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Exact oscillation regions for a partial difference equation
Advances in Difference Equations volumeÂ 2015, ArticleÂ number:Â 100 (2015)
Abstract
This paper is concerned with a partial difference equation with constant coefficients. By means of the theory of envelopes, we consider the regions of nonpositive roots of its characteristic equation and obtain a necessary and sufficient condition for the oscillation of all solutions of the partial difference equation.
1 Introduction
Partial difference equations have numerous applications in image processing, material mechanics, random walk problems, molecular orbits, finite difference schemes, as well as population dynamics [1â€“7]. In recent years, the oscillatory behavior of partial difference equations has been discussed in many papers (see [7â€“14] and the references therein).
In [15â€“18], Lin and Cheng gave explicit necessary and sufficient conditions for all solutions of some ordinary difference equations with constant coefficients to be oscillatory by means of the envelope theory of a family of straight lines. However, to the best of our knowledge, very little attention has been paid to the analysis of the oscillatory behavior of solutions of partial difference equations from the perspective of the envelope theory.
In this paper, we consider the partial difference equation of the form
where a, b, c are real numbers and m, n are nonnegative integers. The purpose of this paper is to develop a new method for the analysis of the oscillation of (1) based on the theory of envelopes.
By a solution of (1), we mean a nontrivial double sequence \(\{A_{m,n}\}\) of real numbers which is defined for \(m \geq0\) and \(n\geq 0\) and satisfies (1) for \(m \geq0 \) and \(n\geq0\).
A solution \(\{A_{m,n}\}\) of (1) is said to be eventually positive (or negative) if \(A_{m,n} \geq0 \) (or \(A_{m,n} \leq0 \)) for large m and n. It is said to be oscillatory if it is neither eventually positive nor eventually negative.
The paper is organized as follows. SectionÂ 2 presents several useful lemmas. In SectionÂ 3, we derive the oscillation criterion for partial difference equation (1). Two examples are given to illustrate our oscillation criterion in SectionÂ 4. Finally SectionÂ 5 is devoted to concluding remarks.
2 Some lemmas
In this section, we give some preliminaries that will be needed in the next section.
From Corollary 2.9 in [14], we can easily obtain the following lemma.
Lemma 1
The following statements are equivalent:

(a)
Every solution of (1) is oscillatory.

(b)
The characteristic equation of (1)
$$ \lambda^{2}+\mu^{2}+a\lambda+b\mu+c=0 $$has no positive roots.
Lemma 2
([8])
Suppose that \(f(x,y)\), \(g(x,y)\), \(h(x,y)\) and \(v(x,y)\) are differentiable on \((\infty, +\infty)\times(\infty,+\infty)\). Let Î“ be a twoparameter family of planes defined by the equation
where Î» and Î¼ are parameters. Let Î£ be the envelope of the family Î“. Then the equation
has no real roots if and only if there is no tangent plane of Î£ passing through the point \((a,b,c)\) in the Euclidean space \(R^{3}\).
Lemma 3
([19])
For the linear homogeneous difference equation
where n is a nonnegative integer, k is a positive integer and \(a_{1}, a_{2}, \ldots, a_{k}\) are real numbers, the following statements are equivalent:
3 Main results
In this section, we establish the necessary and sufficient condition for oscillations of all solutions of (1) by the envelope theory.
Theorem 1
Every solution of (1) oscillates if and only if \(a\geq0\), \(b\geq 0\) and \(c\geq0\) or \(a<0\), \(b<0\) and
Proof
The characteristic equation of (1) is
Let
Since we mainly discuss the oscillations of (1), by Lemma 1, attention will be restricted to the case where \(\lambda>0\) and \(\mu> 0\). To this end, we will think of \((a,b,c)\) as a point in the Euclidean space \(R^{3}\) and try to find the exact regions containing points \((a,b,c)\) in the Euclidean space \(R^{3}\) such that (3) has no positive roots. In fact, \(f(x,y,z,\lambda,\mu)= 0\) can be regarded as an equation describing a twoparameter family of planes in the Euclidean space \(R^{3}\), where x, y and z are the coordinates of points of the planes in the Euclidean space \(R^{3}\) and Î», Î¼ are two parameters.
By the envelope theory, the points of the envelope of the twoparameter family of planes described by (3) satisfy the system of equations
where \(\lambda>0\) and \(\mu> 0\). Eliminating the two parameters Î» and Î¼ from (4) leads to the equation of the envelope
where \(x<0\) and \(y < 0\). From (5), we have \(z(x,y)>0\) for \(x<0\) and \(y<0\), \(\partial^{2} z/\partial x^{2}=1/2>0\), \(\partial^{2} z/\partial y^{2}=1/2>0\) and \(\partial^{2} z/\partial x^{2} \cdot\partial^{2} z/\partial y^{2}(\partial^{2} z/\partial x\,\partial y)^{2}=1/4>0\). Hence, \(z(x, y)\) is a positive and strictly convex function on \((\infty ,0)\times(\infty, 0)\). Furthermore, the envelope defined by (5) is a convex surface S over \((\infty, 0)\times(\infty, 0)\) as depicted in FigureÂ 1. In view of FigureÂ 1 and the obtained information of \(z(x,y)\), it is easily seen that when the point \((a,b,c)\) is in the first closed octant, that is, \(a\geq0\), \(b\geq 0\) and \(c\geq0\), there cannot be any tangent plane of the envelope S which also passes through this point, and when the point \((a,b,c)\) is vertically above the envelope S, that is, \(a<0\), \(b<0\) and \(c>(a^{2}+b^{2})/4\), there cannot exist any tangent plane of the envelope S which also passes through this point, while the point \((a,b,c)\) is situated elsewhere, there always exists a tangent plane of the envelope S which also passes through this point. By Lemma 2, the characteristic equation (3) does not have any positive roots if and only if \(a\geq0\), \(b\geq0\) and \(c\geq0\) or \(a<0\), \(b<0\) and
Lemma 1 implies that the statement of this theorem is true. The proof is thus completed.
â€ƒâ–¡
If we let \(\mu=0\) in (3), then (3) reduces to the form
The corresponding ordinary difference equation of (6) takes the form
On the basis of Theorem 1, we can obtain the following results.
Corollary 1
Equation (6) has no positive roots if and only if \(c\geq0\) and \(a\geq0\) or \(a<0\) and \(c>a^{2}/4\).
Remark 1
In fact, Corollary 1 is just Theorem 5.1 of [20].
Corollary 2
Every solution of (7) oscillates if and only if \(c\geq0\) and \(a\geq0\) or \(a<0\) and \(c>a^{2}/4\).
Proof
Combining the results of Corollary 1 and Lemma 3 yields the proof.â€ƒâ–¡
Remark 2
Corollary 2 shows that Theorem 1 is a natural generalization for the corresponding result of ordinary difference equation (7), and ordinary difference equation (7) is a special case of our study.
4 Illustrative examples
In this section, two examples are given to illustrate the applications of Theorem 1.
Example 1
Consider the partial difference equation
where m, n are nonnegative integers.
From (8), we have \(a=0.3<0\), \(b=0.1 < 0\) and \((a^{2}+b^{2})/4 = ((0.3)^{2}+(0.1)^{2})/4 = 0.025<0.28 = c\). By Theorem 1, every solution of (8) is oscillatory. The oscillatory behavior of (8) is demonstrated by FigureÂ 2.
Example 2
Consider the partial difference equation
where m, n are nonnegative integers.
From (9), we have \(a=0.02>0\), \(b=0.12>0\) and \(c=0.12>0\). It follows from Theorem 1 that every solution of (9) is oscillatory. The oscillatory behavior of (9) is demonstrated by FigureÂ 3.
5 Conclusions
In this paper, we have introduced a novel approach to problems of oscillations of a partial difference equation. Our approach is based on the envelope theory of the family of planes. We derive effective criteria to determine oscillations of a partial difference equation by this approach. Numerical examples are given to illustrate the results presented in this paper.
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Acknowledgements
This work is supported by the National Natural Science Foundation of P.R. China under Grant No. 61273088. The authors thank the editor and the referees for their valuable suggestions and comments.
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Yuan, C., Liu, S. & Liu, J. Exact oscillation regions for a partial difference equation. Adv Differ Equ 2015, 100 (2015). https://doi.org/10.1186/s1366201503879
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DOI: https://doi.org/10.1186/s1366201503879