We study the generalized Keldys-Fichera boundary value problem for a class of higher order equations with nonnegative characteristic. By using the acute angle principle and the Hölder inequalities and Young inequalities we discuss the existence of the weak solution. Then by using the inverse Hölder inequalities, we obtain the regularity of the weak solution in the anisotropic Sobolev space.
1. Introduction
Keldys [1] studies the boundary problem for linear elliptic equations with degenerationg on the boundary. For the linear elliptic equations with nonnegative characteristic forms, Oleinik and Radkevich [2] had discussed the Keldys-Fichera boundary value problem. In 1989, Ma and Yu [3] studied the existence of weak solution for the Keldys-Fichera boundary value of the nonlinear degenerate elliptic equations of second-order. Chen [4] and Chen and Xuan [5], Li [6], and Wang [7] had investigated the existence and the regularity of degenerate elliptic equations by using different methods. In this paper, we study the generalized Keldys-Fichera boundary value problem which is a kind of new boundary conditions for a class of higher-order equations with nonnegative characteristic form. We discuss the existence and uniqueness of weak solution by using the acute angle principle, then study the regularity of solution by using inverse Hölder inequalities in the anisotropic Sobolev Space.
We firstly study the following linear partial differential operator
(11)where
is an open set, the coefficients of
are bounded measurable, and the leading term coefficients satisfy
(12)We investigate the generalized Keldys-Fichera boundary value conditions as follows:
(13)
(14)
(15)with
and
, where
.
The leading term coefficients are symmetric, that is,
which can be made into a symmetric matrix
. The odd order term coefficients
can be made into a matrix
is the outward normal at
.
and
are the eigenvalues of matrices
and
, respectively.
and
are orthogonal matrix satisfying
(16)The boundary sets are
(17)At last, we study the existence and regularity of the following quasilinear differential operator with boundary conditions (1.3)–(1.5):
(18)where
and 
2. Formulation of the Boundary Value Problem
For second-order equations with nonnegative characteristic form, Keldys [1] and Fichera presented a kind of boundary that is the Keldys-Fichera boundary value problem, with that the associated problem is of well-posedness. However, for higher-order ones, the discussion of well-posed boundary value problem has not been seen. Here we will give a kind of boundary value condition, which is consistent with Dirichlet problem if the equations are elliptic, and coincident with Keldys-Fichera boundary value problem when the equations are of second-order.
We consider the linear partial differential operator
(21)where
is an open set, the coefficients of
are bounded measurable functions, and 
Let
be a series of functions with
. If in certain order we put all multiple indexes
with
into a row
, then
can be made into a symmetric matrix
. By this rule, we get a symmetric leading term matrix of (2.1), as follows:
(22)Suppose that the matrix
is semipositive, that is,
(23)and the odd order part of (2.1) can be written as
(24)where
is the Kronecker symbol. Assume that for all
, we have
(25)We introduce another symmetric matrix
(26)where
is the outward normal at
. Let the following matrices be orthogonal:
(27)satisfying
(28)where
is the transposed matrix of
are the eigenvalues of
and
are the eigenvalues of
. Denote by
(29)For multiple indices
means that
. Now let us consider the following boundary value problem,
(210)
(211)
(212)
(213)for all
and
, where
.
We can see that the item (2.13) of boundary value condition is determined by the leading
term matrix (2.2), and (2.12) is defined by the odd term matrix (2.6). Moreover, if
the operator
is a not elliptic, then the operator
(214)has to be elliptic.
In order to illustrate the boundary value conditions (2.11)–(2.13), in the following we give an example.
Example 2.1.
Given the differential equation
(215)Here
. Let
and
, then the leading and odd term matrices of (2.15) respectively are
(216)and the orthogonal matrices are
(217)We can see that
, and
as shown in Figure 1.The item (2.12) is
(218)and the item (2.13) is
(219)for all
and
. Since only
, hence we have
(220)however,
and
, therefore,
(221)Thus the associated boundary value condition of (2.15) is as follows:
(222)which implies that
is free on 
Remark 2.2.
In general the matrices
and
arranged are not unique, hence the boundary value conditions relating to the operator
may not be unique.
Remark 2.3.
When all leading terms of
are zero, (2.10) is an odd order one. In this case, only (2.11) and (2.12) remain.
Now we return to discuss the relations between the conditions (2.11)–(2.13) with Dirichlet and Keldys-Fichera boundary value conditions.
It is easy to verify that the problem (2.10)–(2.13) is the Dirichlet problem provided
the operator
being elliptic (see [11]). In this case,
for all
. Besides, (2.13) run over all
and
, moreover
is nondegenerate for any
. Solving the system of equations, we get
.
When
, namely,
is of second-order, the condition (2.12) is the form
(223)and (2.13) is
(224)Noticing
(225)thus the condition (2.13) is the form
(226)It shows that when
, (2.12) and (2.13) are coincide with Keldys-Fichera boundary value condition.
Next, we will give the definition of weak solutions of (2.10)–(2.13) (see [12]). Let
(227)where
is defined by
(228)We denote by
the completion of
under the norm
and by
the completion of
with the following norm
(229)Definition 2.4.
is a weak solution of (2.10)–(2.13) if for any
, the following equality holds:
(230)We need to check the reasonableness of the boundary value problem (2.10)–(2.13) under
the definition of weak solutions, that is, the solution in the classical sense are
necessarily the solutions in weak sense, and conversely when a weak solution satisfies
certain regularity conditions, it will surely satisfy the given boundary value conditions.
Here, we assume that all coefficients of
are sufficiently smooth.
Let
be a classical solution of (2.10)–(2.13). Denote by
(231)Thanks to integration by part, we have
(232)Since
, we have
(233)Because
satisfies (2.12),
(234)From the three equalities above we obtain (2.30).
Let
be a weak solution of (2.10)–(2.13). Then the boundary value conditions (2.11) and
(2.13) can be reflected by the space
. In fact, we can show that if
, then
satisfies
(235)Evidently, when
, we have
(236)If we can verify that for any
, (2.36) holds true, then we get
(237)which means that (2.35) holds true. Since
is dense in
, for
given, let
and
in
. Then
(238)Due to
satisfying (2.36), hence
satisfies (2.36). Thus (2.31) is verified.
Remark 2.5.
When (2.2) is a diagonal matrix, then (2.13) is the form
(239)where
In this case, the corresponding trace embedding theorem can be set, and the boundary
value condition (2.13) is naturally satisfied. On the other hand, if the weak solution
of (2.10)–(2.13) belongs to
for some
, then by the trace embedding theorems, the condition (2.13) also holds true.
It remains to verify the condition (2.12). Let
satisfy (2.30). Since
, hence we have
(240)On the other hand, by (2.30), for any
, we get
(241)Because the coefficients of
are sufficiently smooth, and
is dense in
, equality (2.41) also holds for any
. Therefore, due to
, we have
(242)From (2.36), one drives
(243)Furthermore,
(244)From (2.30) and (2.42), one can see that
(245)Noticing
in
, one deduces that
satisfies (2.12) provided
Finally, we discuss the well-posedness of the boundary value problem (2.10)–(2.13).
Let
be a linear space, and
be the completion of
, respectively, with the norm
. Suppose that
is a reflexive Banach space and
is a separable Banach space.
Definition 2.6.
A mapping
is called to be weakly continuous, if for any
in
, one has
(246)Lemma 2.7 (see [3]).
Suppose that
is a weakly continuous, if there exists a bounded open set
, such that
(247)then the equation
has a solution in
.
Theorem 2.8 (existence theorem).
Let
be an arbitrary open set,
and
. If there exist a constant
and
such that
(248)where
is the component of
corresponding to
, then the problem (2.10)–(2.13) has a weak solution in
.
Proof.
Let
be the inner product as in (2.31). It is easy to verify that
defines a bounded linear operator
. Hence
is weakly continuous (see [3]). From (2.42), for
we drive that
(249)Hence we obtain
(250)Thus by Hölder inequality (see [13]), we have
(251)By Lemma 2.7, the theorem is proven.
Theorem 2.9 (uniqueness theorem).
Under the assumptions of Theorem 2.8 with
in (2.48). If the problem (2.10)–(2.13) has a weak solution in
, then such a solution is unique. Moreover, if
in
,
, then the weak solution
of (2.10)–(2.13) is unique.
Proof.
Let
be a weak solution of (2.10)–(2.13). We can see that (2.30) holds for all
. Hence
is well defined. Let
. Then from (2.49) it follows that
, we obtain
, which means that the solution of (2.10)–(2.13) in
is unique. If all the odd terms
of
, then (2.30) holds for all
, in the same fashion we known that the weak solution of (2.10)–(2.13) in
is unique. The proof is complete.
Remark 2.10.
In next subsection, we can see that under certain assumptions, the weak solutions
of degenerate elliptic equations are in
.
3. Existence of Higher-Order Quasilinear Equations
Given the quasilinear differential operator
(31)where
and 
Let
, the odd order part of (3.1) be as that in (2.4),
, and
be the same as those in Section 2. The leading matrix is
(32)and the eigenvalues are
. We denote 
We consider the following problem:
(33)Denote the anisotropic Sobolev space by
(34)whose norm is
(35)when all
for
, then the space is denoted by
.
is termed the critical embedding exponent from
to
, if
is the largest number of the exponent
in where
, and the embedding is continuous.
For example, when
is bounded, the space
with norm
is an anisotropic Sobolev space, and the critical embedding exponents from
to
are
.
Suppose that the following hold.
The coefficients of the leading term of
satisfy one of the following two conditions:
(
)
(
)
There is a constant
such that
(36)
There are functions
with
, such that
(37)
There is a constant
such that
(38)where
or
.
There is a constant
such that
(39)where
is a critical embedding exponent from
to
. Let
be defined by (2.27) and
be the completion of
under the norm
(310)and
be the completion of
with the norm
(311)where 
is a weak solution of (3.3), if for any
, we have
(312)Theorem 3.1.
Under the conditions
, if
, then the problem (3.3) has a weak solution in
.
Proof.
Denote by
the left part of (3.12). It is easy to verify that the inner product
defines a bounded mapping
by the condition
.
Let
, by
, one can deduce that
(313)Noticing that
,
,
, by Hölder and Young inequalities (see[13]), from (3.13) we can get
(314)Ones can easily show that the mapping
is weakly continuous. Here we omit the details of the proof. By Lemma 2.7, this theorem
is proven.
In the following, we take an example to illustrate the application of Theorem 3.1.
Example 3.2.
We consider the boundary value problem of odd order equation as follows:
(315)where
is an unit ball in
, see Figure 2
The odd term matrix is
(316)It is easy to see that
(317)The boundary value condition associated with (3.15) is
(318)Applying Theorem 3.1, if
, then the problem (3.15)–(3.18) has a weak solution
.
4.
-Solutions of Degenerate Elliptic Equations
We start with an abstract regularity result which is useful for the existence problem
of
-solutions of degenerate quasilinear elliptic equations of order
. Let
be the spaces defined in Definition 2.6, and
be a reflective Banach space, at the same time
.
Lemma 4.1.
Under the hypotheses of Lemma 2.7, there exists a sequence of
in
such that
. Furthermore, if, we can derive that
,
is a constant, then the solution
of
belongs to
.
In the following, we give some existence theorems of
-solutions for the boundary value conditions (4.3)–(4.5) of higher-order degenerate
elliptic equations.
First, we consider the quasilinear equations
(41)where
. Now, we consider the following problem
(42)
(43)
(44)
(45)The boundary value condition associated with (4.1) is given by (4.3)–(4.5). Suppose
that
is bounded, and the following assumptions hold.
The condition (3.6) holds, and there is a continuous function
on
such that
(46)where
, 

is a measure zero set in
, and there is a sequence of subdomains
with cone property such that
and 
The positive definite condition is
(47)where
is a constant,
or
for
.
The structure conditions are
(48)where
is a constant,
,
is the critical embedding exponent from
to
.
Let
be defined by (2.27) and
be the completion of
with the norm
(49)Definition 4.2.
is a weak solution of (4.2)–(4.5), if for any
, the following equality holds:
(410)Theorem 4.3.
Under the assumptions
, if
, then the problem and (4.2)–(4.5) has a weak solution
. Moreover, if there is a real number
, such that
(411)then the weak solution 
Proof.
According to Lemma 4.1, it suffices to prove that there is a constant
such that for any
(
is as that in Section 3) with
, we have
(412)From (4.10) we know
(413)Due to
and
we have
(414)Noticing that
, and
consequently we have
(415)where the
or
,
is the critical embedding exponent from
to
. By the reversed Hölder inequality (see [14])
(416)Then we obtain
(417)From (4.15) and (4.17), the estimates (4.12) follows. This completes the proof.
Next, we consider a quasilinear equation
(418)where 
Suppose that the following holds.
There is a real number
such that
(419)
The structural conditions are
(420)where C is a constant,
,
are the critical embedding exponents from
to
.
Theorem 4.4.
Let the conditions
and
be satisfied. If
, then the problem (4.2)–(4.5) has a weak solution
.
The proof of Theorem 4.4 is parallel to that of Theorem 4.3; here we omit the detail.
Acknowledgment
This project was supported by the National Natural Science Foundation of China (no. 10971148).
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Figure 1.
Figure 2.