We consider hyperbolic inequalities with Hardy potential
where is the unit ball in , , , , and f is a nontrivial -function. We study separately the cases: , and . For each case, we obtain an optimal criterium for the nonexistence of weak solutions. Our study yields naturally optimal nonexistence results for the corresponding stationary problem. The novelty of this work lies in two facts: (i) To the best of our knowledge, in all previous works dealing with nonexistence results for evolution equations with Hardy potential in a bounded domain, only the parabolic case has been investigated, making use of some comparison principles. (ii) To the best of our knowledge, in all previous works, the issue of nonexistence has been studied only in the case of positive solutions. In this paper, there is no restriction on the sign of solutions.
This work is concerned with the study of existence and nonexistence of weak solutions to hyperbolic inequalities with Hardy potential
where , , , , and , .
Problems of type (1) (with ) posed in have been considered in [8]. Namely, the authors studied the nonexistence of weak solutions to higher-order semilinear evolution inequalities of the form
where , , (a natural number) and . In particular, in the case and , it was shown that,
where and are the roots of the polynomial function
with . The proof of the above results is based on the test function method introduced by Mitidieri and Pohozaev (see e.g. [17]). Notice that in the case , we have , and then condition (i) reduces to
where is the Kato exponent obtained by Kato [15] for the hyperbolic inequality
Recently, in [13], the authors considered problem (1) (with ) posed in under an inhomogeneous Robin-type boundary condition. Namely, they investigated the existence and nonexistence of weak solutions to
where , , and . In the case , it was shown that,
if and , then for all , (3) admits no weak solution;
if and , then for all
(3) admits no weak solution;
The study of parabolic equations with hardy potential in a bounded domain was considered by some authors. For instance, in [3], the authors considered parabolic equations of the form
where , , is a bounded regular domain containing the origin, , , and , belong to a suitable class of functions. Namely, it was shown the existence of a critical exponent such that for , there is no distributional solution to (4), while for , and under some additional conditions on the data, (4) admits solutions. Notice that in [3], the positivity of u is essential in the proof of the obtained results. Moreover, in this reference, the authors used the comparison principle for the heat equation, which cannot be applied for our problem (1). For other contributions related to the study of parabolic equations with Hardy potential in a bounded domain, see e.g. [4,5,7,11,20] and the references therein. For the study of existence and nonexistence of solutions to elliptic equations involving Hardy potential, see e.g. [1,2,6,9,10] and the references therein.
From the above mentioned works, it is a natural question to ask about the critical behavior of hyperbolic inequalities involving hardy potential in a bounded domain. This motivates our study in the present paper.
Before stating our main results, we need to define weak solutions to (1). For , we denote by the closed ball centered at the origin with radius δ, i.e.,
Let
(Admissible test functions).
A function is said to be admissible, if it satisfies the following conditions:
(A1)
, .
(A2)
.
(A3)
, , where ν denotes the outward unit normal vector on .
We denote by the space of admissible functions.
(Weak solutions).
We say that is a weak solution to (1), if for all , we have
Multiplying (1) by φ, where , an integrating by parts, it can be easily seen that any smooth solution to (1) is a weak solution in the sense of Definition 1.2.
For , let
For , we introduce the parameter β given by
We first consider the case .
Letand.
Letbe such that. If, then for all, (
1
) admits no weak solution.
If, then for all, (
1
) admits positive solutions for some.
We next consider the case .
Letand.
Letbe such that. Then, for all(
1
) admits no weak solution.
If, then for all(
1
) admits positive solutions for some.
We now consider the case .
Letand.
Letbe such that. If, then for all(
1
) admits no weak solution.
If, then for all, (
1
) admits positive solutions for some.
If, then for all(
1
) admits positive solutions for some.
Let , , , and
For sufficiently small , one can check that
is a stationary solution to (1) with . This shows the necessity of the assumption in the nonexistence results given by Theorems 1.3, 1.4 and 1.5, when .
Theorems 1.3, 1.4 and 1.5 leave open the issue of existence and nonexistence in the following two cases:
and .
, and , where
Clearly, Theorems 1.3, 1.4 and 1.5 yield nonexistence results for the corresponding stationary problem
Let,,andwith.
Ifand, then for all, (
7
) admits no weak solution.
Letand. Then, for all(
7
) admits no weak solution.
In the proof of the existence results given by Theorems 1.3, 1.4 and 1.5 (see Section 3.2), we establish that (1) admits both stationary and time-dependent positive solutions for some . Hence, we also deduce the following existence results for (7).
Letand.
Ifand, then for all, (
7
) admits positive solutions for some.
Ifand, then for all(
7
) admits positive solutions for some.
Let.
If, then for all, (
7
) admits positive solutions for some.
If, then for all(
7
) admits positive solutions for some.
Let us say some words about our approach:
Our nonexistence results are based on suitable test functions and integral estimates. This technique was introduced by Mitidieri and Pohozaev (see e.g. [17,18]). Next, it was used by many authors for studying the nonexistence of solutions for various nonlinear problems posed in infinite domains (see e.g. [8,12–14,16,19]). For instance, in the case of the whole space, we often use a family of cut-off functions satisfying
Next, by a contradiction argument, using an a priori estimate and taking the limit as , we deduce the nonexistence of solutions. For problem (1), due to the boundedness of the domain, the above choice cannot be considered. To overcome this difficulty, we make use of test functions vanishing only in a neighborhood of the origin. Moreover, the considered test functions involve a function H satisfying
In the most previous works dealing with nonexistence results for nonlinear problems involving Hardy potential in a bounded domain, only the case of positive solutions has been treated. In this paper, there is no restriction on the sign of solutions.
Our existence results are established by the construction of explicit positive solutions to (1) for some .
The rest of the paper is organized as follows. In Section 2, we establish some preliminary results that will be useful in the proof of the above theorems. Namely, we first establish an a priori estimate for problem (1). Next, we introduce a certain class of admissible test functions specifically adapted to our problem and the considered bounded domain, and prove some useful estimates involving such functions. Finally, Section 3 is devoted to the proof of Theorems 1.3, 1.4 and 1.5. Namely, we first establish the nonexistence results (Section 3.1). Next, we prove the existence results (Section 3.2).
Throughout this paper, the symbol C denotes always a generic positive constant, which is independent of the scaling parameters T, R and the solution u. Its value could be changed from one line to another.
Preliminaries
Let , , , and .
A priori estimate
For any admissible function φ, let
and
We have the following a priori estimate.
Letbe a weak solution to (
1
). Then, for all, there holdsprovided that,.
Let be a weak solution to (1). In view of (5), we obtain
for all . Making use of Young’s inequality, we obtain
and
Thus, (10) follows from (11), (12) and (13). □
Admissible test functions
Let us introduce the radial function H defined in by
where the parameter β is given by (6). An elementary calculation shows that H is a nonnegative solution to
Let η and ξ be two cut-off functions satisfying:
and
For sufficiently large T, R and ℓ, let
and
that is,
We introduce test functions of the form
Properties (A1) and (A2) follow immediately from (15), (16), (17), (18) and (19). On the other hand, using that , we obtain
Next, for , it follows from (14) and (18) that
which yields
and
Hence, (20) and (21) show that condition (A3) is satisfied. Consequently, the function φ belongs to . □
Further estimates
We have
By (15) and (17), we obtain
which proves (22). On the other hand, observing that
we obtain
which proves (23). □
We have, as,
By (16) and (18), we obtain
On the other hand, by (14), we get
Thus, (24) follows from (25) and (26). □
We have, as, For sufficiently large ℓ, there holds, as,
Using (18) and taking in consideration that
we obtain
where “·” is the inner product in . Hence, by (16), it holds that
and
On the other hand, by (16), for , we obtain
Moreover, by (14), we have
Hence, using (28), (30), (31) and Cauchy–Schwartz inequality, we get
Next, using (14), (16), (29) and (32), we obtain
which proves (27). □
The following estimate follows immediately form (8), (19), (23) and Lemma 2.4.
We havewhere φ is the test function given by (
19
).
The following estimate follows immediately form (9), (19), (22) and Lemma 2.5.
We havewhere φ is the test function given by (
19
).
Proofs of the main results
In this section, we prove Theorems 1.3, 1.4 and 1.5.
Proofs of the nonexistence results
We argue by contradiction by supposing that is a weak solution to (1). Then, by Lemma 2.1, (10) holds for any admissible function φ. For sufficiently large T, R and ℓ, let φ be the test function given by (19). Since by Lemma 2.2, there holds
On the other hand, in view of (15), (17) and (21), we obtain
Using the change of variable , we get
Thus, combining (34) with (35), we obtain
Moreover, by Lemmas 2.6 and 2.7, we have
where
Hence, it follows from (33), (36) and (37) that
that is,
Since , by (6), we have . Then, by (38), and (39) reduces to
Taking in the above estimate, we obtain
Since , passing to the limit as in (40), we get , which contradicts the condition . Consequently, for all , no weak solution exists. This proves part (I) of Theorem 1.3. □
As previously, let us suppose that is a weak solution to (1). Following exactly the same argument used in the proof of part (I) of Theorem 1.3, we obtain (39). Since , then by (6), we have . Then, by (38), and (39) reduces to
Taking in the above inequality, we obtain
Case 1: .
In this case, taking in consideration that , we deduce that
Hence, passing to the limit as in (42), we obtain a contradiction with .
Case 2: and .
As in Case 1, (43) holds. Thus, proceeding as above, we reach a contradiction with .
Consequently, in both cases, no weak solution exists, which proves part (I) of Theorem 1.4. □
Again, we suppose that is a weak solution to (1). Then, the estimate (39) holds. Since , then by (6), we have . Thus, we have three possible cases.
Case 1: .
In this case, by (38), and (39) reduces to (41). Taking in (41), we obtain (42). Hence, if and , then (43) holds. Thus, passing to the limit as in (42), we obtain a contradiction with .
Case 2: .
In this case, by (38), and (39) reduces to
Proceeding as above, taking in the above estimate and passing to the limit as , under the condition and , a contradiction with follows.
Case 3: .
In this case, by (38), and (39) reduces to
Taking in the above estimate, where
we get
Notice that, since , and , then . Passing to the limit as in (44), we reach a contradiction with .
Thus, in all the above cases, no weak solution exists. This completes the proof of part (I) of Theorem 1.5. □
Proof of the existence results
Let us introduce the functional space
It is not difficult to show that . For instance, the function defined by
belongs to Λ.
The following lemma will be used later in the proof of our existence results.
Assume thatis a stationary positive solution to (
1
) for some. Let. Thenis a positive solution to (
1
) with, where.
Let be a positive solution to
and
where . Let and
Then, using (45), (46) and the properties of the function ρ, we obtain
and
Hence, by (47) and (48), we deduce that u is a positive solution to (1) with . □
Let and . Let
where
and
Notice that, since , and , the set of δ satisfying (50) is nonempty. Moreover, by (50), we have , which shows that the set of ϵ satisfying (51) is nonempty. An elementary calculation shows that
Hence, using (50) and (51), we obtain
This shows that ϑ is a stationary positive solution to (1) with . Then, by Lemma 3.1, we deduce that for any function , functions of the form
are positive solutions to (1) with . This proves part (II) of Theorem 1.3. □
Let , and
Consider functions ϑ of the form (49), where
and
Notice that, since (so ) and p satisfies (53), the set of δ satisfying (54) is nonempty. Moreover, by (54), we have , which shows that the set of ϵ satisfying (55) is nonempty. An elementary calculation shows that
Hence, in view of (54) and (55), we obtain
Then, ϑ is a stationary positive solution to (1) with . Thus, by Lemma 3.1, we deduce that for any function , functions of the form (52) are positive solutions to (1) with . This proves part (II) of Theorem 1.4. □
(i) Let and . Consider functions ϑ of the form (49), where
and the parameter ϵ satisfies (55). Observe that, since (so ), the set of δ satisfying (57) is nonempty. Moreover, by (57), we have , which shows that the set of ϵ satisfying (55) is nonempty. Hence, using (55), (56), (57), and taking in consideration that , we obtain
which proves that ϑ is a stationary positive solution to (1) with . Hence, for any function , functions of the form (52) are positive solutions to (1) with .
(ii) Let , and
In this case, we consider functions ϑ of the form (49), where
and the parameter ϵ satisfies (55). Notice that, due to (58) and the fact that , the set of δ satisfying (59) is nonempty. Moreover, due to (59), the set of ϵ satisfying (55) is nonempty. Proceeding as in the case (i), we obtain that for any function , functions of the form (52) are positive solutions to (1) with . Then, part (II) of Theorem 1.5 is proved. □
Footnotes
Acknowledgement
The first author is supported by Researchers Supporting Project number (RSP2023R57), King Saud University, Riyadh, Saudi Arabia.
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