#### Abstract

We show that every well-defined solution of the fourth-order difference equation ,    , where parameter , is eventually periodic with period four.

#### 1. Introduction

The study of max-type difference equations attracted recently a considerable attention, see, for example, [127], and the references listed therein. This type of difference equations stems from, for example, certain models in automatic control theory (see [28]). In the beginning of the study of these equations experts have been focused on the investigation of the behavior of some particular cases of the following general difference equation of order :

where , , are real sequences (mostly constant or periodic ones) and where the initial values are different from zero (see, e.g., [2, 3, 6, 7, 912, 2225] and the references cited therein).

The study of max-type equations of the following general form

where , are natural numbers such that , , and , are sequences of real numbers, was proposed by Stević in numerous talks, for example, in [13, 14]. For some results in this direction see [1, 4, 1517, 1921, 26, 27]. For some nonlinear difference equations related to (1.2) see, for example, [7, 15, 17, 18, 2938].

Definition 1.1. A sequence is said to be eventually periodic with period if there is an index such that for all . Specially, if , then the sequence is periodic with period .

Motivated by some ideas due to Stević (e.g., the main lemmas there, Lemmas and are suggested by him), the authors of [26] considered the following second-order max-type difference equation:

Equation(1.3) is not difficult for handling since, by the change , it is transformed into one of the following first-order difference equations

Using these equations, it is easy to see that for the case every solution of (1.3) is eventually periodic with period two.

Recently, in the paper [5] it was showed that every solution of the third-order max-type difference equation

where the initial conditions are arbitrary nonzero real numbers and is eventually periodic with period three. The fact that all solutions of (1.5) are periodic is not a surprising fact (for an explanation see [4]).

For some recent papers on difference equations all the solutions of which are periodic see, for example, [7, 3945] and the references cited therein.

Here we show that every well-defined solution of the following fourth-order max-type difference equation

where the parameter is eventually periodic with period four.

Remark 1.2. Note that if , then (1.6) becomes , from which it follows that every solution is periodic with period four. Hence, in the sequel we will consider the case

In the sequel we will frequently use the following simple lemma, given without a proof (for related results see [4, 5]).

Lemma 1.3. Assume that is a solution of (1.6) and there is such that Then this solution is eventually periodic with period four.

#### 2. Main Results

In this subsection we give a specific form of the solutions of the difference equation (1.6) when the parameter and in each case we can deduce that every solution of this equation is periodic with period four.

Depending on the positivity of four initial values of (1.6), there are the following 16 cases to be considered:

First, we prove another auxiliary result.

Lemma 2.1. Assume that the parameter . Then every solution of (1.6) is eventually positive if initial values satisfy one of conditions (i), (iii)–(xvi).

Proof. If or , then From this, (1.6), and by induction it follows that for every .
If , then
From this, (1.6), and by induction it follows that for every .
If , then
Similar to the previous case, by induction it follows that for every .

Now, we can formulate and prove our main results.

Theorem 2.2. Assume that the parameter . Then every solution of (1.6) with positive initial values is eventually periodic with period four.

Proof. From (1.6), we see that We consider the following two cases. In this case , and we see that Now, there exists two subcases. which occurs when . We have If , then and Hence, , , , and , which implies that is an eventually (from ) periodic solution with period four. In this case we see that the solution has the following form: If , then and Hence, , , , and , which implies that is an eventually (from ) periodic solution with period four (in this case minimal period is two). This solution takes the form which occurs when , and If , then and If , then and Hence, , , , and , which implies that is an eventually (from ) periodic solution with period four. It can be written in the form If , then and Hence, , , , and , which implies that is an eventually (from ) periodic solution with period four. Moreover, it can be written as follows: If , then and As above, the solution is eventually (from ) periodic with period four and it has the form In this case , and we see that There again exist two subcases. which occurs when . So, If , then and Then we see that the solution is and is an eventually (from ) periodic solution with period four. If , then and So, the solution takes the following form which is an eventually (from ) periodic solution with period four: which occurs when . So, If , then and If , then .
Therefore is a periodic solution with period four and the solution takes the form
If , then and Therefore, again is an eventually (from ) periodic solution with period four and the solution takes the form If , then and If , then and Thus, the solution is in the following form which is eventually (from ) periodic with period four: If , then and Thus, the solution is of the following form Therefore is eventually (from ) periodic with period four. The proof is completed.

From Lemma 1.3 and Theorem 2.2 we obtain the following result.

Theorem 2.3. Assume the parameter and that initial values of (1.6) satisfy one of conditions (i), (iii)–(xvi) in Lemma 2.1. Then every such solution of (1.6) is eventually periodic with period four.

Proof. If initial values of (1.6) satisfy one of conditions (i), (iii)–(xvi) in Lemma 2.1, then by the same lemma it follows that the corresponding solution is eventually positive. This means that there is such that for every In particular, we have that . Since equation (1.6) is autonomous if is a solution of (1.6), then is also a solution of (1.6) but such that Hence, the problem is reduced to the case when all the initial values are positive. Applying Theorem 2.2, the result follows.

In the next theorem we study those solutions of (1.6) such that We would like to thank Professor Stević for giving us the elegant proof below which drastically reduced our original proof.

Theorem 2.4. Assume that the parameter and all the initial values are negative Then every solution of (1.6) is eventually periodic with period four.

Proof. Since , , , and , by induction we have for each . By the change , (1.6) becomes where for every Hence by Theorem 2.2 the result follows.

Since all the cases are reduced to the case when all initial values are positive, it is of interest to investigate this case in more details. The next theorem describes all eventually constant solutions of (1.6). Our idea stems from [46] (see also [4750]).

Theorem 2.5. Assume that the parameter . Then all positive solutions to (1.6) which are eventually equal to the positive equilibrium have the following form:

Proof. First note that by the change the problem is reduced to the case . Assume that for and Then , , which implies and . On the other hand, we have so that , which is a contradiction. Hence , that is, . Since , we get (case above). Since and , it follows that , as claimed.