Abstract
The article is concerned with large time behavior of solution to second-order fractal difference equation with positive fuzzy parameters
Keywords
Introduction
Difference equations or discrete systems are one of the most important classical dynamical models in applied mathematics, which have wide applications including computer science, biology, economics, infectious disease, etc (see [18–21, 33]). In the past decades, many mathematicians are interested in describing large time behavior of difference equations such as the oscillatory behavior, periodicity, bifurcation, stability, chaos, and the boundedness. Moreover similar results on large time behaviors of solution have been obtained for many nonlinear difference equation system [7, 10, 22, 24, 35, 38, 39].
In real world, the parameters of model often stem from statistical data, based on the experimental data obtained and the statistical method adopted. These models, even in the classic way, often suffer from uncertainty (fuzzy uncertainty) that can be manifested in state variables, initial conditions and system parameters.
In fact, many experts have accepted to cope with uncertainty, and they also affirm the fact that uncertainty often influences large time behaviors of the solution of mathematical model. Contributing mathematical model of the real life problems in such method, it often involves intrinsically uncertainty or vagueness. Up to now, the fuzzy set instituted by Zadeh [16] has become a powerful tool to various theories and many applications including fuzzy difference equations (FDE) and fuzzy differential equations.
FDE is a special type difference equation that the initial values, state variable, or parameters of model are fuzzy numbers and its solutions are a sequence of fuzzy numbers. Since FDE can be used to analyze the phenomena with inherent uncertainty, the study on this model has become an important topic both in theory and in its applications. In recent years, more and more literatures have been published on large time behavior of FDE (see [1, 2, 4, 8, 9, 11–13, 15, 25–32, 34, 36, 37, 40]).
As far as FDE is concerned, let’s briefly review its development. In 1996, Deeba, Korvin, and Koh [8] presented a FDE and its application in economic. In 1999, Deeba and Korvin [9] investigated subsequently the levels of carbon dioxide in blood by FDE model. Papaschinopoulos and Papadopoulos [11, 12] studied first-order and high-order fractal FDE respectively. It is important to point out that Lakshmikantham and Vatsala [37] put forward the basic theory of FDE. Constructing a Lyapunov type function, they proved the comparison theorem and stability principle of FDE in terms of crisp difference equation. As we all know, a classical way to consider uncertainty is the fuzzification of difference equations. The operators such as addition, subtraction, multiplication, and division followed by Zadeh extension principle. There are many literatures on large time behavior of FDE in [15, 26–28, 34]. For example, using Zadeh extension principle, Zhang, Yang and Liao [28] were concerned with large time behaviors of first-order Riccati FDE.
However, some researchers argue that the operations are not invertible including the standard Minkowski addition and multiplication. To overcome these defects, Stefanini [17] proposed a generation of division named g-division and founded a new way to study FDE. Since then, utilizing g-division, many scholars [3, 29–32] studied some nonlinear FDE and obtained desirable results. Compared with using Zadeh extension principle, the merits of g-division is that it can decrease the singularity of fuzzy solution due to reduction of the length of the support interval.
Inspired with the previous works, utilizing g-division, in this article, we further explore large time behaviors of solutions to a second-order fractal FDE.
The outline of this paper is arranged as follows. Sect.2 introduces the basic concepts of fuzzy set used throughout this paper. Section 3 investigates the large time behaviors of solutions to the second-order fractal FDE by means of g-division of fuzzy numbers. Section 4 gives two numerical simulation examples using MATLAB to support our theoretical analysis. Section 5 draws a general conclusion and future work.
In the section, we first review some basic concepts used in the sequel, for more detail, readers can refer to [3, 8, 16].
A function defined as U : R → [0, 1] is said to be a fuzzy number if it is normal, convex, upper semicontinuous, and compactly support on R.
For α ∈ (0, 1], the α-level of fuzzy number U is denoted by [U] α = {x ∈ R : U (x) ≥ α}, and for α = 0, the support of U is written as
It is clear that the [U] α = [Ul,α, Ur,α], is a bounded closed interval in R, where Ul,α (resp. Ur,α) denote the left-hand (resp. right-hand) endpoint of the α-level sets [U] α . U is said to be a positive fuzzy number if suppU ⊂ (0, ∞) . Particularly, if U is a trivial positive fuzzy number (positive real number), then the α-level sets [U] α = [U, U] , for all α ∈ (0, 1] .
Let U, V be fuzzy numbers with [U] α = [Ul,α, Ur,α] , [V] α = [Vl,α, Vr,α], the norm of fuzzy numbers space is defined by
All fuzzy numbers with addition and multiplication is represented by
The definition of g-division of fuzzy numbers is from [17].
Given
Case I. if Ul,αVr,α ≤ Ur,αVl,α, ∀ α ∈ [0, 1] , then
Case II. if Ul,αVr,α ≥ Ur,αVl,α, ∀ α ∈ [0, 1] , then
The definition of the boundedness and persistence is as follows (see [11, 12]).
A positive sequence of fuzzy numbers {x n } is bounded (resp. persistence) provided that there is a Q > 0 (resp. P > 0) such that
A positive sequence of fuzzy numbers {x
n
} is bounded and persistence provided that there exist P > 0, Q > 0 such that
A positive sequence of fuzzy numbers {x n } , n = 1, 2, ⋯, is unbounded provided that the norm ∥x n ∥ , n = 1, 2, ⋯ , is an unbounded sequence.
x n is called a positive fuzzy solution of FDE (1) provided that {x n } is a positive sequence of fuzzy numbers satisfying FDE (1).
Let
(i) u l (α) is nondecreasing and left continuous;
(ii) u r (α) is nonincreasing and left continuous;
(iii) u l (1) ≤ u r (1).
Conversely, for any functions h (α) and g (α) defined on (0, 1] which satisfy (i)-(iii) in the above, there exists a unique
In the section, to find large time behavior of positive fuzzy solution to FDE (1), we first give the existence of positive fuzzy solution of FDE (1) by virtue of Lemma 2.1.
Noting Remark 2.1, utilizing g-division of fuzzy numbers, One of the following two cases may occur.
Case I
Case II
It is clear that there is a unique solution (xn,l,α, xn,r,α) for any initial values (xk,l,α, xk,r,α) , k = -1, 0, α ∈ (0, 1].
We only need to show that, for α ∈ (0, 1] , n ∈ N+, [xn,l,α, xn,r,α] makes certain the positive fuzzy solution x n of FDE (1) with the initial values x i (i = 0, - 1), and satisfying (3).
From [8], since
Secondly, we will show that
Hence from (9) and (10), one has, for n = 1, α ∈ (0, 1],
Next we will show that x
n
is the solution of FDE (1) with the initial values
Suppose that,
If Case II occurs, The proof is similar to the proof above. This completes the proof of Theorem 3.1.
In fact, to obtain the results on large time behaviors of positive fuzzy solution for FDE (1). Case I and Case II are considered respectively.
In this subsection, using g-division of fuzzy numbers, we are concerned with large time behaviors of positive fuzzy solution to FDE (1) under Case I. To obtain the theoretic results, firstly, we give the following lemma.
(i) Every positive solution y
n
of (15) satisfies
(ii) From (15), it is easy to obtain that the unique positive equilibrium of (15) is
From (17), suppose that
(i) Every positive fuzzy solution x n of FDE (1) is bounded and persistent.
(ii) FDE (1) has a unique positive equilibrium
(iii) Every positive fuzzy solution x
n
of FDE (1) tends to the positive equilibrium
From (10), (25),(26), and (3), we have, for n = 1, 2, ⋯ ,
From (27), it follows that, for n ≥ 1,
(ii) Suppose that (xl,α, xr,α) satisfies the following system
(iii) From (30), one has that
Let ɛ > 0, suppose that
On the other hand, let x
n
be a positive fuzzy solution of FDE (1) satisfying
Secondly, if Case II holds true, from (5), then (xn,l,α, xn,r,α) satisfies the following family of systems of parametric crisp difference equations, for α ∈ (0, 1] , n = 0, 1, 2, ⋯ ,
In order to find large time behaviors of FDE (1), we give the following lemma.
(i) Every positive solution (y n , z n ) of (44) is persistence and bounded.
(ii) The system exists a unique positive equilibrium
(ii) From (44), one has that the unique positive equilibrium
On the other hand, since y
n
, z
n
are bounded and persistence, suppose that
Then from (44), one has
Furthermore, (10) and (23) hold, then the following propositions are true.
(i) Every positive fuzzy solution x n of FDE (1) is bounded and persistent.
(ii) FDE (1) has a unique positive equilibrium
(iii) Every positive fuzzy solution x
n
of FDE (1) tends to the positive equilibrium
(ii) Suppose that the positive fuzzy number
It is easy to show that xl,α, xr,α, α ∈ (0, 1] makes certain a positive fuzzy number
(iii) Let x
n
be a positive fuzzy solution of FDE (1) such that Case II occurs. i.e. (43) are true. Since Bl,α > K > 1, using Lemma 3.2 to system (43), one has
In this section, we give the following two examples to verify the correctness of theoretic results.

The large time behavior of FDE (1).

The positive solution of system (73) at α = 0 and α = 0.25 .

The positive solution of system (73) at α = 0.75 and α = 1 .
From (74), (75) and (76), one has

The large time behavior of FDE (1).

The positive solution of system (82) at α = 0 and α = 0.25.

The positive solution of system (82) at α = 0.75 and α = 1.
In this paper, using g-division of fuzzy number, we explored large time behaviors of second order fractal FDE
(1) Provided that Bl,α > 1, and (Al,α + xn,l,α) (Br,α + xn-1,r,α) ≤ (Ar,α + xn,r,α) (Bl,α + xn-1,l,α) , α ∈ (0, 1]. Case I occurs, then the positive fuzzy solution x n is bounded and persistence, and it tends to the unique equilibrium x as n → ∞ .
(2) Provided that Bl,α > 1, and (Ar,α + xn,r,α) (Bl,α + xn-1,l,α) ≤ (Al,α + xn,l,α) (Br,α + xn-1,r,α) , α ∈ (0, 1]. Case II occurs, then the positive fuzzy solution x n is bounded and persistence, and it tends to the unique equilibrium x as n → ∞ .
Up to now, due to lack of available theoretical tools, some complex dynamic behaviors of fuzzy discrete model have not been reported such as oscillation property, the existence of periodic solution and bifurcation. These dynamical behaviors are worth further discussion. We will explore the research on large time behavior of discrete population model or discrete economical model with fuzzy uncertainty conditions.
Footnotes
Acknowledgment
This work was financially supported by Guizhou Scientific and Technological Platform Talents (GCC [2022]020-1), Scientific Research Foundation of Guizhou Provincial Department of Science and Technology ([2022]021, [2022]026), and Scientific Climbing Programme of Xiamen University of Technology (XPDKQ20021), Postgraduate Research Foundation of Guizhou University of Finance and Economics(2022ZXSY139),Scientific Research Foundation of Guizhou University of Finance and Economics(2022ZCZX076).
