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# Stability of Equilibrium Points of Fractional Difference Equations with Stochastic Perturbations

*Advances in Difference Equations*
**volume 2008**, Article number: 718408 (2008)

## Abstract

It is supposed that the fractional difference equation , has an equilibrium point and is exposed to additive stochastic perturbations type of that are directly proportional to the deviation of the system state from the equilibrium point . It is shown that known results in the theory of stability of stochastic difference equations that were obtained via V. Kolmanovskii and L. Shaikhet general method of Lyapunov functionals construction can be successfully used for getting of sufficient conditions for stability in probability of equilibrium points of the considered stochastic fractional difference equation. Numerous graphical illustrations of stability regions and trajectories of solutions are plotted.

## 1. Introduction—Equilibrium Points

Recently, there is a very large interest in studying the behavior of solutions of nonlinear difference equations, in particular, fractional difference equations [1–38]. This interest really is so large that a necessity appears to get some generalized results.

Here, the stability of equilibrium points of the fractional difference equation

with the initial condition

is investigated. Here , , , , are known constants. Equation (1.1) generalizes a lot of different particular cases that are considered in [1–8, 16, 18, 19, 20, 22, 23, 24, 32, 35, 37].

Put

and suppose that (1.1) has some point of equilibrium (not necessary a positive one). Then by assumption

the equilibrium point is defined by the algebraic equation

By condition (1.4), equation (1.5) can be transformed to the form

It is clear that if

then (1.1) has two points of equilibrium

If

then (1.1) has only one point of equilibrium

And at last if

then (1.1) has not equilibrium points.

Remark 1.1.

Consider the case , . From (1.5) we obtain the following. If and , then (1.1) has two points of equilibrium:

If and , then (1.1) has only one point of equilibrium: . If , then (1.1) has only one point of equilibrium: .

Remark 1.2.

Consider the case , . If , then (1.1) has only one point of equilibrium: . If , then each solution is an equilibrium point of (1.1).

## 2. Stochastic Perturbations, Centering, and Linearization—Definitions and Auxiliary Statements

Let be a probability space and let be a nondecreasing family of sub--algebras of , that is, for , let be the expectation, let , , be a sequence of -adapted mutually independent random variables such that , .

As it was proposed in [39, 40] and used later in [41–43] we will suppose that (1.1) is exposed to stochastic perturbations which are directly proportional to the deviation of the state of system (1.1) from the equilibrium point . So, (1.1) takes the form

Note that the equilibrium point of (1.1) is also the equilibrium point of (2.1).

Putting we will center (2.1) in the neighborhood of the point of equilibrium . From (2.1) it follows that

It is clear that the stability of the trivial solution of (2.2) is equivalent to the stability of the equilibrium point of (2.1).

Together with nonlinear equation (2.2) we will consider and its linear part

Two following definitions for stability are used below.

Definition 2.1.

The trivial solution of (2.2) is called stable in probability if for any and there exists such that the solution satisfies the condition for any initial function such that .

Definition 2.2.

The trivial solution of (2.3) is called mean square stable if for any there exists such that the solution satisfies the condition for any initial function such that . If, besides, , for any initial function , then the trivial solution of (2.3) is called asymptotically mean square stable.

The following method for stability investigation is used below. Conditions for asymptotic mean square stability of the trivial solution of constructed linear equation (2.3) were obtained via V. Kolmanovskii and L. Shaikhet general method of Lyapunov functionals construction [44–46]. Since the order of nonlinearity of (2.2) is more than 1, then obtained stability conditions at the same time are [47–49] conditions for stability in the probability of the trivial solution of nonlinear equation (2.2) and therefore for stability in probability of the equilibrium point of (2.1).

Lemma 2.3.

(see [44]). If

then the trivial solution of (2.3) is asymptotically mean square stable.

Put

Lemma 2.4.

(see [44]). If

then the trivial solution of (2.3) is asymptotically mean square stable.

Consider also the necessary and sufficient condition for asymptotic mean square stability of the trivial solution of (2.3).

Let and be two square matrices of dimension such that has all zero elements except for and

Lemma 2.5 ([46]).

Let the matrix equation

has a positively semidefinite solution with . Then the trivial solution of (2.3) is asymptotically mean square stable if and only if

Corollary 2.6.

For condition (2.9) takes the form

If, in particular, , then condition (2.10) is the necessary and sufficient condition for asymptotic mean square stability of the trivial solution of (2.3) for .

Remark 2.7.

Put . If , then the trivial solution of (2.3) can be stable (e.g., or ), unstable (e.g., ) but cannot be asymptotically stable. Really, it is easy to see that if (in particular, ), then sufficient conditions (2.4) and (2.6) do not hold. Moreover, necessary and sufficient (for ) condition (2.10) does not hold too since if (2.10) holds, then we obtain a contradiction

Remark 2.8.

As it follows from results of [47–49] the conditions of Lemmas 2.3, 2.4, 2.5 at the same time are conditions for stability in probability of the equilibrium point of (2.1).

## 3. Stability of Equilibrium Points

From conditions (2.4), (2.6) it follows that . Let us check if this condition can be true for each equilibrium point.

Suppose at first that condition (1.7) holds. Then (2.1) has two points of equilibrium and defined by (1.8) and (1.9) accordingly. Putting via (2.5), (2.3), (1.3), we obtain that corresponding and are

So, . It means that the condition holds only for one from the equilibrium points and . Namely, if , then ; if , then ; if , then . In particular, if , then via Remark 1.1 and (2.3) we have , . Therefore, if , if , if .

So, via Remark 2.7, we obtain that equilibrium points and can be stable concurrently only if corresponding and are negative concurrently.

Suppose now that condition (1.10) holds. Then (2.1) has only one point of equilibrium (1.11). From (2.5), (2.3), (1.3), (1.11) it follows that corresponding equals

As it follows from Remark 2.7 this point of equilibrium cannot be asymptotically stable.

Corollary 3.1.

Let be an equilibrium point of (2.1) such that

Then the equilibrium point is stable in probability.

The proof follows from (2.3), Lemma 2.3, and Remark 2.8.

Corollary 3.2.

Let be an equilibrium point of (2.1) such that

Then the equilibrium point is stable in probability.

Proof.

Via (1.3), (2.3), (2.5) we have

Rewrite (2.6) in the form

and show that it holds. From (3.4) it follows that . Via we have

So,

It means that the condition of Lemma 2.4 holds. Via Remark 2.8 the proof is completed.

Corollary 3.3.

An equilibrium point of the equation

is stable in probability if and only if

The proof follows from (2.3), (2.10), (2.11).

## 4. Examples

Example 4.1.

Consider (3.10) with , , . From (1.3) and (1.7)–(1.9) it follows that , and for any fixed and such that equation (3.10) has two points of equilibrium

In Figure 1, the region where the points of equilibrium are absent (white region), the region where both points of equilibrium and are there but unstable (yellow region), the region where the point of equilibrium is stable only (red region), the region where the point of equilibrium is stable only (green region), and the region where both points of equilibrium and are stable (cyan region) are shown in the space of (). All regions are obtained via condition (3.11) for . In Figures 2, 3 one can see similar regions for and , accordingly, that were obtained via conditions (3.11), (3.12). In Figure 4 it is shown that sufficient conditions (3.3) and (3.4), (3.5) are enough close to necessary and sufficient conditions (3.11), (3.12): inside of the region where the point of equilibrium is stable (red region) one can see the regions of stability of the point of equilibrium that were obtained by condition (3.3) (grey and green regions) and by conditions (3.4), (3.5) (cyan and green regions). Stability regions obtained via both sufficient conditions of stability (3.3) and (3.4), (3.5) give together almost whole stability region obtained via necessary and sufficient stability conditions (3.11), (3.12).

Consider now the behavior of solutions of (3.10) with in the points , , , of the space of () (Figure 1). In the point with , both equilibrium points and are unstable. In Figure 5 two trajectories of solutions of (3.10) are shown with the initial conditions , , and , . In Figure 6 two trajectories of solutions of (3.10) with the initial conditions , , and , are shown in the point with , . One can see that the equilibrium point is stable and the equilibrium point is unstable. In the point with , the equilibrium point is unstable and the equilibrium point is stable. Two corresponding trajectories of solutions are shown in Figure 7 with the initial conditions , , and , . In the point with , both equilibrium points and are stable. Two corresponding trajectories of solutions are shown in Figure 8 with the initial conditions , , and , . As it was noted above in this case, corresponding and are negative: and .

Example 4.2.

Consider the difference equation

Different particular cases of this equation were considered in [2–5, 16, 22, 23, 37].

Equation (4.2) is a particular case of (2.1) with

Suppose firstly that and consider two cases: (1) , (2) . In the first case,

In the second case,

In both cases, Corollary 3.1 gives stability condition in the form or

with

Corollary 3.2 in both cases gives stability condition in the form or (4.6) with

Since then condition (4.6), (4.7) is better than (4.6), (4.8).

In the case , Corollary 3.3 gives stability condition in the form

or

In particular, from (4.10) it follows that for , (this case was considered in [3, 23]) the equilibrium point is stable if and only if . Note that in [3] for this case the condition only is obtained.

In Figure 9 four trajectories of solutions of (4.2) in the case , , , are shown: (1) , , , (red line, stable solution); (2) , , , (brown line, unstable solution); (3) , , , (blue line, unstable solution); (4) , , , (green line, stable solution).

In the case , , Corollary 3.3 gives stability condition in the form

or

For example, from (4.12) it follows that for , (this case was considered in [22, 37]), the equilibrium point is stable if and only if . In Figure 10 four trajectories of solutions of (4.2) in the case , , , are shown: (1) , , , (red line, stable solution); (2) , , , (brown line, unstable solution); (3) , , , (blue line, unstable solution); (4) , , , (green line, stable solution).

Via simulation of a sequence of mutually independent random variables consider the behavior of the equilibrium point by stochastic perturbations. In Figure 11 one thousand trajectories are shown for , , , , . In this case, stability condition (4.12) holds () and therefore the equilibrium point is stable: all trajectories go to . Putting , we obtain that stability condition (4.12) does not hold (). Therefore, the equilibrium point is unstable: in Figure 12 one can see that 1000 trajectories fill the whole space.

Note also that if goes to zero all obtained stability conditions are violated. Therefore, by conditions the equilibrium point is unstable.

Example 4.3.

Consider the equation

(its particular cases were considered in [18, 19, 35]). Equation (4.13) is a particular case of (2.1) with , , , . From (1.7)–(1.9) it follows that by condition it has two equilibrium points

For equilibrium point sufficient conditions (3.3) and (3.4), (3.5) give

From (3.11), (3.12) it follows that an equilibrium point of (4.13) is stable in probability if and only if

For example, for from (4.15) we obtain

From (4.16) it follows

Similar for from (4.15) we obtain

From (4.16) it follows

Put, for example, . Then (4.13) has two equilibrium points: , . From (4.15)-(4.16) it follows that the equilibrium point is unstable and the equilibrium point is stable in probability if and only if

Note that for particular case , , , in [35] it is shown that the equilibrium point is locally asymptotically stable if ; and for particular case , , , in [18] it is shown that the equilibrium point is locally asymptotically stable if . It is easy to see that both these conditions follow from (4.21).

Similar results can be obtained for the equation that was considered in [1].

In Figure 13 one thousand trajectories of (4.13) are shown for , , , , , . In this case stability condition (4.21) holds () and therefore the equilibrium point is stable: all trajectories go to zero. Putting , we obtain that stability condition (4.21) does not hold (). Therefore, the equilibrium point is unstable: in Figure 14 one can see that 1000 trajectories by the initial condition , fill the whole space.

Example 4.4.

Consider the equation

that is a particular case of (3.10) with , , , , , . As it follows from (1.4), (1.7)–(1.9) by conditions , , (4.22) has two equilibrium points

From (3.11), (3.12) it follows that an equilibrium point of (4.22) is stable in probability if and only if

Substituting (4.23) into (4.24), we obtain stability conditions immediately in the terms of the parameters of considered equation (4.22): the equilibrium point is stable in probability if and only if

the equilibrium point is stable in probability if and only if

Note that in [24] equation (4.18) was considered with and positive , . There it was shown that equilibrium point is locally asymptotically stable if and only if that is a part of conditions (4.25).

In Figure 15 the region where the points of equilibrium are absent (white region), the region where the both points of equilibrium and are there but unstable (yellow region), the region where the point of equilibrium is stable only (red region), the region where the point of equilibrium is stable only (green region) and the region where the both points of equilibrium and are stable (cyan region) are shown in the space of (,). All regions are obtained via conditions (4.25), (4.26) for . In Figures 16 similar regions are shown for .

Consider the point (Figure 15) with , . In this point both equilibrium points and are unstable. In Figure 17 two trajectories of solutions of (4.22) are shown with the initial conditions , and , . In Figure 18 two trajectories of solutions of (4.22) with the initial conditions , and , are shown in the point (Figure 15) with . One can see that the equilibrium point is stable and the equilibrium point is unstable. In the point (Figure 15) with , the equilibrium point is unstable and the equilibrium point is stable. Two corresponding trajectories of solutions are shown in Figure 19 with the initial conditions and , . In the point (Figure 15) with , both equilibrium points and are stable. Two corresponding trajectories of solutions are shown in Figure 20 with the initial conditions , and , .

Consider the behavior of the equilibrium points of (4.22) by stochastic perturbations with . In Figure 21 trajectories of solutions are shown for , (the point in Figure 16) with the initial conditions , and . One can see that the equilibrium point (red trajectories) is stable and the equilibrium point (green trajectories) is unstable. In Figure 22 trajectories of solutions are shown for , (the point in Figure 16) with the initial conditions , and , . In this case both equilibrium points (red trajectories) and (green trajectories) are stable.

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Paternoster, B., Shaikhet, L. Stability of Equilibrium Points of Fractional Difference Equations with Stochastic Perturbations.
*Adv Differ Equ* **2008**, 718408 (2008). https://doi.org/10.1155/2008/718408

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DOI: https://doi.org/10.1155/2008/718408