Abstract
In this paper we study the existence of even positive homoclinic solutions for p-Laplacian ordinary differential equations (ODEs) of the type
, where
,
and the functions a and b are strictly positive and even. First, we prove a result on symmetry of positive
solutions of p-Laplacian ODEs. Then, using the mountain-pass theorem, we prove the existence of
symmetric positive homoclinic solutions of the considered equations. Some examples
and additional comments are given.
MSC: 34B18, 34B40, 49J40.
Keywords:
p-Laplacian ODEs; homoclinic solution; weak solution; Palais-Smale condition; mountain-pass theorem1 Introduction and main results
In this paper we prove the existence of positive homoclinic solutions for p-Laplacian ODEs of the type
(H) the functions
are
are continuously differentiable, strictly positive,
and
. Let, moreover,
and
be even functions on ℝ,
and
for
.
By a solution of (1), we mean a function
such that
,
and Eq. (1) holds for every
. We are looking for positive solutions of (1) which are homoclinic, i.e.,
and
as
.
In the case
,
and
, similar problems are considered in [1-3] using variational methods. Note that in [2] and [3] the following second-order differential equations are considered:
and
where a, b and c are periodic, bounded functions and a and c are positive. These equations come from a biomathematics model suggested by Austin [4] and Cronin [5]. Further results and the phase plane analysis of these equations with constant coefficients are given in [6]. Note that the periodic and homoclinic solutions of p-Laplacian ODEs are considered in [7,8].
The present work is an extension of these studies to p-Laplacian ODEs. Let
be the Sobolev space of p-integrable absolutely continuous functions
such that
We use a variational treatment of the problem considering the functional 
Using the well-known mountain-pass theorem, we conclude that the functional
has a nontrivial critical point
, which is a solution of the restricted problem
Further, we obtain uniform estimates for the solutions
, extended by 0 outside
. Then, a positive homoclinic solution
of (1) is found as a limit of
, as
in
. The function
is also an even function.
To obtain the property, we extend the symmetry lemma of Korman and Ouyang [9] to the p-Laplacian equations. The result is formulated and proved in Section 2.
Our main result is:
Theorem 1Suppose that
,
and assumptions (H) hold. Then Eq. (1) has a positive solution
such that
and
as
. Moreover, the solution
is an even function,
as
and
for
.
Theorem 1 is proved in Section 3. From its proof we have
from which it follows that
as
. Observe that if
, the problem

has a unique solution
. Indeed, multiplying the equation by u and integrating by parts over ℝ, we obtain
A simplified method can be applied to the equations
under assumptions (H) and
,
. Note that in this case, the even homoclinic solution
of Eq. (3) satisfies
and again
as
. If a and b are constants, Eq. (3) is a conservative system and one can plot the phase curves
in the phase plane
. An example is given at the end of Section 3.
2 Preliminary results
Let
,
and
. It is clear that
is a differentiable function and
. Moreover,
exists and
for
.
Let
,
be the space of Lebesgue measurable functions
such that the norm
.
The dual space of
is
, where
. Let
be the duality pairing between
and
. By the Hölder inequality,
for any
and
. We will use the following lemmata in further considerations.
Lemma 2For any
, the following inequality holds:
Proof of Lemma 2. Note that for
,
. From the Hölder inequality, we have

□
The statement of Lemma 3 follows simply from the identity
The one-dimensional p-Laplacian operator
for a differentiable function u on the interval I is introduced as
. Let us consider the problem
A function
is said to be a solution of the problem (4) if
with
is such that
is absolutely continuous and
holds a.e. in
.
We formulate an extension of Lemma 1 of [9] for p-Laplacian nonlinear equations. The result of Korman and Ouyang is one-dimensional analogue of the result of Gidas, Ni and Nirenberg [10] for symmetry of positive solutions of semilinear Laplace equations. In the case of p-Laplacian equations, the symmetry of solutions in higher dimensions is discussed by Reihel and Walter [11].
Theorem 4Assume that
satisfies (5). Then any positive solutionuof (4) is an even function such that
and
for
.
Remark 1 Let us note that if the function f satisfies (5), but u is not a positive solution of (4), then u is not necessarily an even function. A simple counter example in the case
is the problem
The term
satisfies (5) in the interval
, but the solution of the problem
is negative in
and not an even function. Its graph is presented in Figure 1. It would be more interesting to show an example for the case
and f satisfying the additional assumption
.
Figure 1. Graph of the functions
.
Sketch of Proof of Theorem 4 Suppose that the function u has only one global maximum on
.
Assume that the function
has a finite number of local minima in the interval
, and let
be the largest local minimum. Let
be the local maximum and
be such that
. Denote
and
, and let
and
be the inverse functions of the function
in the intervals
and
, respectively. Multiplying the equation in (4) by
and integrating in
, we obtain by Lemma 3 and (5):
which leads to contradiction. One can prove the last fact using other arguments;
see, for instance, Theorem 2.1 of [12]. Suppose now that u has infinitely many local minima in
. Further, we can follow the steps of the proof of Lemma 1 of [9] with corresponding modifications based on Lemma 3. □
3 Proof of the main result
Let
be the Sobolev space of p-integrable absolutely continuous functions
such that
and
. Note that if
is strictly positive and bounded, i.e., there exist a and A such that
, then
is an equivalent norm in
.
We need an extension to the p-case of the following proposition by Rabinowitz [13].
Proof of Proposition 5 Let
. It follows
Integrating with respect to
and using the Hölder and Jensen inequalities, we obtain
(ii) Take
. Since
, there exists
such that by (i)
□
We are looking for positive solutions of (1), which are homoclinic, i.e.,
and
as
. Firstly, we look for positive solutions of the problem

A function
is said to be a solution of the problem (
) if
with
is such that
is absolutely continuous and
holds a.e. in
.
A function
is said to be a weak solution of the problem (
) if
Standard arguments show that a weak solution of the problem (
) is a solution of (
) (see [14] and [15]). Consider the modified problem

where
. It is easy to see that solutions of the problem (
) are positive solutions of the problem (
). Indeed, if
is a solution of (
) and
has negative minimum at
, since for
,
, by the equation
, we reach a contradiction
Then
and u is a solution of (
). We use a variational treatment of the problem (
), considering the functional 
Critical points of
are weak solutions of (
), i.e.,
and, by a standard way, they are solutions of (
). We show that
satisfies the assumptions of the mountain-pass theorem of Ambrosetti and Rabinowitz
[16].
Theorem 6 (Mountain-pass theorem)
LetXbe a Banach space with norm
,
,
andIsatisfy the (PS) condition. Suppose that there exist
,
and
such that
Thencis a critical value ofI, i.e., there exists
such that
and
.
Next, denote by
several positive constants.
Lemma 7Let
,
and assumptions (H) hold. Then for every
, the problem (
) has a positive solution
. Moreover, there is a constant
, independent ofT, such that
ProofStep 1.
satisfies the (PS) condition.
Let
be a sequence, and suppose there exist
and
such that for 
and
Let us denote
. From (9) and (10), it follows that
and
Then
and
We have
which implies that the sequence
is bounded in
. By the compact embedding
, there exist
and the subsequence of
, still denoted by
, such that
weakly in
and
strongly in
. We will show that
strongly in
using Lemma 2. By uniform convergence of
to u in
, it follows that

and
Then
and by Lemma 2,
which implies that
. Then
and by the uniform convexity of the space
, it follows that
, as
.
Step 2. Geometric conditions.
Obviously,
. By assumption (H) it follows
Let
be such that
if
and also
. Consider the function
Then
for μ large enough.
By the mountain-pass theorem, there exists a solution
such that
where
Moreover, using the variational characterization (11), we have
Therefore,
is a nontrivial and positive solution of (
). By Theorem 4,
and
for
.
Step 3. Uniform estimates.
Let
. By continuation with zero of a function
to
, we have
and
. Using the variational characterization (11), we infer that
and then
Multiplying the equation of (
) by
and integrating by parts, we have
Then by (12),
We get (8) with
, which completes the proof. □
Proof of Theorem 1 Take
and let
be the solution of the problem (
) given by Lemma 2. Consider the extension of
to ℝ with zero outside
and denote it by the same symbol.
Claim 1. The sequence of functions
is uniformly bounded and equicontinuous.
By (8) and the embedding of
in
, there is
such that
. Then by the equation of (
), it follows that
By the mean value theorem for every natural n and every
, there exists
such that
Then, as a consequence of (13), we obtain
from which it follows
and the sequence of functions
is equicontinuous. Further, we claim that the sequence
is also equicontinuous.
Claim 2. The sequence of functions
is equicontinuous.
To prove this statement, we follow the method given by Tang and Xiao [7]. For completeness, we present it in details.
Suppose that
is not an equicontinuous sequence in
. Then there exist an
and sequences
and
such that
and
By (14), there are numbers
and
and the subsequence
such that
and
as
. By (15),
. On the other hand, by (13) we have
Then passing to a limit as
, we obtain
. Hence,
which contradicts
. Thus, the sequence
is equicontinuous.
Let
. By Claim 1 and Claim 2 and the Arzelà-Ascoli theorem, there is a subsequence of
, still denoted by
, and functions
and
of
such that
and
. Trivially, it follows that
,
and
. Repeating this procedure as in [7], we obtain that there is a subsequence of
, still denoted by
, and
such that
in
. The function
satisfies Eq. (1). Indeed, let
be an interval of ℝ and
such that
. By the above considerations, taking a limit as
in the equation
equivalent to
we obtain
and hence
Since
and
are arbitrary,
is a solution of (1). Moreover, we have
It remains to show that
is nonzero and
and
.
By Theorem 4,
is an even function and attains its maximum at 0. Then by Eq. (1),
By assumption (H)
independently of n. Hence, passing to a limit as
, we obtain
From (16) and Proposition 5, it follows
(17)Now, we will show that
. The arguments for
are similar.
If
, there exist
and a monotone increasing sequence
such that
. Then for
,
which contradicts (16).
Moreover, u is an even function that attains its only maximum at 0, since the same holds for
the functions
. Arguing as in the proof of Theorem 4, we easily obtain that
if
. □
Remark 2 A simplified method can be applied to the equations
under assumptions (H) and
,
. Namely, first one looks for the even positive solutions
of the problem
where
is the Sobolev space of square integrable functions such that
Since
is a Hilbert space, compactly embedded in
the proof of the (PS)-condition is easier. Similar considerations are made in [1] and [3]. Then, the even homoclinic solution
is obtained as a
limit of the sequence
. Note that in this case, the even homoclinic solution
of Eq. (3) satisfies
and again
as
. If a and b are constants, Eq. (3) is a conservative system and one can plot the phase curves
in the phase plane
. Consider the equation
. The phase portrait in a
plane, for
in the rectangle
, is plotted on Figure 2.
Figure 2. Phase portrait of
, in
.
Competing interests
The author declares that he has no competing interests.
Acknowledgements
Dedicated to Professor Jean Mawhin on the occasion of his 70th anniversary.
The author thanks Prof. Alberto Cabada and Prof. Luis Sanchez for helpful remarks concerning Theorem 4. The author would like to thank the Department of Mathematics and Theoretical Informatics at the Technical University of Kosice, Slovakia, where the paper was prepared during his visit on the SAIA Fellowship programme. The author is thankful to the editor and anonymous referee for their comments and suggestions on the article.
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