 Research
 Open Access
 Published:
Fast homoclinic solutions for damped vibration problems with superquadratic potentials
Boundary Value Problems volume 2018, Article number: 183 (2018)
Abstract
In this paper we investigate the existence and multiplicity of homoclinic solutions for the following damped vibration problem:
where \(q:\mathbb{R}\rightarrow\mathbb{R}\) is a continuous function, \(L\in C(\mathbb{R}, \mathbb{R}^{n^{2}})\) is a symmetric and positive definite matrix for all \(t\in\mathbb{R}\) and \(W\in C^{1}(\mathbb{R}\times\mathbb{R}^{n}, \mathbb{R})\). The novelty of this paper is that, assuming \(\lim_{t\rightarrow+\infty }Q(t)=+\infty\) (\(Q(t)=\int_{0}^{t} q(s) \,ds\)) and L is coercive at infinity, we establish one new compact embedding theorem. Subsequently, supposing that W satisfies the global Ambrosetti–Rabinowitz condition, we obtain some new criterion to guarantee the existence of homoclinic solution of (DS) using the mountain pass theorem. Moreover, if W is even, then (DS) has infinitely many homoclinic solutions. Recent results in the literature are generalized and significantly improved.
Introduction
The purpose of this work is to deal with the existence of homoclinic solutions for the following damped vibration problem:
where \(q:\mathbb{R}\rightarrow\mathbb{R}\) is a continuous function such that
with \(Q(t)=\int_{0}^{t} q(s)\,ds\), \(L\in C(\mathbb{R}, \mathbb{R}^{n^{2}})\) is a symmetric and positive definite matrix for all \(t\in\mathbb{R}\) and \(W\in C^{1}(\mathbb{R}\times\mathbb{R}^{n}, \mathbb{R})\).
When \(q(t)\equiv0\), (DS) is just the following second order Hamiltonian system:
It is well known that the existence of homoclinic solutions for Hamiltonian systems and their importance in the study of the behavior of dynamical systems have been recognized from Poincaré [16]. They may be “organizing centers” for the dynamics in their neighborhood. From their existence one may, under certain conditions, infer the existence of chaos nearby or the bifurcation behavior of periodic orbits. In the past two decades, with the works of [15] and [18], variational methods and critical point theory have been successfully applied for the search of the existence and multiplicity of homoclinic solutions of (HS). Assuming that \(L(t)\) and \(W(t,u)\) are independent of t or Tperiodic in t, many authors have studied the existence of homoclinic solutions for the Hamiltonian system (HS) (see, for instance, [3, 6, 8, 18, 26] and the references therein) and some more general Hamiltonian systems are considered in the recent papers [10, 12, 22]. In this case, the existence of homoclinic solutions can be obtained by going to the limit of periodic solutions of approximating problems.
If \(L(t)\) and \(W(t,u)\) are neither autonomous nor periodic in t, the existence of homoclinic solutions of (HS) is quite different from the periodic systems because of the lack of compactness of the Sobolev embedding, see for instance [1, 11, 15, 19] and the references therein. It is worthy of pointing out that to obtain the existence of homoclinic solutions of (HS), the following socalled global Ambrosetti–Rabinowitz condition ((AR) condition, see (\(\mathrm{W}_{1}\)) below) on W due to Ambrosetti–Rabinowitz (e.g., [2]) is assumed in the works mentioned above, which implies that \(W(t,u)\) is of superquadratic growth as \(u\rightarrow+\infty\). However, there are lots of potentials which are superquadratic as \(u\rightarrow+\infty\) but do not satisfy the (AR) condition. Therefore, many authors have been focusing their attention on obtaining the existence of homoclinic solutions under the conditions weaker than the (AR) condition, see for instance [7, 13, 14, 23, 32] and the references listed therein. In addition, to verify the (PS) condition for the corresponding energy functional of (HS), the following coercive assumption on L is often needed:
 (L):

\(L\in C(\mathbb{R}, \mathbb{R}^{n^{2}})\) is a symmetric and positive definite matrix for all \(t\in\mathbb{R}\), and there is a continuous function \(\beta:\mathbb{R}\rightarrow\mathbb{R}\) such that \(\beta(t)>0\) for all \(t\in\mathbb{R}\) and \((L(t)u,u)\geq\beta(t)u^{2}\) and \(\beta(t)\rightarrow+\infty\) as \(t\rightarrow+\infty\),
which indicates that the smallest eigenvalue \(l(t)\) of \(L(t)\) is coercive, i.e.,
where \(l(t):=\inf_{u=1}(L(t)u,u)\), \((\cdot,\cdot):\mathbb {R}^{n}\times\mathbb{R}^{n}\rightarrow\mathbb{R}\) denotes the standard inner product in \(\mathbb{R}^{n}\) and subsequently \(\cdot\) is the induced norm.
Compared with the literature available for \(W(t,u)\) being superquadratic as \(u\rightarrow+\infty\), the study of the existence of homoclinic solutions of (HS) under the assumption that \(W(t,u)\) is subquadratic at infinity is much more recent and the number of references is considerably smaller, see for instance [8, 20, 21, 28, 29], where some other types of coercive conditions on L are also utilized. In addition, the existence of homoclinic solutions under the condition that \(W(t,u)\) is asymptotically quadratic at infinity has also been investigated by many researchers, see for instance [9, 24, 30, 32].
As far as the case that \(q(t)\neq0\) is concerned, to our best knowledge, there is little research about the existence of homoclinic solutions of (DS). In the recent paper [31], for the first time the authors investigated the existence of fast homoclinic solutions for the following special case of (DS):
with W (\(W(t,u)=a(t)u^{\gamma}\), \(1<\gamma<2\)) is subquadratic at infinity and \(c\geq0\) via a standard minimizing argument, which has been improved in [4] where, using the genus property in critical point theory, the authors considered the case that q satisfies (1.1) and \(W(t,u)\) is of subquadratic growth and obtained the existence of infinitely many fast homoclinic solutions of (DS). In addition, in [25], the authors studied the existence of solutions for the following damped vibration problems:
using the variational methods, where \(Q(T)=\int_{0}^{T}q(s)\,ds\).
Motivated by the above papers, in this paper we use the mountain pass theorem to establish some new criterion to guarantee (DS) has infinitely many fast homoclinic solutions for the case that W satisfies the (AR) condition. In the following, in order to introduce the concept of fast homoclinic solutions of (DS) conveniently, we firstly describe some properties of the weighted Sobolev space E on which the energy functional associated with (DS) is defined. Letting
where \(Q(t)\) is defined in (1.1), and for any u, \(v\in E\), define
Then the space E is a Hilbert space with the above inner product, and the corresponding norm is
Here, \(H^{1}(\mathbb{R}, \mathbb{R}^{n})\) denotes the Banach spaces of functions on \(\mathbb{R}\) with values in \(\mathbb{R}^{n}\) under the norm
Throughout this paper, we adopt the definition of [4] for fast homoclinic solution of (DS):
Definition 1.1
If (1.1) holds, a solution u of (DS) is called a fast homoclinic solution if \(u\in E\).
In what follows, we can state our main result. For the convenience of statement, \(W(t,u)\) is assumed to satisfy the following conditions:
 (\(\mathrm{W}_{1}\)):

There is a constant \(\mu>2\) such that, for every \(t\in \mathbb{R}\) and \(u\in\mathbb{R}^{n}\backslash \{0 \}\),
$$0< \mu W(t,u)\leq\bigl(W_{u}(t,u),u\bigr); $$  (\(\mathrm{W}_{2}\)):

\(W_{u}(t,u)=o(u)\) as \(u\rightarrow0\) uniformly with respect to \(t\in\mathbb{R}\);
 (\(\mathrm{W}_{3}\)):

There exists \(\overline{W}\in C(\mathbb{R}^{n}, \mathbb {R})\) such that \(W_{u}(t,u)\leq\overline{W}(u)\) for every \(t\in\mathbb{R}\) and \(u\in\mathbb{R}^{n}\).
Theorem 1.2
Suppose that (1.1), (L), and (\(\mathrm{W}_{1}\))–(\(\mathrm{W}_{3}\)) are satisfied, then (DS) has at least one nontrivial fast homoclinic solution. Moreover, if we assume that \(W(t,u)\) is even in u, i.e.,
 (\(\mathrm{W}_{4}\)):

\(W(t,u)=W(t,u)\) for all \(t\in\mathbb{R}\) and \(u\in\mathbb{R}^{n}\),
then (DS) possesses infinitely many distinct fast homoclinic solutions.
Remark 1.3
In (DS), if \(q(t)\equiv0\), then Theorem 1.2 (under the same hypothesis on L and \(W(t,u)\)) reaches the results in [15](see its Theorem 1 and Theorem 2). Therefore, we extend the results of [15] for (HS) to the more general situations (DS).
It is worth pointing out that an open problem was proposed in [31], explicitly, how to obtain the existence of fast homoclinic solutions of (1.3) for the case that W satisfies the (AR) condition using the mountain pass theorem. Here, Theorem 1.2 gives some partial answer to this open problem. For some recently related results, we refer the reader to [5, 27].
Remark 1.4
From (L), it is easy to obtain that there exists a constant \(\beta>0\) such that
(\(\mathrm{W}_{1}\)) is called the global Ambrosetti–Rabinowitz condition due to Ambrosetti and Rabinowitz (see [2]), which implies that
In fact, it suffices to show that for every \(u\neq0\) and \(t\in\mathbb {R}\) the function \((0,+\infty)\ni\xi\rightarrow W(t,\xi^{1}u)\xi ^{\mu}\) is nonincreasing, which is an immediate consequence due to (\(\mathrm{W}_{1}\)). Moreover, choose \(\eta(t)=\min_{u=1}W(t,u)>0\), one has
for every \(t\in\mathbb{R}\) and \(u\geq1\). In addition, by (\(\mathrm{W}_{1}\)) and (\(\mathrm{W}_{2}\)), we have \(W(t,u)=o(u^{2})\) as \(u\rightarrow0\) uniformly with respect to \(t\in\mathbb{R}\), i.e., for any \(\epsilon>0\), there is \(\delta>0\) such that
Furthermore, by (\(\mathrm{W}_{2}\)) and (\(\mathrm{W}_{3}\)), for any \(u\in\mathbb{R}^{n}\) such that \(u\leq r\), there exists some constant d (dependent on r) such that
In what follows, we present some examples for \(q(t)\), \(L(t)\), and \(W(t,u)\) satisfying (1.1), (L), and (\(W_{1}\))–(\(\mathrm{W}_{3}\)) to demonstrate our Theorem 1.2. Let us choose
where \(I_{n}\) is the \(n\times n\) identity matrix and \(\mu>2\) is a constant. Then it is easy to check that all the hypotheses of Theorem 1.2 are satisfied.
The remaining part of this paper is organized as follows. Some preliminary results are presented in Sect. 2. In Sect. 3, we are devoted to accomplishing the proof of our main result.
Preliminary results
The main difficulty in dealing with the existence of infinitely many homoclinic solutions for (DS) is the lack of compactness of the Sobolev embedding. To overcome this difficulty under the assumptions of Theorem 1.2, we employ the following compact embedding theorem. For the statement convenience, define the function space \(L^{2}(e^{Q(t)})\) as the Banach space of functions on \(\mathbb{R}\) with values in \(\mathbb{R}^{n}\) under the norm
It is obvious that \(E\subset L^{2}(e^{Q(t)})\) with the embedding continuous, i.e., there is a constant \(C>0\) such that
In fact, we have the following compact embedding lemma.
Lemma 2.1
Suppose that (1.1) holds and L satisfies (L), then the embedding of E in \(L^{2}(e^{Q(t)})\) is compact.
Proof
For any \(R>0\), define
By (L), \(\zeta(R)\rightarrow+\infty\) as \(R\rightarrow+\infty\).
Let \(K\subset E\) be a bounded set, then there exists some \(M>0\) such that \(\u\\leq M\) for all \(u\in K\). We show that K is precompact in \(L^{2}(e^{Q(t)})\). For any \(\epsilon>0\), take \(R_{0}\) large enough such that
By the Sobolev compact embedding theorem, \(E_{(R,R)}\) is compactly embedded in \(L^{2}(e^{Q(t)})_{(R,R)}\) for all \(R>0\). Hence, there are \(u_{1}, \dots, u_{m}\in K\) such that, for any \(u\in K\), there is \(u_{i}\) (\(1\leq i\leq m\)) satisfying
and so
which implies that K has a finite ϵnet and, consequently, it is precompact in \(L^{2}(e^{Q(t)})\). □
In order to obtain the existence of homoclinic solutions of (DS), we also need the following inequality. Denote by \(L^{\infty}(\mathbb{R}, \mathbb {R}^{n})\) the Banach space of essentially bounded functions from \(\mathbb{R}\) into \(\mathbb{R}^{n}\) equipped with the norm
Then we have
Lemma 2.2
([4, Lemma 2.1])
For \(u\in E\), one has
where β is defined in (1.5) and \(e_{0}=\min_{t\in\mathbb{R}} e^{Q(t)}\).
Now we introduce more notations and some necessary definitions. Let \(\mathcal{B}\) be a real Banach space, \(I\in C^{1}(\mathcal{B}, \mathbb {R})\), which means that I is a continuously Fréchetdifferentiable functional defined on \(\mathcal{B}\). Recall that \(I\in C^{1}(\mathcal{B}, \mathbb{R})\) is said to satisfy the (PS) condition if any sequence \(\{u_{j} \}_{j\in\mathbb{N}}\subset\mathcal{B}\), for which \(\{I(u_{j}) \}_{j\in\mathbb{N}}\) is bounded and \(I'(u_{j})\rightarrow0\) as \(j\rightarrow+\infty\), possesses a convergent subsequence in \(\mathcal{B}\).
Moreover, let \(B_{\rho}\) be the open ball in \(\mathcal{B}\) with the radius ρ and centered at 0 and \(\partial B_{\rho}\) denote its boundary. To obtain the existence and multiplicity of fast homoclinic solutions of (DS), we appeal to the following wellknown mountain pass theorem, see [17].
Lemma 2.3
([17, Theorem 2.2 ])
Let \(\mathcal{B}\) be a real Banach space and \(I\in C^{1}(\mathcal{B}, \mathbb{R})\) satisfying the (PS) condition. Suppose that \(I(0)=0\) and

(A1)
there are constants ρ, \(\alpha>0\) such that \(I_{\partial B_{\rho}}\geq\alpha\), and

(A2)
there is \(e\in\mathcal{B}\setminus\overline {B}_{\rho}\) such that \(I(e)\leq0\).
Then I possesses a critical value \(c\geq\alpha\). Moreover, c can be characterized as
where
Lemma 2.4
([17, Theorem 9.12])
Let \(\mathcal{B}\) be an infinite dimensional real Banach space, and let \(I\in C^{1}(\mathcal{B}, \mathbb{R})\) be even, satisfy the (PS) condition and \(I(0)=0\). If \(\mathcal{B}=V\oplus X\), where V is finite dimensional and I satisfies
 (A3):

there are constants ρ, \(\alpha>0\) such that \(I_{\partial B_{\rho}\cap X}\geq\alpha\), and
 (A4):

for each finite dimensional subspace \(\tilde {E}\subset\mathcal{B}\), there is \(R=R(\tilde{E})\) such that \(I\leq 0\) on \(\tilde{E}\backslash B_{R(\tilde{E})}\),
then I has an unbounded sequence of critical values.
Proof of Theorem 1.2
Now we are going to establish the corresponding variational framework to obtain fast homoclinic solutions of (DS). To this end, define the functional \(I:\mathcal{B}=E\rightarrow\mathbb{R}\) by
Lemma 3.1
Under the conditions of Theorem 1.2, we have
for all u, \(v\in E\), which yields that
Moreover, I is a continuously Fréchetdifferentiable functional defined on E, i.e., \(I\in C^{1}(E, \mathbb{R})\).
Proof
We firstly show that \(I:E\rightarrow\mathbb{R}\). By (1.8), there exist constants \(R_{1}>0\) and \(M>0\) such that
Letting \(u\in E\), then \(u\in C^{0}(\mathbb{R}, \mathbb{R}^{n})\), the space of continuous functions u on \(\mathbb{R}\) such that \(u(t)\rightarrow0\) as \(t\rightarrow+\infty\), i.e., \(E\subset C^{0}(\mathbb{R}, \mathbb{R}^{n})\). Therefore, there is a constant \(R_{2}>0\) such that \(t\geq R_{2}\) implies that \(u(t)\leq R_{1}\). Hence, by (3.3), we have
Combining (3.1) and (3.4), we show that \(I:E\rightarrow\mathbb{R}\).
Next we prove that \(I\in C^{1}(E, \mathbb{R})\). Rewrite I as follows:
where
It is easy to check that \(I_{1}\in C^{1}(E, \mathbb{R})\), and we have
Thus it is sufficient to show that this is the case for \(I_{2}\). In the process we see that
which is defined for all u, \(v\in E\). Let \(u\in E\) and suppose the norm of u is M, i.e., \(\u\=M\). Then, by (\(\mathrm{W}_{2}\)), for any \(\epsilon>0\), there is \(\delta>0\) such that \(x\leq\delta\) implies that
where C is defined in (2.1). It is well known that
for any finite R. Therefore, there is \(\sigma=\sigma(\epsilon, R, u)\) such that \(v\in E\) and \(\v\\leq\sigma\) implies that
Choose R so large that \(u(t)\leq\delta/2\) for \(t\geq R\). For \(v\in E\), \(\v\\leq\min\{\sqrt{e_{0}\sqrt{\beta}}\delta/\sqrt {2},1\}\), by (2.4), we have
Therefore,
The mean value theorem, (3.6), and (3.9) show that, for \(t\geq R\),
Hence, by (2.1) and Hölder’s inequality, one deduces that
Likewise, by (3.6) and Hölder’s inequality, we obtain
which together with (3.8) and (3.10) yields the Fréchet differentiability of \(I_{2}\). To prove that \(I'_{2}\) is continuous, suppose that \(u_{j}\rightarrow u\) in E and note that
Let \(\epsilon>0\) and choose R so that \(t\geq R\) implies that
Moreover, we can also assume (3.12) holds for \(u_{j}\) for large j. Therefore, by (3.12), one has
which with (3.11) implies that \(I_{2}'\) is continuous. Therefore, we show that \(I\in C^{1}(E, \mathbb{R})\). □
Lemma 3.2
Suppose that (L), (\(\mathrm{W}_{2}\)), and (\(\mathrm{W}_{3}\)) are satisfied. If \(u_{j}\rightharpoonup u\) (weakly) in E, then there exists one subsequence still denoted by \(\{u_{j}\}_{j\in\mathbb{N}}\) such that \(W_{u}(t,u_{j})\rightarrow W_{u}(t,u)\) in \(L^{2}(e^{Q(t)})\).
Proof
Assume that \(u_{j}\rightharpoonup u\) in E. Then there exists a constant \(M>0\) such that, by the Banach–Steinhaus theorem and (2.4),
which combined with (1.9) deduces that there is a constant d (dependent on M) such that
for all \(j\in\mathbb{N}\) and \(t\in\mathbb{R}\). Hence, we have
On the other hand, by Lemma 2.1, \(u_{j}\rightarrow u\) in \(L^{2}(e^{Q(t)})\), which yields that there exists one subsequence, still denoted by \(\{u_{j}\}_{j\in\mathbb{N}}\) such that
Therefore, \(u_{j}(t)\rightarrow u(t)\) for almost every \(t\in\mathbb{R}\) and
Consequently, we have
Using Lebesgue’s convergence theorem, the lemma is proved. □
Lemma 3.3
If (L), (\(\mathrm{W}_{1}\)), (\(\mathrm{W}_{2}\)), and (\(\mathrm{W}_{3}\)) hold, then I satisfies the (PS) condition.
Proof
Assume that \(\{u_{j} \}_{j\in\mathbb{N}} \subset E\) is a sequence such that \(\{I(u_{j}) \}_{j\in \mathbb{N}}\) is bounded and \(I'(u_{j})\rightarrow0\) as \(j\rightarrow+\infty\). Then there exists a constant \(M>0\) such that
for every \(j\in\mathbb{N}\).
We firstly prove that \(\{u_{j} \}_{j\in\mathbb{N}}\) is bounded in E. By (3.1), (3.13), and (\(\mathrm{W}_{1}\)), we obtain that
Since \(\mu>2\), inequality (3.14) shows that \(\{ u_{j} \}_{j\in\mathbb{N}}\) is bounded in E. Then the sequence \(\{u_{j} \}_{j\in\mathbb{N}}\) has a subsequence, again denoted by \(\{u_{j} \}_{j\in\mathbb{N}}\), and there exists \(u\in E\) such that
Hence,
as \(j\rightarrow+\infty\). Moreover, by Lemma 3.2 and Hölder’s inequality, passing to subsequence if necessary, we have
On the other hand, an easy computation shows that
which deduces that \(\u_{j}u\\rightarrow0\) as \(j\rightarrow+\infty\). □
Now we are in a position to give the proof of Theorem 1.2. We divide the proof into several steps.
Proof of Theorem 1.2
Step 1 It is clear that \(I(0)=0\) and \(I\in C^{1}(E,\mathbb{R})\) satisfies the (PS) condition by Lemmas 3.1 and 3.3.
Step 2 We now show that there exist constants \(\rho >0\) and \(\alpha>0\) such that I satisfies condition (A1) of Lemma 2.3. By (1.9), for all \(\varepsilon>0\), there exists \(\delta >0\) such that \(W(t,u)\leq\varepsilonu^{2}\) whenever \(u\leq\delta\). Choosing \(\rho=\frac{\delta}{\sqrt {2e_{0}\sqrt{\beta}}}\) and \(\u\=\rho\), we have \(\u\_{\infty}\leq\delta\). Hence \(W(t,u(t))\leq\varepsilon u(t)^{2}\) for all \(t\in\mathbb{R}\). Integrating on \(\mathbb{R}\) and by (2.1), we get
In consequence, combining this with (3.1), we obtain that, for \(\u\=\rho\),
Setting \(\varepsilon=\frac{1}{4 C^{2}}\), inequality (3.15) implies that
Step 3 It remains to prove that there exists \(e\in E\) such that \(\e\>\rho\) and \(I(e)\leq0\), where ρ is defined in Step 2. By (3.1), we have, for every \(m\in\mathbb{R}\setminus \{0 \}\) and \(u\in E\setminus \{0 \}\),
Take some \(\psi\in E\) such that \(\\psi\=1\). Then there exists a subset Ω of positive measure of \(\mathbb{R}\) such that \(\psi(t)\neq0\) for \(t\in\varOmega\). Take \(m>0\) such that \(m \psi(t)\geq1\) for \(t\in\varOmega\). Then, by (1.7), we obtain that
Since \(\eta(t)>0\) and \(\mu>2\), (3.16) implies that \(I(m \psi )<0\) for some \(m>0\) with \(m \psi(t)\geq1\) for \(t\in\varOmega\) and \(\m \psi\> \rho\), where ρ is defined in Step 2. By Lemma 2.3, I possesses a critical value \(c\geq\alpha>0\) given by
where
Hence there is \(u\in E\) such that
Step 4 Now suppose that \(W(t,u)\) is even in u, i.e., (\(\mathrm{W}_{4}\)) holds, which implies that I is even. Furthermore, we have already known that \(I(0)=0\) and \(I\in C^{1}(E,\mathbb{R})\) satisfies the (PS) condition in Step 1.
To apply Lemma 2.4, it suffices to prove that I satisfies conditions (A3) and (A4) of Lemma 2.4. Here we take \(V= \{0 \}\) and \(X=E\). (A3) is identically the same as in Step 2, so it is already proved. Now we prove that (A4) holds. Let \(\tilde{E}\subset E\) be a finite dimensional subspace. From Step 3, we know that, for any \(\psi\in \tilde{E}\subset E\) such that \(\\psi\=1\), there is \(m_{\psi}>0\) such that
Since \(\tilde{E}\subset E\) is a finite dimensional subspace, we can choose \(R=R(\tilde{E})>0\) such that
Hence, by Lemma 2.4, I possesses an unbounded sequence of critical values \(\{c_{j} \}_{j\in \mathbb{N}}\). Let \(u_{j}\) be the critical point of I corresponding to \(c_{j}\), then (DS) has infinitely many distinct fast homoclinic solutions. □
References
 1.
Alves, C.O., Carrião, P.C., Miyagaki, O.H.: Existence of homoclinic orbits for asymptotically periodic systems involving Duffinglike equation. Appl. Math. Lett. 16(5), 639–642 (2003)
 2.
Ambrosetti, A., Rabinowitz, P.H.: Dual variational methods in critical point theory and applications. J. Funct. Anal. 14(4), 349–381 (1973)
 3.
Caldiroli, P., Montecchiari, P.: Homoclinic orbits for second order Hamiltonian systems with potential changing sign. Commun. Appl. Nonlinear Anal. 1(2), 97–129 (1994)
 4.
Chen, P., Tang, X.H.: Fast homoclinic solutions for a class of damped vibration problems with subquadratic potentials. Math. Nachr. 286(1), 4–16 (2013)
 5.
Chen, P., Tang, X.H., Agarwal, R.P.: Fast homoclinic solutions for a class of damped vibration problems. Appl. Math. Comput. 219(11), 6053–6065 (2013)
 6.
Coti Zelati, V., Rabinowitz, P.H.: Homoclinic orbits for second order Hamiltonian systems possessing superquadratic potentials. J. Am. Math. Soc. 4(4), 693–727 (1991)
 7.
Daouas, A.: Homoclinic solutions for superquadratic Hamiltonian systems without periodicity assumption. Nonlinear Anal. 74(11), 3407–3418 (2011)
 8.
Ding, Y.H.: Existence and multiplicity results for homoclinic solutions to a class of Hamiltonian systems. Nonlinear Anal. 25(11), 1095–1113 (1995)
 9.
Ding, Y.H., Lee, C.: Homoclinics for asymptotically quadratic and superquadratic Hamiltonian systems. Nonlinear Anal. 71, 1395–1413 (2009)
 10.
Izydorek, M., Janczewska, J.: Homoclinic solutions for a class of the second order Hamiltonian systems. J. Differ. Equ. 219(2), 375–389 (2005)
 11.
Korman, P., Lazer, A.C.: Homoclinic orbits for a class of symmetric Hamiltonian systems. Electron. J. Differ. Equ. 1994, 01 (1994)
 12.
Lv, X., Jiang, J.F.: Existence of homoclinic solutions for a class of secondorder Hamiltonian systems with general potentials. Nonlinear Anal., Real World Appl. 13, 1152–1158 (2012)
 13.
Lv, X., Lu, S.P., Yan, P.: Existence of homoclinic solutions for a class of secondorder Hamiltonian systems. Nonlinear Anal. 72, 390–398 (2010)
 14.
Lv, Y., Tang, C.L.: Existence of even homoclinic orbits for a class of Hamiltonian systems. Nonlinear Anal. 67(7), 2189–2198 (2007)
 15.
Omana, W., Willem, M.: Homoclinic orbits for a class of Hamiltonian systems. Differ. Integral Equ. 5(5), 1115–1120 (1992)
 16.
Poincaré, H.: Les méthodes nouvelles de la mécanique céleste. GauthierVillars, Paris (1897–1899)
 17.
Rabinowitz, P.H.: Minimax methods in critical point theory with applications to differential equations. In: CBMS Reg. Conf. Ser. in. Math., vol. 65. American Mathematical Society, Provodence, RI (1986)
 18.
Rabinowitz, P.H.: Homoclinic orbits for a class of Hamiltonian systems. Proc. R. Soc. Edinb., Sect. A 114(1–2), 33–38 (1990)
 19.
Rabinowitz, P.H., Tanaka, K.: Some results on connecting orbits for a class of Hamiltonian systems. Math. Z. 206(3), 473–499 (1991)
 20.
Sun, J.T., Chen, H.B., Nieto, J.J.: Homoclinic solutions for a class of subquadratic secondorder Hamiltonian systems. J. Math. Anal. Appl. 373(1), 20–29 (2011)
 21.
Tang, X.H., Lin, X.Y.: Infinitely many homoclinic orbits for Hamiltonian systems with indefinite subquadratic potentials. Nonlinear Anal. 74, 6314–6325 (2011)
 22.
Tang, X.H., Lin, X.Y.: Existence of infinitely many homoclinic orbits in Hamiltonian systems. Proc. R. Soc. Edinb., Sect. A 141, 1103–1119 (2011)
 23.
Wan, L.L., Tang, C.L.: Existence and multiplicity of homoclinic orbits for second order Hamiltonian systems without (AR) condition. Discrete Contin. Dyn. Syst., Ser. B 15, 255–271 (2011)
 24.
Wang, J., Zhang, F.B., Xu, J.X.: Existence and multiplicity of homoclinic orbits for the second order Hamiltonian systems. J. Math. Anal. Appl. 366, 569–581 (2010)
 25.
Wu, X., Chen, S.X., Teng, K.M.: On variational methods for a class of damped vibration problems. Nonlinear Anal. 68, 1432–1441 (2008)
 26.
Yang, M.H., Han, Z.Q.: The existence of homoclinic solutions for secondorder Hamiltonian systems with periodic potentials. Nonlinear Anal., Real World Appl. 12, 2742–2751 (2011)
 27.
Zhang, C.F., Han, Z.Q.: Infinitely many homoclinic orbits for a class of secondorder damped differential equations. Math. Methods Appl. Sci. 38, 5048–5062 (2015)
 28.
Zhang, Q.Y., Liu, C.G.: Infinitely many homoclinic solutions for second order Hamiltonian systems. Nonlinear Anal. 72, 894–903 (2010)
 29.
Zhang, Z.H., Yuan, R.: Homoclinic solutions for a class of nonautonomous subquadratic second order Hamiltonian systems. Nonlinear Anal. 71, 4125–4130 (2009)
 30.
Zhang, Z.H., Yuan, R.: Homoclinic solutions for a class of asymptotically quadratic Hamiltonian systems. Nonlinear Anal., Real World Appl. 11, 4185–4193 (2010)
 31.
Zhang, Z.H., Yuan, R.: Fast homoclinic solutions for some second order nonautonomous systems. J. Math. Anal. Appl. 376, 51–63 (2011)
 32.
Zou, W.M., Li, S.J.: Infinitely many homoclinic orbits for the secondorder Hamiltonian systems. Appl. Math. Lett. 16, 1283–1287 (2003)
Acknowledgements
The authors would like to thank the referees for carefully reading the manuscript, giving valuable comments and suggestions to improve the results as well as the exposition of the paper.
Availability of data and materials
Data sharing not applicable to this article as no datasets were generated or analysed during the current study.
Funding
The authors are supported financially by the National Natural Science Foundation of China (11771044).
Author information
Affiliations
Contributions
All authors contributed equally and significantly in writing this article. All authors read and approved the final manuscript.
Corresponding author
Ethics declarations
Competing interests
The authors declare that there is no conflict of interests regarding the publication of this paper.
Additional information
Publisher’s Note
Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Rights and permissions
Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.
About this article
Cite this article
Zhu, X., Zhang, Z. Fast homoclinic solutions for damped vibration problems with superquadratic potentials. Bound Value Probl 2018, 183 (2018). https://doi.org/10.1186/s136610181103y
Received:
Accepted:
Published:
DOI: https://doi.org/10.1186/s136610181103y
MSC
 34C37
 35A15
 35B38
Keywords
 Homoclinic solutions
 Critical point
 Variational methods
 Mountain pass theorem