Formulas and properties of some class of nonlinear di

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We obtain the formulas of the solutions of the recursive sequences ...... and N. Taskara, On the Solutions of Di erence Equation Systems with Padovan Num-.
J. COMPUTATIONAL ANALYSIS AND APPLICATIONS, VOL. 24, NO.8, 2018, COPYRIGHT 2018 EUDOXUS PRESS, LLC

Formulas and properties of some class of nonlinear di erence equations E. M. Elsayed1 2, Faris Alzahrani1 , and H. S. Alayachi1 1 Mathematics Department, Faculty of Science, King Abdulaziz University, P. O. Box 80203, Jeddah 21589, Saudi Arabia. 2 Department of Mathematics, Faculty of Science, Mansoura University, Mansoura 35516, Egypt. E-mails: [email protected], [email protected], [email protected]. ABSTRACT We obtain the formulas of the solutions of the recursive sequences +1

5

=

4 (±1 ±

5)

=0 1

where the initial conditions are arbitrary non zero real numbers. Also, we discuss and illustrate the stability of the solutions in the neighborhood of the critical points and the periodicity of the considered equations. Keywords: equilibrium point, recursive sequences, periodicity. Mathematics Subject Classification: 39A10.

– – – – – – – – – – – – – – – – – – – – – –

1. INTRODUCTION In recent years, the qualitative study of di erence equations has become an active research area among a considerable number of mathematicians. Some economical and biological examples can be seen in [9,36,40,47,48,54]. It is commonly known that nonlinear di erence equations are able to produce and present sophisticated behaviors regardless their orders. Some articles show that a great e ort has been done to demonstrate and explore the dynamics of nonlinear di erence equations (see [40]-[61]). In fact, investigating these equations is a challenge and still new in the mathematical world. It is strongly believed that the rational di erence equations are signiÞcant in their own right. Abo-Zeid and Cinar [1] illustrated the global stability, cyclical behavior, oscillation of all acceptable solutions of the equation 1 +1 = 2 In [7], [8] Cinar considered the solutions of the equations +1

=

1

1+

+1

1

=

1

1+

1

A. El-Moneam, and Alamoudy [16] examined the positive solutions of the equation in terms of its periodicity, boundedness and the global stability. The considered di erence equation is given by +1

=

+

1+

2+

3+

4

1+

2+

3+

4

Khatibzadeh and Ibrahim [42] studied the boundedness, asymptotic stability, oscillatory behavior and discovered the closed form of solutions of the equation

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E. M. Elsayed et al 1517-1531

J. COMPUTATIONAL ANALYSIS AND APPLICATIONS, VOL. 24, NO.8, 2018, COPYRIGHT 2018 EUDOXUS PRESS, LLC

+1

=

1

+

+

1

Simsek et al. [49] has found and explored solutions for the recursive formula 3

=

+1

1+

1

For other related papers, see [25— 46]. We analyze and explore the solutions of the following nonlinear recursive equation +1

5

=

4(±1

±

=0 1

5)

(1)

with conditions posed on the initial values are arbitrary non zero real numbers. Also, we will survey some dynamic behaviors of its solutions. The linearized equation of equation +1

about the equilibrium

= (

)

1

=0 1

(2)

is the linear di erence equation +1

=

P

(

)

=0

Theorem A [43]: Assume that =1 2 and {0 1 2 condition for the asymptotic stability of the di erence equation +

+

1

+

1

+

+

=0

2. THE FIRST EQUATION

+1

P

}. Then

=1 |

|

1 is a su cient

=0 1 5

=

4 (1+

5)

This section is devoted to give a speciÞc solution of the Þrst di erence equation which is +1

Theorem 2.1. Let { 10

5

=

10

3

=

10

1

=

10 +1

=

}

5

=

4 (1

=

¶ Y1 µ 1 + (10 ) 1 + (10 + 5) =0 µ 1 Y 1 + (10 + 2) ¶ 1 + (10 + 7) =0 µ 1 Y 1 + (10 + 4) ¶ 1 + (10 + 9) =0 Y1 µ 1 + (10 + 6) (1 + ) 1 + (10 + 11)

where we put

(1 + 3 5

=

(3)

5)

be a solution of Eq.(3). Then

= 5

Y1 µ 1 + (10 + 1) ¶ 1 + (10 + 6) =0 µ 1 Y 1 + (10 + 3) ¶ 10 2 = 1 + (10 + 8) =0 µ 1 Y 1 + (10 + 5) ¶ = 10 1 + (10 + 10) =0 ¶ Y1 µ 1 + (10 + 7) = 10 +2 (1 + 2 ) 1 + (10 + 12) 10

=0

10 +3

+



=0

=

3

=

=

=0

Y1 µ 1 + (10 + 8) ) 1 + (10 + 13) 4

4

2

=

1518

10 +4

1

=

=

(1 + 4 0

Y1 µ 1 + (10 + 9) ) 1 + (10 + 14) =0

¶ ¶

=

E. M. Elsayed et al 1517-1531

J. COMPUTATIONAL ANALYSIS AND APPLICATIONS, VOL. 24, NO.8, 2018, COPYRIGHT 2018 EUDOXUS PRESS, LLC

Proof: The result holds for

10

10

10

15

=

13

=

11

=

10

9

=

10

7

=

= 0. Assume that

Y2 µ 1 + (10 ) 1 + (10 + 5) =0 µ 2 Y 1 + (10 + 2) 1 + (10 + 7) =0 µ 2 Y 1 + (10 + 4) 1 + (10 + 9) =0

0 and our assumption true for



1. Then;

Y2 µ 1 + (10 + 1) ¶ 1 + (10 + 6) =0 µ 2 Y 1 + (10 + 3) ¶ = 10 12 1 + (10 + 8) =0 ¶ 2 Y µ 1 + (10 + 5) = 10 10 1 + (10 + 10) =0

10





Y2 µ 1 + (10 + 6) ¶ (1 + ) =0 1 + (10 + 11) Y2 µ 1 + (10 + 8) ¶ (1 + 3 ) =0 1 + (10 + 13)

10

10

14

=

Y2 µ 1 + (10 + 7) ¶ 8 = (1 + 2 ) =0 1 + (10 + 12) Y2 µ 1 + (10 + 9) ¶ 6 = (1 + 4 ) =0 1 + (10 + 14)

Now, it follows from Eq.(3) that 10

5

10

=

10(1

10

+

6 10

11

10

6 10

(1+4

=

=

=

=

=

"

Y2 ³

)

11) Y2 ³

# "=0 ´ 1+

1+(10 +5) 1+(10 +10)

=0

´ Y2 ³ 1+(10 +4)

1+(10 +9) 1+(10 +14)

1+(10 +9)

=0

(1+4

)

Y2 ³

1+(10 +9) 1+(10 +14)

=0

´

´ Y2 ³ ´ 1+(10 +4) 1+(10 +9)

=0

¶ Y2 µ 1 + (10 + 4) (1 + 4 ) =0 1 + (10 + 14) " 2µ #" Y 1 + (10 + 5) ¶ Y2 µ 1 + (10 + 4) 1+ 1 + (10 + 10) (1 + 4 ) =0 1 + (10 + 14) =0 µ ¶ " "

1 + (10 6) # Y2 µ 1 + (10 + 5) ¶ 1+ 1 + (10 + 10) 1 + (10

6)

=0

Y2 µ 1 + (10 + 5) 1 + (10 + 10) =0

[1 + (10

¶#

[1 + (10

6)

Y2 µ 1 + (10 + 10) ] 1 + (10 + 5)

5)

=0

+



=

#

¶#

¸ ]

¶ Y1 µ 1 + (10 ) 1 + (10 + 5) =0

Also, we have 10

4

10

= 10

9 (1

1519

+

5 10

10

10

5 10

10)

E. M. Elsayed et al 1517-1531

J. COMPUTATIONAL ANALYSIS AND APPLICATIONS, VOL. 24, NO.8, 2018, COPYRIGHT 2018 EUDOXUS PRESS, LLC

= "

Y1 ³

1+(10 ) 1+(10 +5)

=0

(1+

Y2 ³

)

1+(10 +6) 1+(10 +11)

=0

"

=

(1+

)

Y2 ³ =0

#" ´

´ Y2 ³

1+(10 +5) 1+(10 +10)

=0

1+

µ

Y1 ³

´ Y2 ³

1+(10 ) 1+(10 +5)

=0

1 + (10 5) # ´ 1+(10 +6) 1+ 1+(10 +11)

1+(10 +5) 1+(10 +10)

=0



1

´

1 + (10

´

#

¸

5)

"

# Y2 µ 1 + (10 + 6) ¶ [1 + (10 5) + ] (1 + ) =0 1 + (10 + 11) Y2 µ 1 + (10 + 11) ¶ Y1 µ 1 + (10 + 1) (1 + ) = [1 + (10 4) ] =0 1 + (10 + 6) 1 + (10 + 6) =0

=

=



Similarly 10

3

10

= 10

=

=

"

"

=

=

=

(1+2

)

8(1

"

1 + (10 + 6) #" 2 ³ Y 1+(10 +7) ´ Y1 µ 1 + 1+(10 +12)

"

(1+2

)

=0

Y2 ³ =0

1 (1+2

)

Y2 ³

µ

9)

1+(10 +7) 1+(10 +12)

# ´

1+(10 +7) 1+(10 +12)

# ´

)

Y2 ³ =0

[1 + (10

(1 + (10 + 6)

=0

1 + (10

4)

3)

]

(1 + (10 + 6)

=0

)

#

¶¸

4)

+

#

)

¶ Y2

1 + (10 + 6)

= [1 + (10

´

=0



1 + (10 4) # µ ´ 1+(10 +7) 1+ 1+(10 +12)

=0

1 (1+2

4 10

¶ Y2

=0

"

9

10

=0

Y1 µ =0

)

4 10

Y1 µ 1 + (10 + 1) ¶ Y2 µ 1 + (10 + 6) ¶ (1+ ) 1 + (10 + 6) 1 + (10 + 11) =0 =0 # " 2 1 ³ ´ ³ Y 1+(10 +7) Y 1+(10 +1) ´ Y2 ³ 1+(10 +6) 1 + 1+(10 +12) 1+(10 +6) (1+ ) 1+(10 +11) =0

(1+2

+

] Y1 µ 1 + (10 + 2) 1 + (10 + 7) =0



Similarly, one can simply find the other relations. Thus, the proof is done. Theorem 2.2. The unique equilibrium point of Eq.(3) is the number zero which is not locally asymptotically stable.

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E. M. Elsayed et al 1517-1531

J. COMPUTATIONAL ANALYSIS AND APPLICATIONS, VOL. 24, NO.8, 2018, COPYRIGHT 2018 EUDOXUS PRESS, LLC

Proof: The equilibrium points of Eq.(3) obtained by 2

¡

= 4

Arranging the previous equation gives Let

: (0

)3

(0

= 0 Thus

3

1+

=0

¢

) be a function takes the form (

)=

(1 +

)

Therefore (

)=

(

2

(1 +

)

)=

2 (1

+

(

)

)=

2

(1 +

)

So (

)=1

(

)=1

(

)=1

Then by using Theorem A the proof follows. Example 1. We assume

5

=6

4

= 11

3

=3

2

=2

1

=18

0

=

7. See Fig. 1.

plot of x(n+1)=x(n)x(n 5)/(x(n 4)(1+x(n)x(n 5)) 12 10 8 6 4 2 0 2 4 6 8

0

10

20

30

40

50 n

60

70

80

90

100

Figure 1. Example 2. See Fig. 2, since

5

=16

4

=12

1521

3

=

3

2

= 7

1

=18

0

= 3.

E. M. Elsayed et al 1517-1531

J. COMPUTATIONAL ANALYSIS AND APPLICATIONS, VOL. 24, NO.8, 2018, COPYRIGHT 2018 EUDOXUS PRESS, LLC

plot of x(n+1)=x(n)x(n 5)/(x(n 4)(1+x(n)x(n 5)) 3

2

1

0

1

2

3

0

10

20

30

40

50 n

60

70

80

90

100

Figure 2.

3. THE SECOND EQUATION

+1

=

5 4(

1+

5)

This section is devoted to obtain the solution of the di erence equation which is +1

where

0

5

6= 1

Theorem 3.1. Let {

}

= 5

4(

1+

(4)

5)

be a solution of Eq.(4). Then for

10

5

=

10

3

=

10 1

=

10 +1

=

10 +3

=

Proof: The result holds for

5

=

10

4

( 1+

)

( 1+

)

10

( 1+

)

10

( 1+

)

+1

( 1+

)

+1

= 0. Assume that

= ( 1+ 2

= ( 1+

= ( 1+

10 +2

)

=

10 +4

=

) )

( 1+

)

( 1+

)

0 and that our assumption true for

1522

1. Then;

E. M. Elsayed et al 1517-1531

J. COMPUTATIONAL ANALYSIS AND APPLICATIONS, VOL. 24, NO.8, 2018, COPYRIGHT 2018 EUDOXUS PRESS, LLC

10

15

=

10

13

=

10 11

=

10

9

=

10

7

=

10

14

= ( 1+

1

)

( 1+

)

1

)

1

10

12

= ( 1+

)

1

( 1+

)

1

10

10

= ( 1+

)

1

( 1+

( 1+

1

( 1+

10

)

( 1+

10

)

=

8

6

)

( 1+

=

1

)

It follows from (4) that 10

5

10

=

10(

10

10

4

6 10

1+

11

10

10

= 10

9(

= ( 1+

5 10

1+

=

( 1+ ( 1+

)

1+

1[

)

1

1+

]

=

( 1+

)

10)

5 10

) ( 1+ )

)

( 1+

10

10

( 1+ ) ¸ 1+

= ( 1+

11)

6 10

( 1+

)

)

( 1+

)

1

¸

( 1+ ) = ( 1+ [1 + ]

¸=

)

Similarly one can simply prove the other relations. Theorem 3.2. Eq.(4) has a period ten solution i ½

= 2 and will be in the following form ¾

Proof: Firstly, assume that there exists a period ten solution ½

¾

of Eq.(4). Then, we can notice from the solution of Eq.(4) that

= = =

( 1+

)

( 1+ ) ( 1+ )

= ( 1+

)

= ( 1+ =

=

( 1+

)

( 1+

=

)

+1

= ( 1+

)

( 1+

) =

)

+1

( 1+

)

or, ( 1+

1523

) =1

E. M. Elsayed et al 1517-1531

J. COMPUTATIONAL ANALYSIS AND APPLICATIONS, VOL. 24, NO.8, 2018, COPYRIGHT 2018 EUDOXUS PRESS, LLC

Then =2 Secondly, suppose that

10

5 10

= 2 Then, it is easily seen from the solution of Eq.(4) that

=

10

4

=

=

10 +1

=

10

3

=

10

10 +2

2

=

=

10 1

10 +3

=

=

10 +4

=

Thus, the periodic solution of period ten is obtained and this proves the theorem. 3

Theorem 3.3. Eq.(4) has two equilibrium points which are 0 asymptotically stable.

2 and these equilibrium points are not locally

Proof: The equilibrium points of Eq.(4) can be written in the following form 2

¡

= Arranging this gives 2

¡

1+

2

¢

2

1+

2

=

2

Therefore, the fixed points are 0 ± 2 Let

: (0

)3

(0

¢

¡

¢ 2 =0

2

) be a function defined by (

)=

( 1+

)

Then it follows that (

) =

(

) =

(

) =

( 1+ 2(

2

)

1+

( 1+

) )2

It can be seen that (

)=

1

(

) = ±1

(

)=

1

Then by using Theorem A the proof follows. Example 3. We consider

5

= 8

4

=17

3

= 3

1524

2

=2

1

=18

0

= 7 See Fig. 3.

E. M. Elsayed et al 1517-1531

J. COMPUTATIONAL ANALYSIS AND APPLICATIONS, VOL. 24, NO.8, 2018, COPYRIGHT 2018 EUDOXUS PRESS, LLC

plot of x(n+1)=x(n)x(n 5)/(x(n 4)( 1+x(n)x(n 5)) 50

40

30

20

10

0

10

20

30

0

5

10

15

20

25 n

30

35

=2

1

40

45

50

Figure 3. Example 4. See Fig. 4, since

5

=8

4

=17

3

= 3

2

=18

0

= 1 4.

plot of x(n+1)=x(n)x(n 5)/(x(n 4)( 1+x(n)x(n 5)) 8

7

6

5

4

3

2

1

0

0

5

10

15

20

25 n

30

35

40

45

50

Figure 4.

4. THE THIRD EQUATION

+1

=

5 4 (1

5)

In this section we will obtain and present the solution of the third di erence equation which is +1

=

5 4 (1

1525

(5)

5)

E. M. Elsayed et al 1517-1531

J. COMPUTATIONAL ANALYSIS AND APPLICATIONS, VOL. 24, NO.8, 2018, COPYRIGHT 2018 EUDOXUS PRESS, LLC

Theorem 4.1. Let {

}

10

5

=

10

3

=

10

1

=

10 +1

=

10 +2

=

10 +3

=

10 +4

=

= 5

be a solution of Eq.(5). Then for

=0 1

¶ Y1 µ 1 (10 ) Y1 µ 1 (10 + 1) ¶ = 10 4 1 (10 + 5) 1 (10 + 6) =0 =0 µ ¶ µ Y1 1 (10 + 2) Y1 1 (10 + 3) ¶ = 10 2 1 (10 + 7) 1 (10 + 8) =0 =0 µ ¶ µ ¶ Y1 1 (10 + 4) Y1 1 (10 + 5) 10 = 1 (10 + 9) 1 (10 + 10) =0 =0 Y1 µ 1 (10 + 6) ¶ (1 ) =0 1 (10 + 11) Y1 µ 1 (10 + 7) ¶ (1 2 ) =0 1 (10 + 12) Y1 µ 1 (10 + 8) ¶ (1 3 ) =0 1 (10 + 13) Y1 µ 1 (10 + 9) ¶ (1 4 ) =0 1 (10 + 14)

Theorem 4.2. The unique critical point of Eq.(5) is the number zero which is not locally asymptotically stable. Example 5. Suppose that

5

=8

4

=17

3

= 3

2

=2

1

=18

0

= 1 4 see Fig. 5.

plot of x(n+1)=x(n)x(n 5)/(x(n 4)(1 x(n)x(n 5)) 8

6

4

2

0

2

4

0

5

10

15

20

25 n

30

35

40

45

50

Figure 5. Example 6. See Fig. 6 since

5

=

7

4

=15

3

1526

=

3

2

=2

1

= 12

0

= 4.

E. M. Elsayed et al 1517-1531

J. COMPUTATIONAL ANALYSIS AND APPLICATIONS, VOL. 24, NO.8, 2018, COPYRIGHT 2018 EUDOXUS PRESS, LLC

plot of x(n+1)=x(n)x(n 5)/(x(n 4)(1 x(n)x(n 5)) 12 10 8 6 4 2 0 2 4 6 8

0

5

10

15

20

25 n

30

35

40

45

50

Figure 6.

5. THE FOURTH EQUATION

+1

5

=

4(

1

5)

Now, we will explore and discover the solution of the following di erence equation +1

where

5 0

6=

=

5 4(

1

=0 1

5)

(6)

1

Theorem 5.1. Let { } = 5 be a solution of Eq.(6). Then Eq.(6) has unboundedness solution (except in the case if = 2) and for = 0 1 10

5

=

10

3

=

10 1

=

10 +1

=

10 +3

=

10

4

( 1

)

( 1

)

10

( 1

)

10

( 1

)

+1

( 1

)

+1

= ( 1 2

= ( 1

= ( 1

10 +2

)

=

10 +4

=

Theorem 5.2. Eq.(6) has a periodic ½ ¾ solution of period ten i

=

Example 7. Consider

1

) )

( 1

)

( 1

)

2 and written in the following form

Theorem 5.3. The unique equilibrium of Eq.(6) is the number zero which is not locally asymptotically stable. 5

=

7

4

=15

3

=

3

1527

2

=2

= 12

0

= 4 see Fig. 7.

E. M. Elsayed et al 1517-1531

J. COMPUTATIONAL ANALYSIS AND APPLICATIONS, VOL. 24, NO.8, 2018, COPYRIGHT 2018 EUDOXUS PRESS, LLC

6

5

plot of x(n+1)=x(n)x(n 5)/(x(n 4)( 1 x(n)x(n 5))

x 10

4

3

2

1

0

1

2

0

5

10

15

20

25 n

30

35

40

45

50

Figure 7. Example 8. Fig. 8 illustrates the solutions when 2 7.

5

=

7

4

=15

3

=

3

2

=2

1

= 12

plot of x(n+1)=x(n)x(n 5)/(x(n 4)( 1 x(n)x(n 5)) 12 10 8 6 4 2 0 2 4 6 8

0

5

10

15

20

25 n

30

35

40

45

50

Figure 8.

1528

E. M. Elsayed et al 1517-1531

0

=

J. COMPUTATIONAL ANALYSIS AND APPLICATIONS, VOL. 24, NO.8, 2018, COPYRIGHT 2018 EUDOXUS PRESS, LLC

REFERENCES 1. R. Abo-Zeid and C. Cinar, Global behavior of the di erence equation

+1

1

=

Paran. Mat. (3s.), 31 (1) (2013), 43— 49. 2. A. M. Ahmed, and N. A. Eshtewy, Basin of attraction of the recursive sequence 3. 4. 5. 6.

Bol. Soc. 2

+1

=

+ +

+ +

1 1

Journal of Fractional Calculus and Applications, 5 (3S) (10) (2014), 1-8. M. Aloqeili, Dynamics of a rational di erence equation, Appl. Math. Comp., 176(2), (2006), 768-774. A. Asiri, E. M. Elsayed, and M. M. El-Dessoky, On the solutions and periodic nature of some systems of di erence equations, Journal of Computational and Theoretical Nanoscience, 12 (10) (2015), 3697-3704. F. Bozkurt, Stability Analysis of a Nonlinear Di erence Equation, International Journal of Modern Nonlinear Theory and Application, 2 (2013), 1-6. D. Chen, and C. Wang, Boundedness of a Max-type Fourth Order Di erence Equation with Periodic CoefÞcients, Journal of Informatics and Mathematical Sciences, 6 (1) (2014), 1— 21.

7. C. Cinar, On the positive solutions of the di erence equation

+1

=

1

1+

Appl. Math. Comp., 1

158(3) (2004), 809-812. 8. C. Cinar, On the positive solutions of the di erence equation

+1

=

1

1+

Appl. Math. Comp., 1

158(3) (2004), 793-797. 9. Q. Din, Global Stability of Beddington Model, Qualitative Theory of Dynamical Systems, In press (2016), DOI 10.1007/s12346-016-0197-9. 10. E. M. Elabbasy, M. Y. Barsoum, H. S. Alshawee, Behavior of solutions of a class of nonlinear rational di erence equation

+1

=

+

, Electronic Journal of Mathematical Analysis and Applications,

4 (2) (2016), 78-87. 11. E. M. Elabbasy , H. El-Metwally and E. M. Elsayed, Global Behavior of the Solutions of Di erence Equation, Advances in Di erence Equations 2011, 2011: 28. 12. E. M. Elabbasy, A. A. Elsadany, and S. Ibrahim, Qualitative behavior of rational di erence equations of higher order, Malaya J. Mat., 3 (4) (2015), 530— 539. 13. H. El-Metwally and E. M. Elsayed, Qualitative Behavior of some Rational Di erence Equations, Journal of Computational Analysis and Applications, 20 (2) (2016), 226-236. 14. H. El-Metwally and E. M. Elsayed, Form of solutions and periodicity for systems of di erence equations, Journal of Computational Analysis and Applications, 15(5) (2013), 852-857. 15. H. El-Metwally and E. M. Elsayed, Solution and Behavior of a Third Rational Di erence Equation, Utilitas Mathematica, 88 (2012), 27— 42. 16. M. A. El-Moneam, and S. O. Alamoudy, On study of the asymptotic behavior of some rational di erence equations, Dynamics of Continuous, Discrete and Impulsive Systems Series A: Mathematical Analysis, 22 (2015) 157-176. 17. M. M. El-Dessoky, and E. M. Elsayed, On the solutions and periodic nature of some systems of rational di erence equations, Journal of Computational Analysis and Applications, 18 (2) (2015), 206-218. 18. E. M. Elsayed, Solution and attractivity for a rational recursive sequence, Discrete Dynamics in Nature and Society, Volume 2011, Article ID 982309, 17 pages. 19. E. M. Elsayed, Behavior and expression of the solutions of some rational di erence equations, Journal of Computational Analysis and Applications 15 (1) (2013), 73-81. 20. E. M. Elsayed, Solution for systems of di erence equations of rational form of order two, Computational and Applied Mathematics 33 (3) (2014), 751-765. 21. E. M. Elsayed, On the solutions and periodic nature of some systems of di erence equations, International Journal of Biomathematics 7 (6) (2014), 1450067, (26 pages). 22. E. M. Elsayed, Dynamics and Behavior of a Higher Order Rational Di erence Equation, The Journal of Nonlinear Science and Applications, 9 (4) (2016), 1463-1474.

1529

E. M. Elsayed et al 1517-1531

J. COMPUTATIONAL ANALYSIS AND APPLICATIONS, VOL. 24, NO.8, 2018, COPYRIGHT 2018 EUDOXUS PRESS, LLC

23. E. M. Elsayed and A. M. Ahmed, Dynamics of a three-dimensional systems of rational di erence equations, Mathematical Methods in The Applied Sciences, 39 (5) (2016), 1026— 1038. 24. E. M. Elsayed and A. Alghamdi, Dynamics and Global Stability of Higher Order Nonlinear Di erence Equation, Journal of Computational Analysis and Applications, 21 (3) (2016), 493-503. 25. E. M. Elsayed and M. M. El-Dessoky, Dynamics and global behavior for a fourth-order rational di erence equation, Hacettepe Journal of Mathematics and Statistics 42 (5) (2013), 479— 494. 26. E. M. Elsayed, M. M. El-Dessoky and E. O. Alzahrani, The Form of The Solution and Dynamics of a Rational Recursive Sequence, Journal of Computational Analysis and Applications, 17 (1) (2014), 172— 186. 27. E. M. Elsayed, M. M. El-Dessoky and Asim Asiri, Dynamics and Behavior of a Second Order Rational Di erence equation, Journal of Computational Analysis and Applications, 16 (4) (2014), 794— 807. 28. E. M. Elsayed and H. El-Metwally, Stability and solutions for rational recursive sequence of order three, Journal of Computational Analysis and Applications, 17 (2) (2014), 305-315. 29. E. M. Elsayed and H. El-Metwally, Global behavior and periodicity of some di erence equations, Journal of Computational Analysis and Applications, 19 (2) (2015), 298-309. 30. E. M. Elsayed and T. F. Ibrahim, Solutions and periodicity of a rational recursive sequences of order Þve, Bulletin of the Malaysian Mathematical Sciences Society, 38 (1) (2015), 95-112. 31. E. M. Elsayed and T. F. Ibrahim, Periodicity and solutions for some systems of nonlinear rational di erence equations, Hacettepe Journal of Mathematics and Statistics, 44 (6) (2015), 1361— 1390. 32. M. E. Erdogan, and C. Cinar, On the dynamics of the recursive sequence, Fasciculi Mathematici, 50 (2013), 59-66. 33. Sk. Hassan, and E. Chatterjee, Dynamics of the equation in the complex plane , Cogent Mathematics, 2 (2015), 1-12. 34. E. Hatõr, T. Mansour, and Iú. Yalçõnkaya, On a fuzzy di erence equation, Utilitas Mathematica, 93 (2014), 135-151. 35. T. F. Ibrahim, Periodicity and Solution of Rational Recurrence Relation of Order Six, Applied Mathematics, 3 (2012), 729-733. 36. D. Jana and E. M. Elsayed, Interplay between strong Allee e ect, harvesting and hydra e ect of a single population discrete - time system, International Journal of Biomathematics, 9 (1) (2016), 1650004, (25 pages). 37. R. Jothilakshmi, and S. Saraswathy, Periodical Solutions for Extended Kalman Filter’s Stability, International Journal of Science and Application, 1 (1) (2015), 1-11. 38. R. Karatas, C. Cinar and D. Simsek, On positive solutions of the di erence equation 39. 40. 41. 42. 43. 44. 45. 46.

+1

=

5

1+

2

5

Int. J. Contemp. Math. Sci., 1(10) (2006), 495-500. A. Khaliq, and E. M. Elsayed, The Dynamics and Solution of some Di erence Equations, Journal of Nonlinear Sciences and Applications, 9 (3) (2016), 1052-1063. A. Q. Khan, Neimark Sacker bifurcation of a two dimensional discrete time predator prey model, SpringerPlus, (2016) 5:126, DOI 10.1186/s40064-015-1618-y. A. Q. Khan, and M. N. Qureshi, Stability analysis of a discrete biological model, Int. J. Biomath., 9 (2) (2015), 1— 19. H. Khatibzadeh and T. F. Ibrahim, Asymptotic stability and oscillatory behavior of a di erence equation, Electronic Journal of Mathematical Analysis and Applications, 4 (2) (2016), 227-233. M. R. S. Kulenovic and G. Ladas, Dynamics of Second Order Rational Di erence Equations with Open Problems and Conjectures, Chapman & Hall / CRC Press, 2001. M. Mansour, M. M. El-Dessoky and E. M. Elsayed, On the solution of rational systems of di erence equations, Journal of Computational Analysis and Applications, 15 (5) (2013), 967-976. R. Mostafaei and N. Rastegar, On a recurrence relation, QScience Connect, 10 (2014), 1-11. O. Ocalan, H. Ogunmez, and M. Gumus, Global behavior test for a nonlinear di erence equation with a period-two coe cient, Dynamics of Continuous, Discrete and Impulsive Systems Series A: Mathematical Analysis, 21 (2014), 307-316.

1530

E. M. Elsayed et al 1517-1531

J. COMPUTATIONAL ANALYSIS AND APPLICATIONS, VOL. 24, NO.8, 2018, COPYRIGHT 2018 EUDOXUS PRESS, LLC

47. M. Ozair, Q. Din, T. Hussain, and A. Awan, Qualitative behavior of vector-borne disease model, Journal of Nonlinear Sciences and Applications, 9 (2016), 1382— 1395. 48. M. N. Qureshi, and A. Q. Khan, Local stability of an open-access anchovy ishery model, Comp Eco Soft, 5 (1) (2015), 48— 62. 49. D. Simsek, C. Cinar and I. Yalcinkaya, On the recursive sequence

+1

=

3

1+

Int. J. Contemp. Math. 1

Sci., 1 (10) (2006), 475-480. 50. N. Touafek and E. M. Elsayed, On the periodicity of some systems of nonlinear di erence equations, Bull. Math. Soc. Sci. Math. Roumanie, Tome 55 (103) (2) (2012), 217– 224. 51. N. Touafek and E. M. Elsayed, On the solutions of systems of rational di erence equations, Math. Comput. Mod., 55 (2012), 1987– 1997. 52. N. Touafek and Y. Halim, Global Attractivity of a Rational Di erence Equation, Mathematical Sciences Letters, 2 (3) (2013), 161-165. 53. C. Wang, and M. Hu, On the solutions of a rational recursive sequence, Journal of Mathematics and Informatics, 1 (14) (2013), 25-33. 54. W. Wang, and H. Feng, On the dynamics of positive solutions for the di erence equation in a new population model, J. Nonlinear Sci. Appl., 9 (2016), 1748— 1754. 55. I. Yalçõnkaya, C. Cinar and M. Atalay, On the solutions of systems of di erence equations, Advances in Di erence Equations, Vol. 2008, Article ID 143943, 9 pages, doi: 10.1155/2008/ 143943. 56. Y. Yazlik, On the solutions and behavior of rational di erence equations, J. Comp. Anal. Appl., 17 (2014), 584— 594. 57. Y. Yazlik, E. M. Elsayed and N. Taskara, On the Behaviour of the Solutions of Di erence Equation Systems, Journal of Computational Analysis and Applications, 16 (5) (2014), 932— 941. 58. Y. Yazlik, D. Tollu, and N. Taskara, On the Solutions of Di erence Equation Systems with Padovan Numbers, Applied Mathematics, 4 (2013), 15-20. + 59. E. M. E. Zayed, Qualitative behavior of the rational recursive sequence +1 = + + , + International Journal of Advances in Mathematics, 1 (1) (2014), 44-55. 60. Q. Zhang, W. Zhang, J. Liu and Y. Shao, On a Fuzzy Logistic Di erence Equation, WSEAS Transactions on Mathematics, 13 (2014), 282-290. 61. D. Zhang, J. Huang, L. Wang, and W. Ji, Global Behavior of a Nonlinear Di erence Equation with Applications, Open Journal of Discrete Mathematics, 2 (2012), 78-81.

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E. M. Elsayed et al 1517-1531

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