int _{B_{10\rho _{i}}(x_{i})}\left \langle A(x^{*}, \nabla v) , \nabla u\right \rangle {\rm d}x. \end{equation}
(3.17)

由(1.2)及(1.4)式得

\begin{equation} \int _{B_{10\rho _{i}}(x_{i})}\left \langle A(x^{*}, \nabla v) , \nabla v\right \rangle {\rm d}x\geq C_{2}\int _{B_{10\rho _{i}}(x_{i})}\left | \nabla v \right |^{p} {\rm d}x. \end{equation}
(3.18)

由(1.3)式及Young不等式,得

\begin{eqnarray} &&\int _{B_{10\rho _{i}}(x_{i})}\left \langle A(x^{*}, \nabla v) , \nabla u\right \rangle {\rm d}x \\ &\leq& C_{1}\int _{B_{10\rho _{i}}(x_{i})}\left | \nabla v \right |^{p-1}\left | \nabla u \right |{\rm d}x \\ &\leq& C_{1}\left \{ \tau_{1} \int _{B_{10\rho _{i}}(x_{i})} \left | \nabla v \right |^{p}{\rm d}x +C(\tau _{1})\int _{B_{10\rho _{i}}(x_{i})} \left | \nabla u \right |^{p}{\rm d}x \right \}. \end{eqnarray}
(3.19)

综合(3.17), (3.18)和(3.19)式,得

\begin{eqnarray} C_{2}\int _{B_{10\rho _{i}}(x_{i})}\left | \nabla v \right |^{p} {\rm d}x \leq C_{1}\left \{ \tau_{1} \int _{B_{10\rho _{i}}(x_{i})} \left | \nabla v \right |^{p}{\rm d}x +C(\tau _{1})\int _{B_{10\rho _{i}}(x_{i})} \left | \nabla u \right |^{p}{\rm d}x \right \}. \end{eqnarray}
(3.20)

令常数 \tau_{1} >0 足够小,满足 C_2>C_1\tau_1 ,则有

\begin{eqnarray} -\!\!\!\!\!\! \int _{B_{10\rho _{i}}(x_{i})}\left | \nabla v \right |^{p} {\rm d}x \leq C -\!\!\!\!\!\!\int _{B_{10\rho _{i}}(x_{i})}\left | \nabla u \right |^{p}{\rm d}x, \end{eqnarray}
(3.21)

其中 C = C(C_{1}, C_{2}) ,于是引理3.3证毕.

在证明主要结论之前,给出如下引理.

引理3.4  若 v \in W^{1, p}(B_{10\rho _{i}}(x_{i})) 是边值问题(3.12)在 B_{10\rho _{i}}(x_{i}) 中的弱解, u \in W_{loc}^{1, p} (\Omega)\cap L^{\infty }(\Omega ) 是方程 \rm (1.1) 的局部弱解,算子 A B 满足(1.2)–(1.6)式.若

\begin{equation} -\!\!\!\!\!\!\int _{B_{10\rho _{i}}(x_{i})}\left | \nabla u \right |^{p}{\rm d}x \leq \epsilon, \end{equation}
(3.22)

则存在 N_{0}> 1 ,使得

\begin{equation} -\!\!\!\!\!\!\int _{B_{10\rho _{i}}(x_{i})}\left | \nabla (u-v) \right |^{p}{\rm d}x \leq \epsilon , \end{equation}
(3.23)

\begin{equation} \sup _{B_{5\rho _{i}}(x_{i})}\left | \nabla v \right |\leq N_{0}. \end{equation}
(3.24)

  若结论(3.23)式成立,则结论(3.24)式可证(参见文献[22,引理5.1]).

下面只需证明 (3.24) 式.选取检验函数 \varphi_{2} = u-v \in W_{0}^{1, p}(B_{10\rho _{i}}(x_{i})) ,代入定义1.1及定义3.1,得

\begin{equation} \int _{B_{10\rho _{i}}(x_{i})} \left \langle A(x, \nabla u), \nabla (u-v) \right \rangle {\rm d}x = \int _{B_{10\rho _{i}}(x_{i})} B(x, \nabla u)(u-v) {\rm d}x, \end{equation}
(3.25)

\begin{equation} \int _{B_{10\rho _{i}}(x_{i})} \left \langle A(x^{*}, \nabla v), \nabla (u-v) \right \rangle {\rm d}x = 0, \end{equation}
(3.26)

其中 x^{*} \in B_{10\rho _{i}}(x_{i}) 为定点.直接计算得

\begin{eqnarray} K_{1} = K_{2}+K_{3}, \end{eqnarray}
(3.27)

其中

\begin{eqnarray} && K_{1} = \int _{B_{10\rho _{i}}(x_{i})} \left \langle A(x, \nabla u)-A(x, \nabla v), \nabla (u-v) \right \rangle {\rm d}x, \\ && K_{2} = - \int _{B_{10\rho _{i}}(x_{i})} \left \langle A(x, \nabla v)-A(x^{*}, \nabla v), \nabla (u-v) \right \rangle {\rm d}x, \\ && K_{3} = \int _{B_{10\rho _{i}}(x_{i})} B(x, \nabla u )(u-v) {\rm d}x. \end{eqnarray}
(3.28)

先估计 K_{1}. 由(1.4)式得

\begin{eqnarray} K_{1}\geq C_{2}\int _{B_{10\rho _{i}}(x_{i})} \left | \nabla (u-v) \right |^{p} {\rm d}x. \end{eqnarray}
(3.29)

再估计 K_{2}. \rho _{i} \in (0, R_{0}/10] , (1.5)式, Young不等式和(2.12)式,得

\begin{eqnarray} K_{2} &\leq& C_{3}\omega (10\rho _{i}) \int _{B_{10\rho _{i}}(x_{i}) } \left | \nabla v \right |^{p-1} (\left | \nabla u \right |+\left | \nabla v \right | ) {\rm d}x \\ &\leq& C_{3}\omega (R_{0}) \left \{ \int _{B_{10\rho _{i}}(x_{i}) } \left | \nabla v \right | ^{p}{\rm d}x +\int _{B_{10\rho _{i}}(x_{i}) } (\left | \nabla u \right |^{p} + \left | \nabla v \right |^{p} ) {\rm d}x \right \} \\ &\leq& C_{3}\epsilon \left \{ \int _{B_{10\rho _{i}}(x_{i}) } \left | \nabla v \right |^{p} {\rm d}x +\int _{B_{10\rho _{i}}(x_{i}) } \left | \nabla u \right |^{p} {\rm d}x \right \}, \end{eqnarray}
(3.30)

由引理3.3得

\begin{eqnarray} K_{2} \leq C_{3}\epsilon \int _{B_{10\rho _{i}}(x_{i}) } \left | \nabla u \right |^{p} {\rm d}x, \end{eqnarray}
(3.31)

再利用(3.22)式得

\begin{eqnarray} K_{2} \leq C_{3}\left | B_{10\rho _{i}}(x_{i}) \right | \epsilon . \end{eqnarray}
(3.32)

最后估计 K_{3} .利用(1.6)式得

\begin{eqnarray} K_{3} \leq C_{4} \int _{B_{10\rho _{i}}(x_{i}) }\left | \nabla u \right |^{p}\left | u-v \right |{\rm d}x , \end{eqnarray}
(3.33)

\left | u \right |\leq M 和引理3.2得

\begin{eqnarray} K_{3}\leq C \int _{B_{10\rho _{i}}(x_{i}) }\left | \nabla u \right |^{p} {\rm d}x, \end{eqnarray}
(3.34)

其中 C = C(C_{4}, M) .综合所有 K_{i}(i = 1, 2, 3) ,得

\begin{eqnarray} \int _{B_{10\rho _{i}}(x_{i}) }\left | \nabla (u-v) \right |^{p}{\rm d}x \leq C\left | B_{10\rho _{i}}(x_{i}) \right | \epsilon +C \int _{B_{10\rho _{i}}(x_{i}) }\left | \nabla u \right |^{p} {\rm d}x, \end{eqnarray}
(3.35)

再由(3.22)式得

\begin{eqnarray} -\!\!\!\!\!\!\int _{B_{10\rho _{i}}(x_{i}) }\left | \nabla (u-v) \right |^{p} {\rm d}x\leq C\epsilon , \end{eqnarray}
(3.36)

其中 C = C(C_{2}, C_{3}, C_{4}, M). 引理3.4证毕.

现在开始证明定理1.1.

  对于任意的 \lambda \geq \lambda _{*} = (10/R_{0}) ^{n/p}\lambda _{0}+1 ,取 N_{0}>1 如引理3.4所述.利用引理3.4有

\begin{eqnarray} && \left | \left \{ x \in B_{5\rho _{i}}(x_{i}) :\left | \nabla u \right | > 2N_{0}\lambda \right \} \right | \\ &\leq& \left | \left \{ x \in B_{5\rho _{i}}(x_{i}) :\left | \nabla (u-v) \right | > N_{0}\lambda \right \} \right |+ \left | \left \{ x \in B_{5\rho _{i}}(x_{i}) :\left | \nabla v\right | > N_{0}\lambda \right \} \right | \\ & = & \left | \left \{ x \in B_{5\rho _{i}}(x_{i}) :\left | \nabla (u-v) \right | > N_{0}\lambda \right \} \right | \\ &\leq& \int _{B_{5\rho _{i}}(x_{i})\cap \left \{ x: \frac{\nabla (u-v)}{N_{0}}> \lambda\right \} } \lambda ^{p} {\rm d}x \\ &\leq& \frac{1}{N_{0}^{p}}\int _{B_{5\rho _{i}}(x_{i})}\left | \nabla (u-v) \right |^{p} {\rm d}x \\ &\leq& C\epsilon \left | B_{\rho _{i}}(x_{i}) \right |, \end{eqnarray}
(3.37)

于是,由(2.15)式得

\begin{eqnarray} \left | \left \{ x \in B_{5\rho _{i}}(x_{i}) :\left | \nabla u \right | > 2N_{0}\lambda \right \} \right |\leq \frac{C\epsilon }{\lambda ^{p}} \int _{ \left \{ x \in B_{\rho _{i}}(x_{i}) :\left | \nabla u \right |^{p}> \lambda ^{p}/2 \right \} } \left | \nabla u \right |^{p} {\rm d}x, \end{eqnarray}
(3.38)

其中 C = C(n, p, N_{0}). 考虑一族互不相交的球 \left \{ B_{\rho _{i}}(x_{i}) \right \} ,由引理2.2有

\begin{eqnarray} \bigcup _{i \in {\Bbb N}}B_{5\rho _{i}}(x_{i}) \supset E(1) = \left \{ x \in B_{1}:\left | \nabla u \right |^{p} > \lambda ^{p}\right \}, \end{eqnarray}
(3.39)

对任意的 \lambda \geq \lambda _{*} = (10/R_{0})^{n/p}\lambda _{0}+1 成立.综合(3.39)和(3.38)式,并注意到 \rho_{i} \leq \frac{R_{0}}{10} R_{0} \in (0, 1) ,得

\begin{eqnarray} \left | \left \{ x \in B_{1}:\left | \nabla u \right |^{p}> (2N_{0})^{p}\lambda ^{p} \right \} \right | & = & \left | \left \{ x \in B_{1}:\left | \nabla u \right |> 2N_{0} \lambda \right \} \right | \\ &\leq & \sum _{i}\left | \left \{ x \in B_{5\rho _{i}}(x_{i}): \left | \nabla u \right |> 2N_{0} \lambda \right \} \right | \\ &\leq & \frac{C\epsilon }{\lambda ^{p}} \sum _{i}\int _{\left \{ x \in B_{\rho _{i}}(x_{i}):\left | \nabla u \right |^{p} > \lambda ^{p} /2 \right \}}\left | \nabla u \right |^{p} {\rm d}x \\ &\leq & \frac{C\epsilon }{\lambda ^{p}} \int _{\left \{ x \in B_{2}:\left | \nabla u \right |^{p} > \lambda ^{p} /2 \right \} }\left | \nabla u \right |^{p} {\rm d}x. \end{eqnarray}
(3.40)

利用(2.7)式得

\begin{eqnarray} \int _{B_{1}}\phi \left ( \left | \nabla u \right |^{p} \right ) {\rm d}x & = & \int_{0}^{\infty }\left | \left \{ x \in B_{1}: \left | \nabla u \right |^{p}> \mu \right \} \right | {\rm d}\left [ \phi (\mu ) \right ] \\ & = & \int_{0}^{(2N_{0})^{p}\lambda _{*}^{p}} \left | \left \{ x \in B_{1} : \left | \nabla u \right |^{p} > \mu \right \} \right | {\rm d}\left [ \phi (\mu ) \right ] \\ &&+\int_{(2N_{0})^{p}\lambda _{*}^{p}}^{\infty } \left | \left \{ x \in B_{1} : \left | \nabla u \right |^{p} > \mu \right \} \right | {\rm d}\left [ \phi (\mu ) \right ] \\ & = & \int_{0}^{(2N_{0})^{p}\lambda _{*}^{p}} \left | \left \{ x \in B_{1} : \left | \nabla u \right |^{p} > \mu \right \} \right | {\rm d}\left [ \phi (\mu ) \right ] \\ &&+\int_{\lambda _{*}}^{ \infty } \left | \left \{ x \in B_{1} : \left | \nabla u \right |^{p} > (2N_{0})^{p}\lambda ^{p} \right \} \right | {\rm d}\left [ \phi \left ( (2N_{0})^{p}\lambda^{p} \right ) \right ] \\ & = & J_{1}+J_{2}. \end{eqnarray}
(3.41)

估计 J_{1} . \lambda _{*} 的定义及(2.9)式,得

\begin{eqnarray} \lambda _{*}^{p}\leq C\left [ \lambda _{0}^{p} +1 \right ]\leq C\left [ -\!\!\!\!\!\!\int _{B_{1}}\left | \nabla u \right |^{p}{\rm d}x+1 \right ], \end{eqnarray}
(3.42)

其中 C = C(n, p) .由引理3.1得

\begin{eqnarray} \lambda _{*}^{p}\leq C\left \{ -\!\!\!\! \!\! \int _{B_{2}}\left | u-u_{2R} \right |^{p} {\rm d}x +1 \right \}, \end{eqnarray}
(3.43)

因此,由(2.3)和(3.43)式得

\begin{eqnarray} J_{1} \leq \phi \left [ (2N_{0})^{p}\lambda _{*}^{p} \right ]\left | B_{1} \right | \leq C\left \{ \phi \left ( \int _{B_{2}} \left | u-u_{2R} \right |^{p}{\rm d}x \right )+1 \right \}, \end{eqnarray}
(3.44)

其中 C = C(n, p, \phi, N_{0} ).

再估计 J_{2}. 由(3.40)式得

\begin{eqnarray} J_{2} &\leq & \int_{0}^{ \infty } \left | \left \{ x \in B_{1} : \left | \nabla u \right |^{p} > (2N_{0})^{p}\lambda ^{p} \right \} \right | {\rm d}\left [ \phi \left ((2N_{0})^{p}\lambda^{p} \right ) \right ] \\ &\leq & C\epsilon \int_{0}^{\infty } \frac{1}{\lambda ^{p}} \int _{ \left \{ x \in B_{2} : \left | \nabla u \right |^{p} > \lambda ^{p}/2 \right \} } \left | \nabla u \right |^{p} {\rm d}x {\rm d}\left [ \phi \left ( (2N_{0})^{p}\lambda^{p} \right ) \right ], \end{eqnarray}
(3.45)

\mu = \lambda ^{p} 代入上述不等式,再利用(2.8)式得

\begin{eqnarray} J_{2} &\leq & C\epsilon \int_{0}^{\infty }\frac{1}{\mu } \int _{\left \{ x \in B_{2} :\left | \nabla u \right |^{p} > \mu /2\right \}} \left | \nabla u \right |^{p}{\rm d}x {\rm d}\left [ \phi \left ((2N_{0})^{p} \mu \right ) \right ] \\ &\leq & C\epsilon \int _{B_{2}}\phi ( \left | \nabla u \right |^{p}){\rm d}x, \end{eqnarray}
(3.46)

其中 C = C(n, p, \phi , N_{0}).

于是综合估计 J_{1} J_{2} ,得

\begin{eqnarray} \int _{B_{1}} \phi (\left | \nabla u \right |^{p}){\rm d}x \leq C\left \{ \phi \left ( \int _{B_{2}} \left | u-u_{2R} \right |^{p}{\rm d}x \right )+1 \right \} + C\epsilon \int _{B_{2}}\phi ( \left | \nabla u \right |^{p}){\rm d}x, \end{eqnarray}
(3.47)

选择适当的 \epsilon ,使得

\begin{eqnarray} C\epsilon = \frac{1}{2}, \end{eqnarray}
(3.48)

再通过引理2.3,将上述不等式最后一项积分重新吸收,得

\begin{eqnarray} \int _{B_{1}}\phi \left ( \left | \nabla u \right |^{p} \right ){\rm d}x \leq C\left \{ \phi \left ( \int _{B_{2}}\left | u-u_{2R} \right |^{p} {\rm d}x \right )+1 \right \}. \end{eqnarray}
(3.49)

最后通过缩放讨论,证毕.

3.2 逼近

现参考[18, 23]采用逼近方法将3.1小节添加的假设条件 \left | \nabla u \right |^{p} \in L_{loc}^{\infty }(\Omega )\subset L_{loc}^{\phi}(\Omega) 移除.

考虑Dirichlet问题

\begin{eqnarray} \left\{\begin{array}{ll} {\rm div}A(x, \nabla u_{k}) = B(x, \nabla u_{k}) in \;B_{2R}, \\ u_{k}-u \in W_{0}^{1, p}(B_{2R}). \end{array}\right. \end{eqnarray}
(3.50)

对所有 k = 1, 2, 3, \cdot\cdot\cdot ,存在唯一弱解 u_{k} \in W^{1, p}(B_{2R}) ,且 u_{k} \in L^{\infty}(B_{2R}) .由梯度的正则性理论知, \nabla u_{k} \in L^{\infty}(B_{2R}) (参见文献[23-24]).于是上一节在Orlicz空间的估计成立,即

\begin{equation} \int _{B_{R}}\phi (|\nabla u_{k}|^{p}){\rm d}x\leq C \left \{ \phi\left ( \int _{B_{2R}}|u_{k}-(u_{k})_{2R}|^{p}{\rm d}x \right ) +1 \right \}. \end{equation}
(3.51)

由于 u_{k} \in L^{\infty}(B_{2R}) \nabla u_{k} \in L^{\infty}(B_{2R}) ,因此存在一个子列 \left \{ u_{k} \right \} (仍表示为 \left \{ u_{k} \right \} )和函数 v \in W^{1, p}( B_{2R} ) ,使得

\begin{eqnarray} \left\{\begin{array}{ll} u_{k}\mathop{\longrightarrow}\limits^{\mbox强} v \; \; \;\; \, & x\in L^{p}(B_{2R} ), \\ \nabla u_{k} \mathop{\longrightarrow}\limits^{\mbox弱} \nabla v & x\in L^{p}(B_{2R} ). \end{array}\right. \end{eqnarray}
(3.52)

则有

\begin{equation} \nabla u_{k}\mathop{\longrightarrow}\limits^{\mbox强} \nabla v x\in L^{p}(B_{2R}) . \end{equation}
(3.53)

稍后给出证明过程.

由(3.53)式可知, v \in W^{1, p}(B_{2R} ) 是Dirichlet问题(3.50)的弱解.已知 u \in W^{1, p}(B_{2R} ) 也是Dirichlet问题(3.50)的弱解.从而由弱解的唯一性得 v = u ,则(3.53)式即为

\nabla u_{k}\mathop{\longrightarrow}\limits^{\mbox强} \nabla u x\in L^{p}(B_{2R} ) .

于是

\begin{equation} \| u_{k}-u \| _{W^{1, p} (B_{2R})}\rightarrow 0 \mbox{当} \;\; k\rightarrow \infty. \end{equation}
(3.54)

因此存在 \{u_{k}\}_{k = 1}^{\infty} 的子列(用 \{u_{k}\} 表示),使得

\begin{eqnarray} && u_{k}\rightarrow u \; \; \; a.e. \; in \; B_{2R} , \\ && \nabla u_{k}\rightarrow \nabla u a.e. \; in \; B_{2R} . \end{eqnarray}
(3.55)

于是由Fatou引理, |u_{k}|^{p} \in L^{\infty} (B_{2R}) \subset L^{\phi} (B_{2R}) , (3.51)式以及(3.55)式,得

\begin{eqnarray*} \int _{B_{R}} \phi ( |\nabla u|^{p} ){\rm d}x &\leq& \liminf\limits_{k\rightarrow \infty} \int _{B_{R}} \phi ( |\nabla u_{k}|^{p} ){\rm d}x \nonumber\\ &\leq& C\liminf\limits_{k\rightarrow \infty} \left \{ \phi\left ( \int _{B_{2R}}|u_{k}-(u_{k})_{2R}|^{p}{\rm d}x \right ) +1 \right \} \nonumber\\ &\leq& C\left \{ \phi\left ( \int _{B_{2R}}|u-u_{2R}|^{p}{\rm d}x \right ) +1 \right \}. \end{eqnarray*}

这就是说,为证明定理1.1,只需增加一个假设( \nabla u_{k} 是局部有界的)证明(1.10)式即可.一旦(1.10)式在一般情况下成立,则可经由标准覆盖讨论得到 |\nabla u|^{p} \in L_{loc}^{\phi} (\Omega) .

现证明(3.53)式.下面主要考虑 p\geq 2 的情形, 1<p<2 时,可参考文献[25]中相同的方法处理.取检验函数 \varphi _{3} = (u_{k}-v)e^{\theta |u_{k}-v|} ,其中 \theta 为待定正常数,代入Dirichlet问题(3.50)弱解的定义,得

\int _{B_{2R}}\left \langle A(x, \nabla u_{k}), \nabla ((u_{k}-v)e^{\theta |u_{k}-v|})\right \rangle {\rm d}x = \int _{B_{2R}} B(x, \nabla u_{k}) (u_{k}-v)e^{\theta |u_{k}-v|} {\rm d}x.

\int _{B_{2R}}\left \langle A(x, \nabla v), \nabla ((u_{k}-v)e^{\theta |u_{k}-v|})\right \rangle {\rm d}x = \int _{B_{2R}} B(x, \nabla v) (u_{k}-v)e^{\theta |u_{k}-v|} {\rm d}x.

两式相减整理得

\begin{eqnarray} J_{3}+J_{4} = J_{5}, \end{eqnarray}
(3.56)

其中

J_{3} = \int _{B_{2R}}\left \langle A(x, \nabla u_{k})-A(x, \nabla v), e^{\theta |u_{k}-v |} \nabla(u_{k}-v) \right \rangle {\rm d}x,

J_{4} = \theta \int _{B_{2R}}\left \langle A(x, \nabla u_{k})-A(x, \nabla v), |u_{k}-v| e^{\theta |u_{k}-v |} \nabla(u_{k}-v) \right \rangle {\rm d}x,

J_{5} = \int _{B_{2R}} (B(x, \nabla u_{k})-B(x, \nabla v)) e^{\theta |u_{k}-v |} (u_{k}-v) {\rm d}x.

估计 J_{3} .由(1.4)式得

\begin{eqnarray} J_{3}\geq C_{2}\int _{B_{2R}} |\nabla (u_{k}-v)|^{p} e^{\theta |u_{k}-v|}{\rm d}x. \end{eqnarray}
(3.57)

估计 J_{4} .由(1.4)式得

\begin{eqnarray} J_{4}\geq C_{2} \theta \int _{B_{2R}} |\nabla (u_{k}-v)|^{p} |u_{k}-v| e^{\theta |u_{k}-v|}{\rm d}x. \end{eqnarray}
(3.58)

最后估计 J_{5} .由(1.6)式得

\begin{eqnarray} J_{5}&\leq& C_{4} \int _{B_{2R}} (|\nabla u_{k}|^{p} + |\nabla v|^{p} ) |u_{k}-v| e^{\theta |u_{k}-v|}{\rm d}x \\ &\leq& C_{4} \int _{B_{2R}} |\nabla (u_{k}-v)|^{p} |u_{k}-v| e^{\theta |u_{k}-v|}{\rm d}x + C_{4} \int _{B_{2R}} |\nabla u_{k}|^{p} |u_{k}-v| e^{\theta |u_{k}-v|}{\rm d}x. \end{eqnarray}
(3.59)

由于 u_{k}, v \in L^{\infty }( B_{2R} ) ,故存在充分大的正常数 M ,使得 |u_{k}|\leq M, |v| \leq M .综合(3.56), (3.57), (3.58)和(3.59)式,并且令 \theta 满足 C_{2} \theta > C_{4} ,移项整理得

\begin{eqnarray} \int _{B_{2R}} |\nabla (u_{k}-v)|^{p} {\rm d}x \leq C \int _{B_{2R}} |\nabla u_{k}|^{p} |u_{k}-v| {\rm d}x. \end{eqnarray}
(3.60)

利用Hölder不等式得

\begin{eqnarray} \int _{B_{2R}} |\nabla (u_{k}-v)|^{p} {\rm d}x \leq C \left( \int _{B_{2R}} |\nabla u_{k}|^{p\alpha_{2}} {\rm d}x \right )^{\frac{1}{\alpha_{2}}} \left( \int _{B_{2R}} | u_{k} -v|^{\frac{\alpha_{2}}{\alpha_{2}-1}} {\rm d}x \right )^{\frac{\alpha_{2}-1}{\alpha_{2}}}, \end{eqnarray}
(3.61)

其中 \alpha_{2} 如(2.3)式所述.由引理2.1及(2.3)式,对任意 g \in L^{\phi } (B_{2R}) ,有

\begin{eqnarray*} \int _{B_{2R}} |g|^{\alpha_{2}} {\rm d}x &\leq& \int_{\{ x\in B_{2R} :|g|\leq 1 \} } |g|^{\alpha_{2}} {\rm d}x + \int_{\{ x\in B_{2R} :|g|\geq 1 \} } |g|^{\alpha_{2}} {\rm d}x \nonumber \\ &\leq& |B_{2R}|+ \frac{2a}{\phi(1)} \int _{B_{2R}} \phi (|g|) {\rm d}x, \end{eqnarray*}

其中常数 a 取自定义2.1, a>1 .由于 |\nabla u_{k}|^{p} \in L^{\phi}(B_{2R}) ,于是

\begin{eqnarray*} \int _{B_{2R}} |\nabla u_{k}|^{p\alpha_{2}} {\rm d}x \leq |B_{2R}|+ \frac{2a}{\phi(1)} \int _{B_{2R}} \phi (|\nabla u_{k}|^{p}) {\rm d}x < +\infty. \end{eqnarray*}

代入(3.61)式,再利用(3.52)式得

\begin{eqnarray} \int _{B_{2R}} |\nabla (u_{k}-v)|^{p} {\rm d}x \leq C \left( \int _{B_{2R}} | u_{k} -v|^{\frac{\alpha_{2}}{\alpha_{2}-1}} {\rm d}x \right )^{\frac{\alpha_{2}-1}{\alpha_{2}}} \rightarrow 0, \mbox{当} \;\; k \rightarrow \infty, \end{eqnarray}
(3.62)

其中 C = C( C_{2}, C_{4}, M, n, p, a) .于是(3.53)式得证.

参考文献

DiBenedetto E , Manfredi J .

On the higher integrability of the gradient of weak solutions of certain degenerate elliptic systems

American Journal of Mathematics, 1993, 115 (5): 1107- 1134

URL     [本文引用: 1]

Iwaniec T .

Projections onto gradient fields and Lp-estimates for degenerated elliptic operators

Studia Mathematica, 1983, 75 (3): 293- 312

URL     [本文引用: 1]

Acerbi E , Mingione G .

Gradient estimates for the p(x)-Laplacean system

Journal für die reine und angewandte Mathmatik, 2005, 584, 117- 148

URL     [本文引用: 1]

Byun S S , Wang L H .

Quasilinear elliptic equations with BMO coefficients in Lipschitz domains

Transactions of the American Mathematical Society, 2007, 359 (12): 5899- 5913

URL     [本文引用: 1]

Kinnunen J , Zhou S L .

A local estimate for nonlinear equations with discontinuous coefficients

Commuications in Partial Differential Equations, 1999, 24 (11/12): 2043- 2068

URL     [本文引用: 1]

Byun S S , Wang L H .

Lp-estimates for general nonlinear elliptic equations

Indiana University Mathematics Journal, 2007, 56 (6): 3193- 3221

Jia H , Li D S , Wang L H .

Regularity in Orlicz spaces for the Poisson equation

Manuscripta Mathematica, 2007, 122 (3): 265- 275

URL     [本文引用: 5]

Yao F P. Gradient estimates for weak solutions of \mathcal{A} -harmonic equations. Journal of Inequalities and Applications, 2010, Article ID: 685046. DOI: 10.1155/2010/685046

[本文引用: 5]

Yao F P .

Gradient estimates for parabolic A-harmonic equations

Nonlinear Analysis, 2011, 74, 1200- 1211

URL     [本文引用: 1]

李惠珍,郑神州.非散度型线性椭圆方程强解的Hessian估计[D].北京:北京交通大学, 2017

[本文引用: 1]

Li H Z, Zheng S Z. Hessian Estimates to Strong Solutions for Nondivergence Linear Elliptic Equations[D]. Beijing: Beijing Jiaotong University, 2017

[本文引用: 1]

Liang S , Zheng S Z .

Gradient estimate in Orlicz spaces for elliptic obstracle problems with partially BMO nonlinearities

Electronic Journal of Differential Equations, 2018, 58, 1- 15

URL     [本文引用: 1]

Zheng S Z , Zheng X L , Feng Z S .

Regularity for a class of degenerate elliptic equations with discontinuous coefficients under natural growth

Journal of Mathematical Analysis and Applications, 2008, 346 (2): 359- 373

URL     [本文引用: 2]

周树清, 胡振华, 彭冬云.

一类A -调和方程的障碍问题的很弱解的全局正则性

数学物理学报, 2017, 37A (4): 706- 713

URL     [本文引用: 1]

Zhou S Q , Hu Z H , Peng D Y .

Global regularity for very weak solutions to obstacle promlems corresponding to a class of A-harmonic equations

Acta Mathematica Scientia, 2017, 37A (4): 706- 713

URL     [本文引用: 1]

高红亚,褚玉明.拟正则映射与A -调和方程.北京:科学出版社, 2013

Gao H Y, Chu Y M. Quasiregular Mappings and A-Harmonic Equation. Beijing: Science Press, 2013

Zhang J J , Zheng S Z .

Weighted Lorentz estimates for nondivergence linear elliptic equations with partially BMO coefficients

Communications on Pure and Applied Analysis, 2017, 16 (3): 899- 914

URL    

佟玉霞, 郑神州, 程林娜.

A -调和张量的奇点可去性

数学物理学报, 2017, 37A (6): 1001- 1011

URL     [本文引用: 1]

Tong Y X , Zheng S Z , Cheng L N .

Removable singularities of weakly A-harmonic tensors

Acta Mathematica Scientia, 2017, 37A (6): 1001- 1011

URL     [本文引用: 1]

Byun S S , Lee M .

Weighted estimates for nondivergence parabolic equations in Orlicz spaces

Journal of Functional Analysis, 2015, 269 (8): 2530- 2563

URL     [本文引用: 2]

Byun S S , Yao F P , Zhou S L .

Gradient estimates in Orlicz space for nonlinear elliptic equations

Journal of Functional Analysis, 2008, 255 (8): 1851- 1873

URL     [本文引用: 2]

Wang L H , Yao F P , Zhou S L , Jia H L .

Optimal regularity for the Poisson equation

Proceedings of the American Mathematical Society, 2009, 137 (6): 2037- 2047

URL     [本文引用: 1]

Giaquinta M. Multiple integrals in the Calculus of Variations and Nonlinear Elliptic Systems. Princeton: Princeton University Press, 1983

[本文引用: 1]

高红亚, 贾苗苗.

障碍问题解的局部正则性和局部有界性

数学物理学报, 2017, 37A (4): 706- 713

URL     [本文引用: 1]

Gao H Y , Jia M M .

Local regularity and local boundedness for solutions to obstacle problems

Acta Mathematica Scientia, 2017, 37A (4): 706- 713

URL     [本文引用: 1]

Lieberman G M .

The natural generalization of the natural conditions of Ladyzhenskaya and Urall'tseva for elliptic equations

Communications in Partial Differential Equations, 1991, 16 (2/3): 311- 361

URL     [本文引用: 1]

Yao F P , Sun Y , Zhou S L .

Gradient estimates in Orlicz spaces for quasilinear elliptic equation

Nonlinear Analysis, 2008, 69 (8): 2553- 2565

URL     [本文引用: 2]

Tolksdorf P .

Regularity for more general class of quasilinear elliptic equations

Journal of Differential Equations, 1984, 51 (1): 126- 150

URL     [本文引用: 1]

Byun S S , Wang L H , Zhou S L .

Nonlinear elliptic equations with small BMO coefficients in Reifenberg domains

Journal of Functional Analysis, 2007, 250 (1): 167- 196

URL     [本文引用: 1]

/