# Linear and nonlinear abstract elliptic equations with *VMO* coefficients and applications

- Veli B Shakhmurov
^{1}Email author

**2013**:6

https://doi.org/10.1186/1687-1812-2013-6

© Shakhmurov; licensee Springer 2013

**Received: **10 September 2012

**Accepted: **13 November 2012

**Published: **9 January 2013

## Abstract

In this paper, maximal regularity properties for linear and nonlinear elliptic differential-operator equations with *VMO* (vanishing mean oscillation) coefficients are studied. For linear case, the uniform separability properties for parameter dependent boundary value problems is obtained in ${L}^{p}$ spaces. Then the existence and uniqueness of a strong solution of the boundary value problem for a nonlinear equation is established. In application, the maximal regularity properties of the anisotropic elliptic equation and the system of equations with *VMO* coefficients are derived.

**MSC:** 58I10, 58I20, 35Bxx, 35Dxx, 47Hxx, 47Dxx.

## Keywords

*VMO*coefficientsboundary value problemsdifferential-operator equationsmaximal ${L}^{p}$ regularityabstract function spacesnonlinear elliptic equations

## 1 Introduction

where *a* is a complex valued function, *s* is a positive, *λ* is a complex parameter, and $A=A(x)$, ${A}_{i}={A}_{i}(x)$ are linear and *B* is a nonlinear operator in a Banach space *E*. Here, the principal coefficients *a* and *A* may be discontinuous. More precisely, we assume that *a* and $A(\cdot ){A}^{-1}({x}_{0})$ belong to the operator-valued Sarason class *VMO*. The Sarason class *VMO* was first defined in [1]. In the recent years, there has been considerable interest in elliptic and parabolic equations with *VMO* coefficients. This is mainly due to the fact that the *VMO* class contains as a subspace $C(\overline{\mathrm{\Omega}})$ that ensures the extension of ${L}_{p}$-theory of operators with continuous coefficients to discontinuous coefficients (see, *e.g.*, [2–7]). On the other hand, the Sobolev spaces ${W}^{1,n}(\mathrm{\Omega})$ and ${W}^{\sigma ,\frac{\sigma}{n}}(\mathrm{\Omega})$, $0<\sigma <1$, are also contained in *VMO*. Global regularity of the Dirichlet problem for elliptic equations with *VMO* coefficients has been studied in [2–4]. We refer to the survey [4], where an excellent presentation and relations with another similar results can be found concerning the regularizing properties of these operators in the framework of Sobolev spaces.

It is known that many classes of PDEs (partial differential equations), pseudo DEs and integro DEs can be expressed in the form of DOEs. Many researchers (see, *e.g.*, [8–24]) investigated similar spaces of functions and classes of PDEs under a single DOE. Moreover, the maximal regularity properties of DOEs with continuous coefficients were studied, *e.g.*, in [10, 19, 20].

*VMO*-operator coefficients is considered in abstract spaces. We shall prove the uniform separability of the problem (1),

*i.e.*, we show that, for each $f\in {L}^{p}(0,1;E)$, there exists a unique strong solution

*u*of the problem (1) and a positive constant

*C*depending only on

*p*,

*γ*,

*E*and

*A*such that

Note that the principal part of a corresponding differential operator is nonselfadjoint. Nevertheless, the sharp uniform coercive estimate for the resolvent and Fredholmness are established. Then the existence and uniqueness of the above nonlinear problem is derived. In application, we study maximal regularity properties of anisotropic elliptic equations in mixed ${L}^{\mathbf{p}}$ spaces and the systems (finite or infinite) of differential equations with *VMO* coefficients in the scalar ${L}^{p}$ space.

Since (1) involves unbounded operators, it is not easy to get representation for the Green function and estimate of solutions. Therefore, we use the modern harmonic analysis elements, *e.g.*, the Hilbert operators and the commutator estimates in *E*-valued ${L}^{p}$ spaces, embedding theorems of Sobolev-Lions spaces and some semigroups estimates to overcome these difficulties. Moreover, we also use our previous results on equations with continuous leading coefficients and the perturbation theory of linear operators to obtain our main assertions.

## 2 Notations and background

*E*to be a Banach space and $\mathrm{\Omega}\subset {R}^{n}$. ${L}^{p}(\mathrm{\Omega};E)$ denotes the space of all strongly measurable

*E*-valued functions that are defined on Ω with the norm

*E*-valued local integrable functions with the norm

where *B* ranges in the class of the balls in ${R}^{n}$ and ${f}_{B}$ is the average $\frac{1}{|B|}{\int}_{B}f(x)\phantom{\rule{0.2em}{0ex}}dx$.

where *B* ranges in the class of balls with radius *ρ*.

We will say that a function $f\in \mathit{BMO}(E)$ is in $\mathit{VMO}(E)$ if ${lim}_{r\to +0}\eta (r)=0$. We will call the $\eta (r)$ a *VMO* modulus of *f*.

Note that, if $E=\mathbf{C}$, where **C** is the set of complex numbers, then $\mathit{BMO}(E)$ and $\mathit{VMO}(E)$ coincide with the John-Nirenberg class *BMO* and Sarason class *VMO*, respectively.

*E*is called a

*UMD*(unconditional martingale difference)-space if the Hilbert operator

is bounded in ${L}_{p}(R,E)$, $p\in (1,\mathrm{\infty})$ (see, *e.g.*, [26, 27]). *UMD* spaces include, *e.g.*, ${L}_{p}$, ${l}_{p}$ spaces and Lorentz spaces ${L}_{pq}$, $p,q\in (1,\mathrm{\infty})$.

*A*is said to be a

*φ*-positive (or positive) in a Banach space

*E*with the bound $M>0$ if $D(A)$ is dense on

*E*and

*I*is an identity operator in

*E*and $L(E)$ is the space of bounded linear operators in

*E*. Sometimes instead of $A+\lambda I$, it will be written as $A+\lambda $ and denoted by ${A}_{\lambda}$. It is known [[22], §1.15.1] that there exist fractional powers ${A}^{\theta}$ of the positive operator

*A*. Let $E({A}^{\theta})$ denote the space $D({A}^{\theta})$ with the graphical norm

*R*-bounded (see [24, 26]) if there is a positive constant

*C*such that for all ${T}_{1},{T}_{2},\dots ,{T}_{m}\in W$ and ${u}_{1,}{u}_{2},\dots ,{u}_{m}\in {E}_{1}$, $m\in N$

where $\{{r}_{j}\}$ is a sequence of independent symmetric $\{-1,1\}$-valued random variables on $[0,1]$.

*i.e.*, the space of all

*E*-valued rapidly decreasing smooth functions on ${R}^{n}$. Let

*F*denote the Fourier transformation. A function $\mathrm{\Psi}\in {L}^{\mathrm{\infty}}({R}^{n};B({E}_{1},{E}_{2}))$ is called a Fourier multiplier from ${L}_{p}({R}^{n};{E}_{1})$ to ${L}_{p}({R}^{n};{E}_{2})$ if the map $u\to {\mathrm{\Lambda}}_{\mathrm{\Psi}}u={F}^{-1}\mathrm{\Psi}(\xi )Fu$, $u\in S({R}^{n};{E}_{1})$ is well defined and extends to a bounded linear operator

The set of all multipliers from ${L}_{p}({R}^{n};{E}_{1})$ to ${L}_{p}({R}^{n};{E}_{2})$ will be denoted by ${M}_{p}^{p}({E}_{1},{E}_{2})$. For ${E}_{1}={E}_{2}=E$, it will be denoted by ${M}_{p}^{p}(E)$.

**Definition 1** A Banach space *E* is said to be a space satisfying the multiplier condition if, for any $\mathrm{\Psi}\in {C}^{(n)}({R}^{n};L(E))$, the *R*-boundedness of the set $\{{\xi}^{\beta}{D}_{\xi}^{\beta}\mathrm{\Psi}(\xi ):\xi \in {R}^{n}\mathrm{\setminus}0,\beta \in {U}_{n}\}$ implies that Ψ is a Fourier multiplier in ${L}_{p}({R}^{n};E)$, *i.e.*, $\mathrm{\Psi}\in {M}_{p}^{p}(E)$ for any $p\in (1,\mathrm{\infty})$.

**Definition 2** The *φ*-positive operator *A* is said to be an *R*-positive in a Banach space *E* if there exists $\phi \in [0,\pi )$ such that the set ${L}_{A}=\{A{(A+\lambda )}^{-1}:\lambda \in {S}_{\phi}\}$ is *R*-bounded.

*E*uniformly in

*x*if $D(A(x))$ is independent of

*x*, $D(A(x))$ is dense in

*E*and

for all $\lambda \in S(\phi )$, $\phi \in [0,\pi )$.

Let ${\sigma}_{\mathrm{\infty}}({E}_{1},{E}_{2})$ denote the space of all compact operators from ${E}_{1}$ to ${E}_{2}$. For ${E}_{1}={E}_{2}=E$, it is denoted by ${\sigma}_{\mathrm{\infty}}(E)$.

*E*are two Banach spaces and ${E}_{0}$ is continuously and densely embedded into

*E*. Let

*m*be a natural number. ${W}^{m,p}(\mathrm{\Omega};{E}_{0},E)$ (the so-called Sobolev-Lions type space) denotes a space of all functions $u\in {L}^{p}(\mathrm{\Omega};{E}_{0})$ possessing the generalized derivatives ${D}_{k}^{m}u=\frac{{\partial}^{m}u}{\partial {x}_{k}^{m}}$ such that ${D}_{k}^{m}u\in {L}^{p}(\mathrm{\Omega};E)$ endowed with the norm

*s*be a positive parameter. We define in ${W}^{m,p}(\mathrm{\Omega};{E}_{0},E)$ the following parameter-dependent norm:

The space ${B}_{p,p}^{s}(\mathrm{\Gamma};{E}_{0},E)$ is defined as a trace space for ${W}^{m,p}(\mathrm{\Omega};{E}_{0},E)$ as in a scalar case (see, *e.g.*, [[22], §3.6.1]).

Function $u\in {W}^{2,p}(0,1;E(A),E,{L}_{k})=\{u\in {W}^{2,p}(0,1;E(A),E),{L}_{k}u=0\}$ satisfying the equation (1) a.e. on $(0,1)$ is said to be a solution of the problem (1) on $(0,1)$.

From [28] we have

**Theorem A**

_{ 1 }

*Suppose the following conditions are satisfied*:

- (1)
*E**is a Banach space satisfying the multiplier condition with respect to*$p\in (1,\mathrm{\infty})$*and**A**is an**R*-*positive operator in**E*; - (2)
$\alpha =({\alpha}_{1},{\alpha}_{2},\dots ,{\alpha}_{n})$

*are**n**tuples of nonnegative integer numbers such that*$\varkappa =\frac{|\alpha |}{m}\le 1$*and*$0<\mu \le 1-\varkappa $; - (3)
$\mathrm{\Omega}\in {R}^{n}$

*is a region such that there exists a bounded linear extension operator from*${W}^{m,p}(\mathrm{\Omega};E(A),E)$*to*${W}^{m,p}({R}^{n};E(A),E)$.

*Then the embedding*

*is continuous and there exists a positive constant*${C}_{\mu}$

*such that*

*for all* $u\in {W}^{m,p}(\mathrm{\Omega};E(A),E)$ *and* $0<h\le {h}_{0}<\mathrm{\infty}$.

**Theorem A**

_{ 2 }

*Suppose all the conditions of Theorem*A

_{1}

*are satisfied*.

*Assume*Ω

*is a bounded region in*${R}^{n}$

*and*${A}^{-1}\in {\sigma}_{\mathrm{\infty}}(E)$.

*Then*,

*for*$0<\mu \le 1-\varkappa $,

*the embedding*

*is compact*.

In a similar way as in [[3], Theorem 2.1], we have the following result.

**Lemma A**

_{ 1 }

*Let*

*E*

*be a Banach space and*$f\in \mathit{VMO}(E)$.

*The following conditions are equivalent*:

- (1)
$f\in \mathit{VMO}(E)$;

- (2)
*f**is in the**BMO**closure of the set of uniformly continuous functions which belong to**VMO*; - (3)
${lim}_{y\to 0}{\parallel f(x-y)-f(x)\parallel}_{\ast ,E}=0$.

*For*$f\in {L}^{p}(\mathrm{\Omega};E)$, $p\in (1,\mathrm{\infty})$, $a\in {L}^{\mathrm{\infty}}({R}^{n})$,

*consider the commutator operator*

From [[21], Theorem 1] and [[29], Corollary 2.7], we have

**Theorem A**_{
3
} *Let* *E* *be a UMD space and* $a\in \mathit{VMO}\cap {L}^{\mathrm{\infty}}({R}^{n})$. *Then* $H[a,f]$ *is a bounded operator in* ${L}^{p}(R;E)$, $p\in (1,\mathrm{\infty})$.

From Theorem A_{3} and the property (2) of Lemma A_{1} we obtain, respectively, the following.

**Theorem A**

_{ 4 }

*Assume all the conditions of Theorem*A

_{3}

*are satisfied*.

*Also*,

*let*$a\in \mathit{VMO}\cap {L}^{\mathrm{\infty}}({R}^{n})$

*and let*

*η*

*be the*

*VMO*

*modulus of*

*a*.

*Then*,

*for any*$\epsilon >0$,

*there exists a positive number*$\delta =\delta (\epsilon ,\eta )$

*such that*

**Theorem A**

_{ 5 }

*Let*

*E*

*be a UMD space and*$A(\cdot )$

*uniformly*

*R*-

*positive in*

*E*.

*Moreover*,

*let*$A(\cdot ){A}^{-1}({x}_{0})\in {L}_{\mathrm{\infty}}(R;L(E))\cap \mathit{BMO}(L(E))$, ${x}_{0}\in R$.

*Then the commutator operator*

*is bounded in* ${L}^{p}(R;E)$, $p\in (1,\mathrm{\infty})$.

**Theorem A**_{
6
} *Assume all the conditions of Theorem* A_{5} *are satisfied and* *η* *is a* *VMO* *modulus of* $A(\cdot ){A}^{-1}({x}_{0})$.

*Then*,

*for any*$\epsilon >0$,

*there exists a positive number*$\delta =\delta (\epsilon ,\eta )$

*such that*

*where*${m}_{k}\in \{0,1\}$,

*a*, ${\alpha}_{ki}$, ${\beta}_{ki}$

*are complex numbers*,

*s*

*is a positive parameter*,

*λ*

*is a complex spectral parameter*, ${\mu}_{i}=\frac{i}{2}+\frac{1}{2p}$, ${\theta}_{k}=\frac{{m}_{k}}{2}+\frac{1}{2p}$, ${A}_{\lambda}=A+\lambda $

*and*

*A*

*is a linear operator in*

*E*.

*Let*${\omega}_{1}$, ${\omega}_{2}$

*be roots of the equation*$a{\omega}^{2}+1=0$

*and let*

*It is known that if the operator*

*A*

*is*

*φ*-

*positive in*

*E*,

*then operators*${\omega}_{k}{A}_{\lambda}^{\frac{1}{2}}$, $k=1,2$

*generate analytic semigroups*

From [[19], Theorem 2] and [[30], Theorem 3.1], we obtain

**Theorem A**

_{ 7 }

*Assume the following conditions are satisfied*:

- (1)
*E**is a Banach space satisfying the multiplier condition with respect to*$p\in (1,\mathrm{\infty})$; - (2)
*A**is an**R*-*positive operator in**E**for*$0\le \phi <\pi $*and*$\mu \ne 0$; - (3)
$Re{\omega}_{k}\ne 0$

*and*$\frac{\lambda}{{\omega}_{k}}\in S(\phi )$*for*$\lambda \in S(\phi )$, $k=1,2$.

*Then*

- (1)
*for*$f\in {L}_{p}(0,1;E)$, ${f}_{k}\in {E}_{k}$, $\lambda \in S(\phi )$*and for sufficiently large*$|\lambda |$,*the problem*(2)*has a unique solution*$u\in {W}^{2,p}(0,1;E(A),E)$.*Moreover*,*the coercive uniform estimate holds*$\sum _{i=0}^{2}{s}^{\frac{i}{2}}|\lambda {|}^{1-\frac{i}{2}}{\parallel {u}^{(i)}\parallel}_{{L}^{p}(0,1;E)}+{\parallel Au\parallel}_{{L}^{p}(0,1;E)}\le C[{\parallel f\parallel}_{{L}^{p}(0,1;E)}+\sum _{k=1}^{2}{\parallel {f}_{k}\parallel}_{{E}_{k}}].$ - (2)

*where*${B}_{ij}(\lambda )$

*and*${D}_{ij}(\lambda )$

*are uniformly bounded operators in*

*E*

*and*

where $a=a(x)$ is a complex valued function, *s* is a positive parameter, ${m}_{k}\in \{0,1\}$, ${\alpha}_{ki}$, ${\beta}_{ki}$ are complex numbers, *λ* is a spectral parameter, ${\theta}_{k}=\frac{{m}_{k}}{2}+\frac{1}{2p}$ and $A(x)$ is a linear operator in *E*.

In the next theorem, let us consider the case that principal coefficients are continuous. The well-posedness of this problem occurs in the studying of equations with *VMO* coefficients. From [[19], Theorem 3] and [[21], Theorem 5.1], we get

**Theorem A**

_{ 8 }

*Suppose the following conditions are satisfied*:

- (1)
*E**is a Banach space satisfying the multiplier condition with respect to*$p\in (1,\mathrm{\infty})$; - (2)
$a\in C[0,1]$, $-a\in S(\phi )$, $a(0)=a(1)$,

*and*$\mu (x)\ne 0$*for a*.*e*. $x\in [0,1]$; - (3)
$Re{\omega}_{k}(x)\ne 0$

*and*$\frac{\lambda}{{\omega}_{k}}\in S(\phi )$*for*$\lambda \in S(\phi )$, $k=1,2$.*a*.*e*. $x\in [0,1]$; - (4)$A(x)$
*is a uniformly**R*-*positive operator in**E**and*$A(\cdot ){A}^{-1}({x}_{0})\in C([0,1];L(E)),\phantom{\rule{1em}{0ex}}{x}_{0}\in (0,1),A(0)=A(1).$

*Then*,

*for all*$f\in {L}^{p}(0,1;E)$, $\lambda \in S(\phi )$

*and for sufficiently large*$|\lambda |$,

*there is a unique solution*$u\in {W}^{2,p}(0,1;E(A),E)$

*of the problem*(4).

*Moreover*,

*the following coercive uniform estimate holds*:

## 3 DOEs with VMO coefficients

**Condition 1**Assume the following conditions are satisfied:

- (1)
*E*is a*UMD*space, $p\in (1,\mathrm{\infty})$; - (2)
$a\in \mathit{VMO}\cap {L}^{\mathrm{\infty}}(R)$, ${\eta}_{1}$ is a

*VMO*modulus of*a*, $-a\in S(\phi )$, $\mu (x)\ne 0$; - (3)
$Re{\omega}_{k}(x)\ne 0$ and $\frac{\lambda}{{\omega}_{k}}\in S(\phi )$ for $\lambda \in S(\phi )$, $0\le \phi <\pi $, $k=1,2$. a.e. $x\in [0,1]$;

- (4)$A(x)$ is a uniformly
*R*-positive operator in*E*and$A(\cdot ){A}^{-1}({x}_{0})\in {L}_{\mathrm{\infty}}(0,1;L(E))\cap \mathit{VMO}(L(E)),\phantom{\rule{1em}{0ex}}{x}_{0}\in (0,1);$ - (5)
$a(0)=a(1)$, $A(0)=A(1)$ and ${\eta}_{2}$ is a

*VMO*modulus of $A(\cdot ){A}^{-1}({x}_{0})$.

First, we obtain an integral representation formula for solutions.

**Lemma 1**

*Let Condition*1

*hold and*$f\in {L}^{p}(0,1;E)$.

*Then*,

*for all solutions*

*u*

*of the problem*(5)

*belonging to*${W}^{2,p}(0,1;E(A),E)$,

*we have*

*here*${B}_{ij}^{\mathrm{\prime}}(\lambda )$, ${D}_{ij}^{\mathrm{\prime}}(\lambda )$

*are uniformly bounded operators*,

*and the expression* ${\mathrm{\Gamma}}_{2\lambda}^{\mathrm{\prime}}(x,x-y)$ *is a scalar multiple of* ${\mathrm{\Gamma}}_{2\lambda}(x,x-y)$.

_{7}, we get

_{3}, gives the conclusion for

□

**Theorem 1**

*Suppose Condition*1

*is satisfied*.

*Then there exists a number*$b\in (0,1)$

*such that the uniform coercive estimate*

*holds for large enough* $|\lambda |$ *and* $u\in {W}^{2,p}(0,b;E(A),E)$, ${L}_{bk}u=0$, $\lambda \in S(\phi )$, *where* *C* *is a positive constant depending only on* *p*, ${M}_{0}$, ${\eta}_{1}$, ${\eta}_{2}$.

*Proof*By Lemma 1, for any solution $u\in {W}^{2,p}(0,b;E(A),E)$ of the problem (8), we have

where the expression ${\mathrm{\Gamma}}_{b\lambda}^{\mathrm{\prime}}(x,x-y)$ differs from ${\mathrm{\Gamma}}_{2b\lambda}(x,x-y)$ only by a constant.

*A*and the analyticity of semigroups ${U}_{k\lambda}(x)$ in a similar way as in [[30], Theorem 3.1], we get

*E*, we have

_{4}, A

_{6}and in view of (10)-(12) for any $\epsilon >0$, there exists a positive number $b=b(\epsilon ,{\eta}_{1},{\eta}_{2})$ such that

Hence, the estimates (13)-(15) imply (9). □

**Theorem 2**

*Assume Condition*1

*holds*.

*Let*$u\in {W}^{2,p}(0,1;E(A),E)$

*be a solution of*(4).

*Then*,

*for sufficiently large*$|\lambda |$, $\lambda \in S(\phi )$,

*the following coercive uniform estimate holds*:

*Proof* This fact is shown by a covering and flattening argument, in a similar way as in Theorem A_{8}. Particularly, by partition of unity, the problem is localized. Choosing diameters of supports for corresponding finite functions, by using Theorem 1, Theorems A_{4}, A_{6}, A_{7} and embedding Theorem A_{1} (see the same technique for DOEs with continuous coefficients [19, 20]), we obtain the assertion.

*i.e.*,

□

**Theorem 3**

*Assume Condition*1

*holds*.

*Then*,

*for all*$f\in {L}^{p}(0,1;E)$, $\lambda \in S(\phi )$

*and for large enough*$|\lambda |$,

*the problem*(5)

*has a unique solution*$u\in {W}^{2,p}(0,1;E(A),E)$.

*Moreover*,

*the following coercive uniform estimate holds*:

*Proof*First, let us show that the operator $Q+\lambda $ has a left inverse. Really, it is clear that

_{1}for $u\in {W}^{2,p}(0,1;E(A),E)$, we have

*ε*and $C(\epsilon )$ such that

The estimate (19) implies that (4) has a unique solution and the operator ${Q}_{s}+\lambda $ has a bounded inverse in its rank space. We need to show the rank space coincides with all the space ${L}^{p}(0,1;E)$. It suffices to prove that there is a solution $u\in {W}^{2,p}(0,1;E(A),E)$ for all $f\in {L}^{p}(0,1;E)$. This fact can be derived in a standard way, approximating the equation with a similar one with smooth coefficients [19, 20]. More precisely, by virtue of [[23], Theorem 3.4], *UMD* spaces satisfy the multiplier condition. Moreover, by the part (2) of Lemma A_{1}, given $a\in \mathit{VMO}$ with *VMO* modules $\eta (r)$, we can find a sequence of mollifiers functions $\{{a}_{h}\}$ converging to *a* in *BMO* as $h\to 0$ with a *VMO* modulus ${\eta}_{h}$ such that ${\eta}_{h}(r)\le \eta (r)$. In a similar way, it can be derived for the operator function $A(x){A}^{-1}({x}_{0})\in \mathit{VMO}(L(E))$. □

**Result 1**Theorem 3 implies that the resolvent ${({Q}_{s}+\lambda )}^{-1}$ satisfies the following sharp uniform estimate:

for $|arg\lambda |\le \phi $, $\phi \in (0,\pi )$ and $s>0$.

The estimate (20) particularly implies that the operator *Q* is uniformly positive in ${L}^{p}(0,1;E)$ and generates analytic semigroups for $\phi \in (\frac{\pi}{2},\pi )$ (see, *e.g.*, [[22], §1.14.5]).

**Remark 1** Conditions $a(0)=a(1)$, $A(0)=A(1)$ arise due to nonlocality of the boundary conditions (4). If the boundary conditions are local, then the conditions mentioned above are not required any more.

Consider the problem (1), where ${L}_{k}u$ is the same boundary condition as in (4). Let ${O}_{s}$ denote a differential operator generated by the problem (1). We will show the separability and Fredholmness of (1).

**Theorem 4**

*Assume*

- (1)
*Condition*1*holds*; - (2)

*Then*,

*for all*$f\in {L}^{p}(0,1;E)$

*and for large enough*$|\lambda |$, $\lambda \in S(\phi )$,

*there is a unique solution*$u\in {W}^{2,p}(0,1;E(A),E)$

*of the problem*(1)

*and the following coercive uniform estimate holds*:

*Proof*It is sufficient to show that the operator ${O}_{s}+\lambda $ has a bounded inverse ${({O}_{s}+\lambda )}^{-1}$ from ${L}^{p}(0,1;E)$ to ${W}^{2,p}(0,1;E(A),E)$. Put ${O}_{s}u={Q}_{s}u+{Q}_{0}u$, where

_{1}, there is a small

*ε*and $C(\epsilon )$ such that

Then, by above relation and by virtue of Theorem 3, we get the assertion. □

Theorem 4 implies the following result.

**Result 2**Suppose all the conditions of Theorem 4 are satisfied. Then the resolvent ${({O}_{s}+\lambda )}^{-1}$ of the operator ${O}_{s}$ satisfies the following sharp uniform estimate:

for $|arg\lambda |\le \phi $, $\phi \in [0,\pi )$ and $s>0$.

**Theorem 5** *Assume all the conditions of Theorem * 4 *hold and* ${A}^{-1}\in {\sigma}_{\mathrm{\infty}}(E)$. *Then the problem* (24) *is Fredholm from* ${W}^{2,p}(0,1;E(A),E)$ *into* ${L}^{p}(0,1;E)$.

*Proof* Theorem 4 implies that the operator ${O}_{s}+\lambda $ has a bounded inverse ${({O}_{s}+\lambda )}^{-1}$ from ${L}^{p}(0,1;E)$ to ${W}^{2,p}(0,1;E(A),E)$ for large enough $|\lambda |$; that is, the operator ${O}_{s}+\lambda $ is Fredholm from ${W}^{2,p}(0,1;E(A),E)$ into ${L}^{p}(0,1;E)$. Then, by virtue of Theorem A_{2} and by perturbation theory of linear operators, we obtain the assertion. □

## 4 Nonlinear DOEs with VMO coefficients

where *a* is a complex valued function, and $A=A(x)$, ${A}_{i}={A}_{i}(x)$ are possible operators in a Banach space *E*, where $b(s)$ is a positive continuous independent of *u*.

Theorem 4 implies the following result.

**Result 3**Let all the conditions of Theorem 4 be satisfied. Then the problem (25), for $f\in {L}^{p}(0,b(s);E)$, $p\in (1,\mathrm{\infty})$, $\lambda \in {S}_{\phi}$ and for large enough $|\lambda |$, has a unique solution $u\in {W}^{2,p}(0,b;E(A),E)$ and the following coercive uniform estimate holds:

*Proof*Really, under the substitution $\tau =xb(s)$, the moving boundary problem (25) maps to the following BVP with a parameter in a fixed domain $(0,1)$:

Then, by virtue of Theorem 4, we obtain the assertion. □

where ${m}_{k}\in \{0,1\}$, ${\alpha}_{ki}$, ${\beta}_{ki}$ are complex numbers, $x\in (0,b)$, where *b* is a positive number in $(0,{b}_{0}]$.

*A*is a

*φ*-positive operator in a Banach space

*E*. Let

**Remark 2**By using [[22], §1.8], we obtain that the embedding ${D}^{j}Y\in {E}_{j}$ is continuous and there exists the constant ${C}_{1}$ such that for $w\in Y$, $W=\{{w}_{0,}{w}_{1}\}$, ${w}_{j}={D}^{j}w(\cdot )$, $j=0,1$,

**Condition 2**Assume the following are satisfied:

- (1)
$\eta ={(-1)}^{{m}_{1}}{\alpha}_{1}{\beta}_{2}-{(-1)}^{{m}_{2}}{\alpha}_{2}{\beta}_{1}\ne 0$ and $a(x)$ is a positive continuous function on $[0,b]$, $a(0)=a(b)$;

- (2)
*E*is a UMD space and $p\in (1,\mathrm{\infty})$; - (3)$F(x,{\upsilon}_{0},{\upsilon}_{1}):[0,b]\times {X}_{0}\to E$ is a measurable function for each ${\upsilon}_{i}\in {E}_{i}$, $i=0,1$; $F(x,\cdot ,\cdot )$ is continuous with respect to $x\in [0,b]$ and $f(x)=F(x,0)\in X$. Moreover, for each $R>0$, there exists ${\mu}_{R}$ such that${\parallel F(x,U)-F(x,\overline{U})\parallel}_{E}\le {\mu}_{R}{\parallel U-\overline{U}\parallel}_{{X}_{0}},$where $U=\{{u}_{0},{u}_{1}\}$ and $\overline{U}=\{{\overline{u}}_{0},{\overline{u}}_{1}\}$ for a.a. $x\in [0,b]$, ${u}_{i},{\overline{u}}_{i}\in {E}_{i}$ and${\parallel U\parallel}_{{X}_{0}}\le R,\phantom{\rule{2em}{0ex}}{\parallel \overline{U}\parallel}_{{X}_{0}}\le R.$
- (4)
for $U=\{{u}_{0},{u}_{1}\}\in {X}_{0}$, the operator $B(x,U)$ is

*R*-positive in*E*uniformly with respect to $x\in [0,b]$; $B(x,U){B}^{-1}({x}^{0},U)\in C([0,b];B(E))$, where the domain definition $D(B(x,U))$ does not depend on*x*and*U*; $B(x,W):(0,b)\times {X}_{0}\to B(E(A),E)$ is continuous, where $A=A(x)=B(x,W)$ for fixed $W=\{{w}_{0},{w}_{1}\}\in {X}_{0}$; - (5)
for each $R>0$, there is a positive constant $L(R)$ such that ${\parallel [B(x,U)-B(x,\overline{U})]\upsilon \parallel}_{E}\le L(R){\parallel U-\overline{U}\parallel}_{{X}_{0}}{\parallel A\upsilon \parallel}_{E}$ for $x\in (0,b)$, $U,\overline{U}\in {X}_{0}$, ${\parallel U\parallel}_{{X}_{0}},{\parallel \overline{U}\parallel}_{{X}_{0}}\le R$ and $\upsilon \in D(A)$ and $A(0)=A(b)$.

**Theorem 6** *Let Condition* 1 *hold*. *Then there is* $b\in (0,{b}_{0}]$ *such that the problem* (26) *has a unique solution that belongs to the space* ${W}_{p}^{2}(0,b;E(A),E)$.

*C*does not depend on $f\in X$ and $b\in (0,{b}_{0}]$. We want to solve the problem (26) locally by means of maximal regularity of the linear problem (27) via the contraction mapping theorem. For this purpose, let

*w*be a solution of the linear BVP (27). Consider a ball

*Q*on ${B}_{r}$ by $Q\upsilon =u$, where

*u*is a solution of the problem (28). We want to show that $Q({B}_{r})\subset {B}_{r}$ and that

*Q*is a contraction operator provided

*b*is sufficiently small and

*r*is chosen properly. For this aim, by using maximal regularity properties of the problem (28), we have

*i.e.*,

By a suitable choice of ${\mu}_{R}$, ${L}_{R}$ and for sufficiently small $b\in (0,{b}_{0})$, we obtain ${\parallel Q\upsilon -Q\overline{\upsilon}\parallel}_{Y}<\eta {\parallel \upsilon -\overline{\upsilon}\parallel}_{Y}$, $\eta <1$, *i.e.*, *Q* is a contraction operator. Eventually, the contraction mapping principle implies a unique fixed point of *Q* in ${B}_{r}$ which is the unique strong solution $u\in Y$. □

## 5 Boundary value problems for anisotropic elliptic equations with VMO coefficients

The Fredholm property of BVPs for elliptic equations with parameters in smooth domains were studied, *e.g.*, in [8, 10], also, for nonsmooth domains, these questions were investigated, *e.g.*, in [31].

*∂*Ω. Let us consider the nonlocal boundary value problems on a cylindrical domain $G=(0,1)\times \mathrm{\Omega}$ for the following anisotropic elliptic equation with

*VMO*top-order coefficients:

*s*is a positive parameter,

*a*, ${d}_{i}$ are complex valued functions, ${\alpha}_{ki}$ and ${\beta}_{ki}$ are complex numbers,

**p**-summable scalar-valued functions with a mixed norm (see,

*e.g.*, [[32], §1]),

*i.e.*, the space of all measurable functions

*f*defined on

*G*, for which

Analogously, ${W}^{2,2m,\mathbf{p}}(G)$ denotes the anisotropic Sobolev space with the corresponding mixed norm [[32], §10].

**Theorem 7**

*Let the following conditions be satisfied*;

- (1)
$a,{d}_{0}\in \mathit{VMO}\cap {L}^{\mathrm{\infty}}(R)$, $a(0)=a(1)$, $-a\in S(\phi )$, $\mu (x)\ne 0$,

*a*.*e*. $x\in [0,1]$; - (2)
$Re{\omega}_{k}\ne 0$

*and*$\frac{\lambda}{{\omega}_{k}}\in S(\phi )$*for*$\lambda \in S(\phi )$, $0\le \phi <\pi $, $k=1,2$*a*.*e*. $x\in [0,1]$; - (3)
${d}_{1}\in {L}^{\mathrm{\infty}}$, ${d}_{1}(\cdot ,y){d}_{0}^{\frac{1}{2}-\nu}(\cdot )\in {L}^{\mathrm{\infty}}(0,1)$

*for a*.*e*. $y\in \mathrm{\Omega}$*and*$0<\nu <\frac{1}{2}$; - (4)
${a}_{\alpha}\in \mathit{VMO}\cap {L}^{\mathrm{\infty}}({R}^{n})$

*for each*$|\alpha |=2m$*and*${a}_{\alpha}\in [{L}^{\mathrm{\infty}}+{L}^{{\gamma}_{k}}](\mathrm{\Omega})$*for each*$|\alpha |=k<2m$*with*${r}_{k}\ge q$*and*$2m-k>\frac{l}{{r}_{k}}$; - (5)
${b}_{j\beta}\in {C}^{2m-{m}_{j}}(\partial \mathrm{\Omega})$

*for each**j*,*β**and*${m}_{j}<2m$, ,*for*$|\beta |={m}_{j}$, ,*where*$\sigma =({\sigma}_{1},{\sigma}_{2},\dots ,{\sigma}_{n})\in {R}^{n}$*is a normal to**∂G*; - (6)
*for*$y\in \overline{\mathrm{\Omega}}$, $\xi \in {R}^{n}$, $\nu \in S(\phi )$, $\phi \in (0,\pi )$, $|\xi |+|\nu |\ne 0$*let*$\nu +{\sum}_{|\alpha |=2m}{a}_{\alpha}(y){\xi}^{\alpha}\ne 0$; - (7)

*has a unique solution* $\vartheta \in {C}_{0}({R}_{+})$ *for all* $h=({h}_{1},{h}_{2},\dots ,{h}_{n})\in {R}^{n}$, *and for* ${\xi}^{\mid}\in {R}^{n-1}$ *with* $|{\xi}^{\mid}|+|\nu |\ne 0$.

*Then*

- (a)
*for all*$f\in {L}^{\mathbf{p}}(G)$, $\lambda \in S(\phi )$*and sufficiently large*$|\lambda |$,*the problem*(29)-(31)*has a unique solution**u**belonging to*${W}^{2,2m,\mathbf{p}}(G)$*and the following coercive uniform estimate holds*:$\sum _{i=0}^{2}{s}^{\frac{i}{2}}|\lambda {|}^{1-\frac{i}{2}}{\parallel \frac{{\partial}^{i}u}{{\partial}^{i}x}\parallel}_{{L}^{\mathbf{p}}(G)}+\sum _{|\beta |=2m}{\parallel {D}_{y}^{\beta}u\parallel}_{{L}^{\mathbf{p}}(G)}\le C{\parallel f\parallel}_{{L}^{\mathbf{p}}(G)};$ - (b)
*for*$\lambda =0$,*the problem*(29)-(31)*is Fredholm in*${L}^{\mathbf{p}}(G)$.

*Proof*Let $E={L}^{{p}_{1}}(\mathrm{\Omega})$. Then by virtue of [26], the part (1) of Condition 1 is satisfied. Consider the operator

*A*acting in ${L}^{{p}_{1}}(\mathrm{\Omega})$ defined by

has a unique solution for $f\in {L}^{{p}_{1}}(\mathrm{\Omega})$ and arg $\nu \in S(\phi )$, $|\nu |\to \mathrm{\infty}$. Moreover, in view of [[10], Theorem 8.2], the operator *A* is *R*-positive in ${L}^{{p}_{1}}(\mathrm{\Omega})$, *i.e.*, Condition 1 holds. Moreover, it is known that the embedding ${W}^{2m,{p}_{1}}(\mathrm{\Omega})\subset {L}^{{p}_{1}}(\mathrm{\Omega})$ is compact (see, *e.g.*, [[22], Theorem 3.2.5]). Then, by using interpolation properties of Sobolev spaces (see, *e.g.*, [[22], §4]), it is clear that the condition (2) of Theorem 4 is fulfilled too. Then from Theorems 4, 5, the assertions are obtained. □

## 6 Systems of differential equations with VMO coefficients

*VMO*coefficients,

where *s* is a positive parameter, *a*, ${b}_{mj}$, ${d}_{mj}$ are complex valued functions, *N* is a finite or infinite natural number, ${\alpha}_{ki}$ and ${\beta}_{ki}$ are complex numbers, ${\mu}_{i}=\frac{i}{2}+\frac{1}{2p}$.

*Q*denote the operator in ${L}^{p}(0,1;{l}_{q})$ generated by the problem (32)-(33). Let

**Theorem 8**

*Suppose the following conditions are satisfied*:

- (1)
$a\in \mathit{VMO}\cap {L}^{\mathrm{\infty}}(R)$, $a(0)=a(1)$, $-a\in S(\phi )$, $\mu (x)\ne 0$

*a*.*e*. $x\in (0,1)$; - (2)
$Re{\omega}_{k}(x)\ne 0$

*and*$\frac{\lambda}{{\omega}_{k}}\in S(\phi )$*for*$\lambda \in S(\phi )$,*a*.*e*. $x\in (0,1)$, $0\le \phi <\pi $, $k=1,2$; - (3)
${d}_{j}\in \mathit{VMO}\cap {L}^{\mathrm{\infty}}(R)$, ${b}_{mj},{d}_{mj}\in {L}^{\mathrm{\infty}}(0,1)$, $p\in (1,\mathrm{\infty})$;

- (4)

*Then*,

*for all*$f(x)={\{{f}_{m}(x)\}}_{1}^{N}\in {L}^{p}(0,1;{l}_{q})$, $\lambda \in S(\phi )$

*and for sufficiently large*$|\lambda |$,

*the problem*(32)-(33)

*has a unique solution*$u={\{{u}_{m}(x)\}}_{1}^{\mathrm{\infty}}$

*belonging to*${W}^{2,p}((0,1),{l}_{q}(D),{l}_{q})$

*and the following coercive estimate holds*:

*Proof*Really, let $E={l}_{q}$,

*A*and ${A}_{k}(x)$ be infinite matrices such that

It is clear that the operator *A* is *R*-positive in ${l}_{q}$. Therefore, by Theorem 4, the problem (32)-(33) has a unique solution $u\in {W}^{2,p}((0,1);{l}_{q}(D),{l}_{q})$ for all $f\in {L}^{p}((0,1);{l}_{q})$, $\lambda \in S(\phi )$ the estimate (34) holds. □

**Remark 3** There are many positive operators in different concrete Banach spaces. Therefore, putting concrete Banach spaces and concrete positive operators (*i.e.*, pseudo-differential operators or finite or infinite matrices for instance) instead of *E* and *A*, respectively, by virtue of Theorem 4, 5, we can obtain a different class of maximal regular BVPs for partial differential or pseudo-differential equations or their finite and infinite systems with *VMO* coefficients.

## Declarations

## Authors’ Affiliations

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