
Recepción: 26 Septiembre 2021
Aprobación: 15 Mayo 2022
Abstract: In this paper, we consider the existence of infinitely many sign-changing solutions for an elliptic equation involving double critical Hardy–Sobolev–Maz’ya terms. By using a compactness result obtained in [C.H. Wang, J. Yang, Infinitely many solutions for an elliptic problem with double Hardy–Sobolev–Maz’ya terms, Discrete Contin. Dyn. Syst., 36(3):1603–1628, 2016], we prove the existence of these solutions by a combination of invariant sets method and Ljusternik–Schnirelman- type minimax method.
Keywords: Hardy–Sobolev–Maz’ya exponents, invariant sets, sign-changing solutions, minimax method.
1 Introduction and main results
Let
and 
. are the critical Hardy–Sobolev–Maz’ya exponents,
is an open bounded domain in
We study the following equation:
(1)where
is a positive function,
It is well known that solutions of (1) are critical points of the corresponding functional 
given by
(2)By using the following Hardy–Sobolev–Maz’ya inequality (Lemma 1), we know that
is well defined and
functional on
for any open subset of 
Since (1) involves the double critical Hardy–Sobolev–Maz’ya exponents, we can use the pioneering idea of Brézis and Nirenberg [5], or the concentration compactness principle of Lions [16, 17], or the global compactness of Struwe [23] to show that (2) has a critical point, then get a positive solution to (1).
When
and
(1) is related to the well-known Brézis– Nirenberg problem [5]
(3)where
is the critical Sobolev exponent. Since the pioneering work of [5], there are some important results on this problem. See, e.g., [6, 8, 9, 11, 25]. Here we would like to point out [10]. In this paper, Devillanova and Solimini proved that when
, (3) has infinitely many solutions for each
. Let us now briefly recall the main results concerning the sign-changing solutions of (3) obtained before. If
and
is a ball, then for any
, (3) has infinitely many nodal solutions, which are built by using particular symmetries of the domain
(see [12]). In [22], Solimini proved that if
is a ball and
, for each
, (3) has infinitely many sign-changing radial solutions. When
is a ball and
, there is a
such that (3) has no radial solutions, which change sign if
(see [2]). In [12, 22], the symmetry of the ball plays an essential role, hence their methods are invalid for general domains.
When
, (1) is becoming Hardy–Sobolev–Maz’ya equation

By using the idea of [10], the authors of [26] obtained infinitely many solutions for Hardy– Sobolev–Maz’ya equation. Ganguly [13] and Wang [29] used different methods to get infinitely many sign-changing solutions. For the existence of infinitely many solutions or infinitely many sign-changing solutions for the related equations, see [14, 24, 30, 32] and the references therein. Very recently, Wang and Yang [27] proved the existence of infinitely many sign-changing solutions for (1).
Theorem 1. Suppose that
and
is a bounded domain. If
in a neighborhood of
, where
is the outward normal of
. If
when
and if
when
, then (1)has infinitely many sign-changing solutions.
Wang and Yang also considered the following nonexistence theorem.
Theorem 2. (See [27].) Suppose that
and
for every
. Then (1)does not have nontrivial solution in a domain, which is star shaped domain with respect to the origin.
Remark 1. Let
be the first eigenvalue of
(4)Since
and is strictly positive, system (4) has infinitely many eigenvalues
such that
. It is characterized by the following variational principle:
(5)Let
be the orthonormal eigenfunction corresponding to
and
. Denote

Then
and
It is easy to know that if
, equation (1) has infinitely many sign-changing solutions. Indeed, by multiplying the first eigenfunction
and integrating both sides, then we can check that if
, any nontrivial solution of (1) has to change sign. Therefore, by the result of [28], to prove Theorem 1 it suffices to consider the case of
.
Remark 2. When
and
, Cao and Peng [6] considered the following system:
(6)They obtained a pair of sign-changing solutions to (6). In [8,32], the authors get infinitely many sign-changing solutions for (6). They only considered the case
In another case,
, the mean curvature of
at
plays an important role in the existence of mountain pass solutions, see [3,6,14]. As it is pointed in [4,31], there are some differences between the case
and
. When
, solutions of (6) have a singularity at
, and the authors of [8, 32] impose the condition
. If
, no such condition is needed. So the estimates for the case
and the case
are very different. Therefore we have generalize the results in [32] to the case
.
Remark 3. In order to prove the results, Wang and Yang [27] first used an abstract theorem, which is introduced by Schechter and Zou [21]. Then by combining with the uniform bounded theorem due to [28], the authors of [27] obtained infinitely many sign-changing solutions. The methods introduced in [4, 8, 13, 21, 31] sometimes are limited because, by general minimax procedure to get the Morse indices of sign-changing critical points, sometimes are not clear. Another limited condition is that the corresponding functional is also needed to be
.
Before giving our main results, we give some notations first. We will always denote
Let
be endowed with the standard scalar and norm

The norm on
with
is given by 
with the norm
, where
denote the Lebesgue measure in
. Denote
and 
We will use the usual Ljusternik–Schnirelman-type minimax method and invariant set method to prove Theorem 1. Our method is much simpler than the proof of [27]. In fact, our approach also works for the Brézis–Nirenberg problem involving subcritical perturbation term
, which is not
. However, the techniques developed by Wang and Yang [27] or Schechter and Zou [21] cannot be applied directly. Let us outline the proof of Theorem 1 and explain the difficulties we will encounter.
In general, by using the combination of invariant sets method and minimax method to obtain infinitely many nodal critical points, we need the energy functional satisfies the Palais–Smale condition in all energy level. This fact prevents us from using the variational methods directly to prove the existence of infinitely many sign-changing solutions for (1) because
does not satisfy the Palais–Smale condition for large energy level due to the double critical Hardy–Sobolev–Maz’ya exponents
and
.
In order to overcome the difficulty, we will adopt the idea in [10, 24] and [4, 31]. We first study the following perturbed problem:
(7)where
is a small constant. The corresponding energy functional is
(8)By the following lemmas, we will know
is a
function on
and satisfies the Palais–Smale condition. It follows from [1, 20] that
has infinitely many critical points. More precisely, there are positive numbers
, with
as
. Moreover, a critical point
for
satisfies 
Next, we will show that for any fixed
are uniformly bounded with respect to
, then we can apply the following compactness result Proposition 1 (see [28, Thm. 1.3]), which essentially follows from the uniform bounded theorem due to Devillanova and Solimini [10], to show that
converges strongly to
in
as
.
Therefore it is easy to prove that
is a solution of (1) with 
Proposition 1. (See [28].) Suppose that
and
satisfies the conditions in Theorem 1. If
when
and
when
, then for any sequence
, which is a solution of (7) with
satisfying
for some constant independent of
has a sequence, which converges strongly in 
.
In the end, we will distinguish two cases to prove that
has infinitely many sign- changing critical points.
Case I. There are
satisfying 
Case II. There is a positive integer
such that
for all
.
The central task in this procedure is to deal with case II. In fact, we can prove that the usual Krasnoselskii genus of
is denoted in Section 2) is at least two, where
Then our result is obtained.
Throughout this paper, the letters
will be used to denote various positive constants, which may vary from line to line and are not essential to the problem. The closure and the boundary of set
are denoted by
and
, respectively. We denote
weak convergence and by
strong convergence. Also if we take a subsequence of a sequence
, we shall denote it again
.
The paper is organized as follows. In Section 2, we introduce some notations and Hardy–Sobolev–Maz’ya inequality. In Section 3, we give an auxiliary operator
and construct the invariant sets. We give the proof of Theorem 1 in Section 4.
2 Preliminaries
Now we give some integrals inequalities, for details we refer to [19].
Lemma 1 [Hardy–Sobolev–Maz’ya inequality]. Let
then there exist a positive constant
such that
(9)for all 
Lemma 2. (See [13].) If
is a bounded subset of
then

with the inclusion being continuous whenever 
Remark 4. If
for
then
with

For each
and
, we define

Lemma 3. (See [13].) Let
and
, then the embedding
is compact.
By Lemmas 2, 3 and Hardy–Sobolev–Maz’ya inequality, we know that the singular term
and
are finite and
where
isindependent of
. Therefore
is a
function on
By Lemma 3,
satisfies the Palais–Smale condition. In order to prove Theorem 1, it is enough to obtain sign-changing critical points for the functional
.
Fix
In the following, we will always assume that 
. In order to construct the minimax values for the perturbed functional
, the following two technique lemmas are needed.
Lemma 4. Assume
Then there exists
such that for all 

where 
Proof. Since
is finite dimensional, by Lemma 2, we know that
is defined as the norm on
There is a constant
such that
for all
Therefore

Since
and
, we have that
The proof is complete.
Lemma 5. For any 
,
there exists
such that

Proof.

Since
and
, there exists
such that
The proof is complete.
Lemma 5 implies that 0 is a strict local minimum critical point. Then we can construct invariant sets containing all the positive and negative solutions of (1) for the gradient flow of
. Therefore nodal solutions can be found outside of these sets.
3 Auxiliary operator and invariant subsets of descending flow
For any 
, let
be given by

for
. Then the gradient of
has the form

Note that the set of fixed points of
is the same as the set of critical points of
, which is
. It is easy to check that
is locally Lipschitz continuous.
We consider the negative gradient flow
of
defined by

Here and in the sequel, for
, denote
, the convex cones

For
we define

In the following, we will show that there exists
such that
is an invariant set under the descending flow for all
. Note that
contains only signchanging functions, where

since
contains only signchanging functions. By a version of the symmetric mountain pass theorem, which provides the minimax critical values on
, we can prove that (6) has infinitely many sign-changing solutions.
For any
and
denotes the open
neighborhood of N , i.e.,

whose closure and boundary are denoted by
and
. By the following result, we can know that a neighborhood of
is an invariant set. We can use similar way as Lemma 2 in [9] and Lemma 3.1 in [3] to get the following lemma.
Lemma 6. There exists
such that for any
there holds

and

Moreover, every nontrivial solutions
and
of (5) are positive and negative, respectively.
By using the combination of invariant sets method and minimax method, we can construct a nodal solution first, then to prove our main result. We need a deformation lemma in the presence of invariant sets.
Definition 1. A subset
is an invariant set with respect to
if, for any
,
for all 
From Lemma 6 we may choose an
sufficiently small such that
are invariant set. Set
. Note that
int
and
only contains sign-changing functions.
Since
satisfies the Palais–Smale condition, we have the following deformation lemma, which follows from Lemma 5.1 in [18] (also see Lemma 2.4 in [15]).
Define
where 
Let
be such that
where
dist 
We can use the similar method to the proof of Lemma 5.1 [18] and Lemma 2.4 [15] to prove the following lemma.
Lemma 7. Assume that
satisfies Palais–Smale condition, then there exists an
such that for any
, there exists
satisfying:


is odd and a homeomorphism of 
is nonincreasing
for any 
4 The proof of Theorem 1
In the following, we assume that
. For any 
small, we define the minimax value
for the perturbed functional
with
We now define a family of sets for the minimax procedure here. We essentially follow [3], also see [18] and [20]. Define

where
is given by Lemma 4. Note that
since
. Set

for
. From [20]
possess the following properties:
and
for all
.
If
is odd and
on
, then
for all
.
If
is open and
and
then 
Now, for
, we can define the minimax value
by

Lemma 8. For any
and
then
is well defined, and
where
is given by Lemma 5.
Proof. Consider the attracting domain of
in
:

Note that
is open since
is a local minimum of
and by the continuous dependence of ODE on initial data. Moreover,
is an invariant set, and
In particular, the following holds

for every
(see [3, Lemma 3.4]). Now we claim that for any
with
, it holds
(10)If this is true, then we have
and
because
and sup
by Lemma 5.
To prove (10), let

with
and
Define

Then
is a bounded open symmetric set with
and
Thus, it follows from the Borsuk–Ulam theorem that
and, by the continuity of
,
. As a consequence,

and therefore

by the “monotone, subadditive and supervariant” property of the genus [23, Prop. 5.4]. Since 

Thus for
, we conclude that

which proves (10).
Thus
is well defined for all
and 
The proof is complete.
Lemma 9.
(11)Proof. If not, we assume that

By Lemma 7, for the functional
, there exist
and a map
such that
is odd,
and
(12)By the definition of
, there exists
such that
. Let
It follows from (14) that

On the other hand, it is easy to show that
by Lemma 4 and the property (ii) of
above. As a result,
This contradicts with
. The proof is complete.
Lemma 9 implies that there exists a sign-changing critical point
such that

As a consequence of Lemma 8, we have that
is well defined for all
and
Now we can show the following lemma.
Lemma 10.
Proof. Here we deduce by a negation. Suppose
Since
satisfies Palais–Smale condition, it follows that
and is compact. Moreover, we have

Indeed, assume
is a sequence of sign-changing solutions to (6) with 
, and we have

By using the variantional principle of (5), we obtain

It follows that, by Sobolev embedding theorem,
where
is a constant independent of
This implies that the limit
of the subsequence of
is still sign-changing.
Assume
Since
and
is compact, by the “continuous” property of the genus [23, Prop. 5.4], there exists an open neighborhood
in
with 
such that
Now using Lemma 7 for the functional
, there exist
and a map
such that
is odd,
and
(13)Since
we can choose
sufficiently large such that
Clearly,
By the definition of
we can find a set
that is,
where
such that

for any
which implies
It follows from (13) that
(14)Let
Then
is symmetric and open, and

Then it is easy to check
by (ii) and (iii) above. As a result, by (14),

This is a contradiction to
. The proof is complete.
Lemma 11. For any fixed
is uniformly bounded with respect to
, and then
converges strongly to ul in
as
.
Proof. Indeed, by using the same
above, we can also define the minimax value for the following auxiliary function:

Here we choose
sufficiently large if necessary such that Lemma 4 also holds for
. Then by a
version of the mountain pass theorem [20, Thm. 9.2], for each
,
is well defined, and
because

where

Therefore, for any fixed
,
is uniformly bounded for 
, that is, there is
independent on
such that
uniformly for
because
is a nodal solution of (6) and
By the definition of
, we can obtain the following:

where
and
Therefore
is uniformly with respect to
. So we can apply Proposition 1 and obtain a subsequence
such that
strongly in
for some
and also
. Thus
is a solution of (5), and
. Moreover, since
is sign-changing, similar to Lemma 10, by Sobolev embedding theorem, we can prove that
is still sign-changing. The proof is complete.
Proof. Proof of Theorem 1 Noting that
is nondecreasing with respect to
, we have the following two cases:
Case I. There are
satisfying
Obviously, in this case, equation (1) has infinitely many sign solutions such that 
Case II. There is a positive integer
such that
for all
.
From now on we assume that there exists a
such that
has no sign-changing critical point
with

Otherwise, we are done. In this case, we claim that
, where 
and
Then as a consequence,
has infinitely many sign-changing critical points.
Now we adopt a technique in the proof of Theorem 1.1 in [7]. Suppose, on the contrary, that
(note that
). Moreover, we assume
contains only finitely many critical points, otherwise, we are done. Then it follows that
is compact. Obviously,
. Then there exists a open neighborhood
in
with 
such that
.
Define

We now claim that if
small,
has no sign-changing critical point
Indeed, arguing indirectly, suppose that there exist
and
satisfying
with
and 
Then, by Proposition 1, up to a subsequence,
converges strongly to
in
. Therefore
,

and
.
This is a contradiction to our assumption and the fact that u is still sign-changing. The following proof is similar to that of Lemma 9. By using Lemma 7, for the functional
, there exist
and a map
such that
is odd,
for
and
(15) Now fix
Since
we can find an
small such that
By the definition of
, we can find a set
that is,

where
such that

for any
, which implies
. Then by (15), we have
(16) Let
. Then
is symmetric and open, and

Then it is easy to check
by (ii) and (iii) above. As a result, by (16),

This contradicts to
. Then the proof for case II is finished. The proof is complete.
Acknowledgments
The first authors like to thank Chern Institute of Mathematics for visiting scholar programme and the authors are grateful to the anonymous referees for their useful suggestions, which improve the contents of this article.
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