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Forced oscillation for solutions of boundary value problems of fractional partial difference equations
Advances in Difference Equations volume 2016, Article number: 263 (2016)
Abstract
In this paper, we obtain the forced oscillation of solutions for certain fractional partial difference equations with two different types of boundary conditions. Our results are based on discrete Gaussian formula and some basic theories of discrete fractional calculus.
1 Introduction
In 1974, Diaz and Osler [1] presented a discrete fractional difference operator based on an infinite series. In 1988, Miller and Ross [2] introduced the definitions of noninteger-order differences and sums. Since then, the theory of fractional difference equations has been studied by several scholars. In recent years, some papers [3–21] on discrete fractional calculus were published, which helped to build up the theory of fractional difference equations. For example, Atici and Eloe [3] discussed the properties of the generalized falling function, the corresponding power rule for fractional delta operators, and the commutativity of fractional sums.
Very recently, the oscillation theory as a part of the qualitative theory of fractional differential equations and fractional difference equations has been developed. We refer the reader to [20–28] and the references therein. In particular, we notice that a few papers [24–28] studied the oscillation of fractional partial differential equations that involve the Riemann-Liouville fractional partial derivatives.
Motivated by the papers [24–29], we investigate the forced oscillation of the fractional partial difference equation of the form
where \(m=(m_{1},m_{2},\ldots,m_{\ell})\), Ω is a convex connected solid net (for the definition of a convex connected solid net, we refer to [29]), and
\(\mathbb{N}(1,N_{i})=\{1,2,\ldots N_{i}\}\), \(i=1,2,\ldots,\ell\), L is the discrete Laplacian on Ω defined as
\(\Delta_{n}^{\alpha}u(m,n)\) is the Riemann-Liouville fractional difference operator of order α of u with respect to n, \(\alpha\in(0,1)\) is a constant, \(\mathbb{N}_{a}=\{a,a+1,a+2,\ldots\} \), and \(a\geq0\) is a real number.
Throughout this paper, we always assume that
-
(A)
\(a(n)\geq0, n\in\mathbb{N}_{a}\); \(q(m,n)\geq0\), \(q(n)=\min_{m\in \Omega}q(m,n)\), \((m,n)\in\Omega\times\mathbb{N}_{a}\); and \(h:\Omega\times\mathbb {N}_{a}\rightarrow\mathbb{R}\).
Consider one of the two following boundary conditions:
or
where
\(\Delta_{N}u(m-1,n)\) is the normal difference at \((m,n)\in\partial\Omega\times\mathbb{N}_{a}\) defined by
N is the unit exterior normal vector to ∂Ω, \(m+1:=\{m_{1}+1,m_{2},\ldots,m_{\ell}\}\cup\cdots\cup\{m_{1},\ldots , m_{\ell -1},m_{\ell}+1\}\), \(m-1:=\{m_{1}-1,m_{2},\ldots,m_{\ell}\}\cup\cdots\cup\{m_{1},\ldots, m_{\ell -1},m_{\ell}-1\}\), and \(g(m,n)\geq0, \phi(m,n)\geq0, (m,n)\in\partial\Omega\times\mathbb{N}_{a}\). For the details on ∂Ω and \(\Delta_{N}u(m-1,n)\), we refer to the monograph [30] and paper [29], respectively.
The function \(u(m,n)\) is said to be a solution of problem (1)-(B1) (or (1)-(B2)) if it satisfies (1) for \((m,n)\in\Omega\times\mathbb{N}_{a}\) and satisfies (B1) (or (B2)) for \((m,n)\in\partial\Omega\times\mathbb{N}_{a}\).
The solution \(u(m,n)\) of problem (1)-(B1) (or (1)-(B2)) is said to be oscillatory in \(\Omega\times\mathbb{N}_{a}\) if it is neither eventually positive nor eventually negative; otherwise, it is nonoscillatory.
2 Preliminaries
In this section, we present some preliminary results of discrete fractional calculus and partial differences.
Definition 2.1
[3]
Let \(0<\nu<1\). The νth fractional sum of f is defined by
where f is defined for \(s\in\mathbb{N}_{a}\), \(\Delta_{a}^{-\nu}f\) is defined for \(s\in\mathbb{N}_{a+\nu}= \{a+\nu,a+\nu+1,a+\nu+2,\ldots\}\), Γ is the gamma function, and
Definition 2.2
Let \(0<\nu<1\). The νth fractional sum with respect to n of \(u(m,n)\) is defined by
Definition 2.3
[3]
Let \(\mu>0\) and \(k-1<\mu<k\), where k denotes a positive integer, \(k=\lceil\mu\rceil\). Set \(\nu=k-\mu\). The μth fractional difference is defined as
where \(\lceil\mu\rceil\) is the ceiling function of μ.
Definition 2.4
Let \(0<\mu<1\) and \(\nu=1-\mu\). The μth fractional partial difference with respect to n of a function \(u(m,n)\) is defined as
Lemma 2.5
[3]
Let f be a real-valued function defined on \(\mathbb{N}_{a}\), and let \(\mu,\nu>0\). Then the following equalities hold:
Lemma 2.6
For \(n_{0}\in\mathbb{N}_{a}\), let
Then
Proof
By Definition 2.1, from (11) we have
Using Definition 2.3, from (13) it follows that
The proof of Lemma 2.6 is complete. □
Lemma 2.7
Discrete Gaussian formula [29]
Let Ω be a convex connected solid net. Then
Lemma 2.8
[31]
For \(\varepsilon>0\),
For convenience, we introduce the following notations:
3 Oscillation of problem (1)-(B1)
Theorem 3.1
For \(n_{0}\in \mathbb{N}_{a}\), if
and
where \(H(n)\) is defined as in (16), then every solution \(u(m,n)\) of problem (1)-(B1) is oscillatory in \(\Omega\times\mathbb{N}_{a}\).
Proof
Suppose to the contrary that there is a nonoscillatory solution \(u(m,n)\) of problem (1)-(B1) that has no zero in \(\Omega\times \mathbb{N}_{a}\) for some \(n^{*}\geq a\). Then \(u(m,n)>0\) or \(u(m,n)<0\) for \(n\geq n^{*}\).
Case 1. \(u(m,n)>0, n\geq n^{*}\). Summing equation (1) over Ω, we have
The discrete Gaussian formula and (B1) yield
From assumption (A) we have
Combining (19)-(21), we obtain
where \(U(n)\) is defined as in (16). It follows from (22) that
Using Lemma 2.6, from (23) we have
where
Summing both sides of (24) from \(n^{*}\) to \(n-1\), we obtain
Taking \(n\rightarrow\infty\) in (25), we have
which contradicts with \(G(n)>0\).
Case 2. \(u(m,n)<0, n\geq n^{*}\). As in the proof of Case 1, we obtain (19). The discrete Gaussian formula and (B1) yield
From assumption (A) we have
Combining (19), (26), and (27), we obtain
Then we have
Using the above-mentioned method in Case 1, we easily obtain a contradiction. This completes the proof of Theorem 3.1. □
Theorem 3.2
If
and
where \(H(n)\) is defined as in (16), then every solution \(u(m,n)\) of problem (1)-(B1) is oscillatory in \(\Omega\times\mathbb{N}_{a}\).
Proof
Suppose to the contrary that there is a nonoscillatory solution \(u(m,n)\) of problem (1)-(B1) that has no zero in \(\Omega\times \mathbb{N}_{a}\) for some \(n^{*}\geq a\). Then \(u(m,n)>0\) or \(u(m,n)<0\) for \(n\geq n^{*}\).
Case 1. \(u(m,n)>0, n\geq n^{*}\). As in the proof of Theorem 3.1, we obtain (22). Applying the operator \(\Delta^{-\alpha}\) to inequality (22), we have
By Lemma 2.5 it follows from the left-hand side of (32) that
where \(\Delta^{-(1-\alpha)}U(a)=\Delta^{-(1-\alpha)}U(n) |_{n=a}=C_{0}\) is a constant. Applying Definition 2.1 to the right-hand side of (32), we have
It follows from (35) that
Using Lemma 2.8, we obtain
Noting (37) and taking \(n\rightarrow\infty\) in (36), we have
which contradicts with \(U(n)>0\).
Case 2. \(u(m,n)<0, n\geq n_{0}\). As in the proof of Theorem 3.1, we obtain the fractional difference inequality (29). Then using the above-mentioned method, we easily obtain a contradiction. This completes the proof of Theorem 3.2. □
4 Oscillation of problem (1)-(B2)
Theorem 4.1
For \(n_{0}\in \mathbb{N}_{a}\), if
and
where \(\Phi(n)\) and \(H(n)\) are defined as in (16), then every solution \(u(m,n)\) of problem (1)-(B2) is oscillatory in \(\Omega\times\mathbb{N}_{a}\).
Proof
Suppose to the contrary that there is a nonoscillatory solution \(u(m,n)\) of problem (1)-(B2) that has no zero in \(\Omega\times \mathbb{N}_{a}\) for some \(n^{*}\geq a\). Then \(u(m,n)>0\) or \(u(m,n)<0\) for \(n\geq n^{*}\).
Case 1. \(u(m,n)>0, n\geq n^{*}\). As in the proof of Theorem 3.1, we obtain (19). Using the discrete Gaussian formula and noting the boundary condition (B2), it follows from (19) that
Combing (19), (21), and (40), we have
The remainder of the proof is similar to that of Case 1 in Theorem 3.1. We omit it here.
Case 2. \(u(m,n)<0, n\geq n^{*}\). In this case, we easily obtain (19), (27), and (40). Then we have
The remainder of the proof is similar to that of Case 2 in Theorem 3.1. We omit it here, too. The proof of Theorem 4.1 is complete. □
Theorem 4.2
If
and
where \(\Phi(n)\) and \(H(n)\) are defined as in (16), then every solution \(u(m,n)\) of problem (1)-(B2) is oscillatory in \(\Omega\times\mathbb{N}_{a}\).
5 Examples
Example 5.1
Consider the fractional partial difference equation
with boundary condition
Here \(\alpha=\frac{1}{2}, a(n)=2n\), \(q(m,n)=\frac{2n}{m}\), \(h(m,n)=\frac{m}{3}+\frac{1}{3}[(-1)^{n+1}e^{n+1}-(-1)^{n}e^{n}-2]\). It is easy to see that \(q(n)=\frac{2}{3}n\) and
Therefore,
It follows from (47) that
and
Using Theorem 3.1, we obtain that every solution of problem (45)-(46) is oscillatory in \(\mathbb{N}(1,3)\times\mathbb{N}_{0}\).
Example 5.2
Consider the fractional partial difference equation
with boundary condition
Here \(\alpha=\frac{1}{4}, a(n)=2\Gamma(n)\), \(q(m,n)=\frac{\Gamma (n+\frac{3}{4})}{2m\Gamma(n)}\), \(h(m,n)=\frac{1}{4}\Gamma(\frac{1}{4})m+\frac{n}{2}\). It is easy to see that
Therefore,
which shows that condition (30) of Theorem 3.2 does not hold. Indeed, \(u(m,n)=mn^{(\frac{1}{4})}\) is a nonoscillatory solution of problem (48)-(49).
Example 5.3
Consider the fractional partial difference equation
with boundary condition
Here \(\alpha=\frac{1}{3}, a(n)=\frac{1}{2}, q(m,n)=\frac{2\Gamma(\frac{1}{3})\Gamma(n+\frac{2}{3})}{ 3n\Gamma(n)}, h(m,n)=\Gamma(\frac{1}{3})m^{2}-\frac{n\Gamma (n)}{\Gamma (n+\frac{2}{3})}, \phi(m,n)=\frac{2n\Gamma(n)}{\Gamma(n+\frac{2}{3})}\). Therefore,
It is easy to see that
Thus, this time, condition (38) of Theorem 4.1 is false. Indeed, we easily see that \(u(m,n)=m^{2}n^{(\frac{1}{3})}\) is a nonoscillatory solution of the problem (51)-(52).
Example 5.4
Consider the fractional partial difference equation
with boundary condition
Here \(\alpha=\frac{2}{3}, a(n)=3n\), \(q(m,n)=\frac{n}{m}\), \(h(m,n)=\frac{m}{3}+\frac{1}{2}[(-1)^{n+1}e^{n+1}-(-1)^{n}e^{n}-1]\), and \(\phi (m,n)=\frac{1}{4}[(-1)^{n+1}e^{n+1}-(-1)^{n}e^{n}]\). It is easy to see that \(q(n)=\frac{n}{2}\),
and
Therefore,
It follows from (56) that
and
We easily see that the conditions of Theorem 4.1 are satisfied. Then every solution of problem (54)-(55) is oscillatory in \(\mathbb {N}(1,2)\times\mathbb{N}_{0}\).
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Acknowledgements
This work is supported by the National Natural Science Foundation of China (10971018). The authors thank the referees very much for their valuable comments and suggestions on this paper.
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Li, W.N., Sheng, W. Forced oscillation for solutions of boundary value problems of fractional partial difference equations. Adv Differ Equ 2016, 263 (2016). https://doi.org/10.1186/s13662-016-0992-2
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DOI: https://doi.org/10.1186/s13662-016-0992-2