11
Williams, Cogent Mathematics (2016), 3: 1269597 http://dx.doi.org/10.1080/23311835.2016.1269597 PURE MATHEMATICS | RESEARCH ARTICLE On a class of nonlinear max-type difference equations J.L. Williams 1 * Abstract: We investigate the solutions to the following system of nonlinear difference equations, x n+1 = max { y 2 n1 , A y n1 } , y n+1 = max { x 2 n1 , A x n1 } for n N 0 , where x 1 = , y 1 = , x 0 = , and y 0 = are constants and A > 0. Subjects: Mathematics & Statistics; Physical Sciences; Science Keywords: nonlinear system; max-type; periodic solutions; general solution 1. Introduction Many authors have studied the solutions of max-type difference equations (see El-Dessoky, 2015; Elsayed, Iricanin, & Stevic, 2010; Kent, Kustesky, Nguyen, & Nguyen, 2003; Kent & Radin, 2003; Stević, 2010, 2013; Yalçinkaya, Iricanin, & Cinar, 2008). Next are a few papers on systems of max-type difference equations: Stević, Alghamdi, Alotaibi, and Naseer Shahzad (2014) studied the boundedness characteristic of the following max-type difference equations Stević (2012) studied the solutions to the following max-type difference equation x n+1 = max { A, y p n x q n1 } , y n+1 = max { A, x p n y q n1 } for n N 0 . *Corresponding author: J.L. Williams, Texas Southern University, 3100 Cleburne, Houston, TX 77004, USA E-mail: [email protected] Reviewing editor: Hari M. Srivastava, University of Victoria, Canada Additional information is available at the end of the article ABOUT THE AUTHOR J.L. Williams received his PhD in mathematics from Mississippi State University (MSU) August 2013 and his master’s in mathematical sciences from MSU May 2008. In particular, his research area is in partial differential equations (PDE). In PDE, he mainly studies the existence and nonexistence to elliptic equations. He is the first African-American to receive a PhD in Mathematics from MSU. Dr Williams received his bachelor’s degree in mathematics with a minor in Business from the University of Mississippi (Olemiss) in 2006, where he was a member of Pi Mu Epsilon (Honorary math society). Dr Williams is an assistant professor of mathematics at Texas Southern University (TSU), where he started in fall 2013. He has published several papers in professional journals since being at TSU. Also, he received the College of Science, Engineering, & Technology Distinguished Teaching Award and the McCleary Teaching Excellent Award at the university level for teaching. PUBLIC INTEREST STATEMENT Difference equations are pervasive in mathematics and recent advances give insight into other fields such as biology and engineering as well. Understanding the analysis of such equations is crucial in many applications in today’s society. In particular, many equations are discrete in nature and need a solid understanding of the theory of difference equations. We develop conditions for which a system of difference equations will be periodic, oscillatory, or nonperiodic. Also, the general solutions of such systems are given. Received: 25 August 2016 Accepted: 26 November 2016 First Published: 08 December 2016 Page 1 of 11 J.L. Williams © 2017 The Author(s). This open access article is distributed under a Creative Commons Attribution (CC-BY) 4.0 license.

On a class of nonlinear max-type difference equations · Williams, Cogent Mathematics (2016), 3: 1269597 PURE MATHEMATICS | RESEARCH ARTICLE On a class of nonlinear

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Williams, Cogent Mathematics (2016), 3: 1269597http://dx.doi.org/10.1080/23311835.2016.1269597

PURE MATHEMATICS | RESEARCH ARTICLE

On a class of nonlinear max-type difference equationsJ.L. Williams1*

Abstract: We investigate the solutions to the following system of nonlinear difference equations, x

n+1= max

{

y2n−1,

A

yn−1

}

, yn+1

= max{

x2n−1,

A

xn−1

}

for n ∈ N0, where x

−1= �,

y−1

= �, x0= �, and y

0= � are constants and A > 0.

Subjects: Mathematics & Statistics; Physical Sciences; Science

Keywords: nonlinear system; max-type; periodic solutions; general solution

1. IntroductionMany authors have studied the solutions of max-type difference equations (see El-Dessoky, 2015; Elsayed, Iricanin, & Stevic, 2010; Kent, Kustesky, Nguyen, & Nguyen, 2003; Kent & Radin, 2003; Stević, 2010, 2013; Yalçinkaya, Iricanin, & Cinar, 2008).

Next are a few papers on systems of max-type difference equations:

Stević, Alghamdi, Alotaibi, and Naseer Shahzad (2014) studied the boundedness characteristic of the following max-type difference equations

Stević (2012) studied the solutions to the following max-type difference equation

xn+1

= max

{

A,ypn

xq

n−1

}

, yn+1

= max

{

A,xpn

yq

n−1

}

for n ∈ N0.

*Corresponding author: J.L. Williams, Texas Southern University, 3100 Cleburne, Houston, TX 77004, USAE-mail: [email protected]

Reviewing editor:Hari M. Srivastava, University of Victoria, Canada

Additional information is available at the end of the article

ABOUT THE AUTHORJ.L. Williams received his PhD in mathematics from Mississippi State University (MSU) August 2013 and his master’s in mathematical sciences from MSU May 2008. In particular, his research area is in partial differential equations (PDE). In PDE, he mainly studies the existence and nonexistence to elliptic equations. He is the first African-American to receive a PhD in Mathematics from MSU.

Dr Williams received his bachelor’s degree in mathematics with a minor in Business from the University of Mississippi (Olemiss) in 2006, where he was a member of Pi Mu Epsilon (Honorary math society).

Dr Williams is an assistant professor of mathematics at Texas Southern University (TSU), where he started in fall 2013. He has published several papers in professional journals since being at TSU. Also, he received the College of Science, Engineering, & Technology Distinguished Teaching Award and the McCleary Teaching Excellent Award at the university level for teaching.

PUBLIC INTEREST STATEMENTDifference equations are pervasive in mathematics and recent advances give insight into other fields such as biology and engineering as well. Understanding the analysis of such equations is crucial in many applications in today’s society. In particular, many equations are discrete in nature and need a solid understanding of the theory of difference equations. We develop conditions for which a system of difference equations will be periodic, oscillatory, or nonperiodic. Also, the general solutions of such systems are given.

Received: 25 August 2016Accepted: 26 November 2016First Published: 08 December 2016

Page 1 of 11

J.L. Williams

© 2017 The Author(s). This open access article is distributed under a Creative Commons Attribution (CC-BY) 4.0 license.

Page 2 of 11

Williams, Cogent Mathematics (2016), 3: 1269597http://dx.doi.org/10.1080/23311835.2016.1269597

We shall study the solutions to the following system of nonlinear difference equations,

where x−1

= �, y−1

= �, x0= �, and y

0= � are constants and A > 0.

2. Main results

Lemma 2.1 Assume that 0 < 𝛼, 𝛽, 𝜆,𝜇 < A < 1. Then ∀n ∈ N0 the following equalities hold:

Proof Show that

We shall proceed by induction on n. Let n = 0, then (

A

𝛽

)20

=A

𝛽> 1 and A

(

𝛽

A

)1

2

= A1

2 𝛽1

2 < 11

2 11

2 = 1.

Therefore, max{

A

�, A

(

A

)2−1}

=A

�. So the result holds for n = 0. For n = 1,

(

𝛽

A

)21

=𝛽2

A2< 1. Now sup-

pose for some k ∈ N, we have

and

Show that

Observe,

xn+1

= max

{

A

xn

,yn

xn

}

, yn+1

= max

{

A

yn

,xn

yn

}

for n ∈ N0.

(1.1)xn+1

= max

{

y2n−1,A

yn−1

}

, yn+1

= max

{

x2n−1,A

xn−1

}

for n ∈ N0,

max

{

(

A

)22n

, A

(

A

)22n−1}

=

(

A

)22n

max

{

(

A

)22n

, A(

A

)22n−1

}

=

(

A

)22n

max

{

(

A

)22n

, A(

A

)22n−1

}

=

(

A

)22n

max

{

(

A

)22n

, A(

A

)22n−1

}

=

(

A

)22n

.

max

{

(

A

)22n

, A

(

A

)22n−1}

=

(

A

)22n

∀n ∈ N0.

(

A

𝛽

)22k

> 1

(

𝛽

A

)22k−1

< 1.

max

{

(

A

)22k+2

, A

(

A

)22k+1}

=

(

A

)22k+2

.

Page 3 of 11

Williams, Cogent Mathematics (2016), 3: 1269597http://dx.doi.org/10.1080/23311835.2016.1269597

and

Hence,

Therefore, the result is true ∀n ∈ N0. Similarly, the remaining equalities hold. ✷

Theorem 2.1 Assume that 0 < x−1, y

−1, x

0, y

0< A < 1. Also, let

{

xn, yn}

be a solution of the system of Equation (1.1) with x

−1= �, y

−1= �, x

0= �, and y

0= �. Then all solutions of (1.1) are of the following:

Proof For n = 1, we have

So the result holds for n = 1. Now suppose the result is true for some k > 0, that is,

(

A

𝛽

)22k+2

=

(

A

𝛽

)22k⋅22

=

(

A

𝛽

)22k⋅4

=

(

A

𝛽

)22k+2

2k+2

2k+2

2k

=

(

A

𝛽

)22k(

A

𝛽

)22k(

A

𝛽

)22k(

A

𝛽

)22k

> 1 ⋅ 1 ⋅ 1 ⋅ 1 = 1

A

(

𝛽

A

)22k+1

= A

(

𝛽

A

)22k−1

⋅22

= A

(

𝛽

A

)22k−1

(

𝛽

A

)22k−1

(

𝛽

A

)22k−1

(

𝛽

A

)22k−1

< A ⋅ 1 ⋅ 1 ⋅ 1 ⋅ 1 = A < 1.

max

{

(

A

)22k+2

, A

(

A

)22k+1}

=

(

A

)22k+2

.

x4n−3

=

(

A

)22n−2

, y4n−3

=

(

A

)22n−2

x4n−2

=

(

A

)22n−2

, y4n−2

=

(

A

)22n−2

x4n−1

=

(

A

)22n−1

, y4n−1

=

(

A

)22n−1

x4n

=

(

A

)22n−2

, y4n

=

(

A

)22n−2

.

x1= max

{

�2,A

}

=A

�, y

1= max

{

�2,A

}

=A

x2= max

{

�2,A

}

=A

�, y

2= max

{

�2,A

}

=A

x3= max

{

A2

�2, �

}

=A

�, y

3= max

{

A2

�2, �

}

=A

x4= max

{

A2

�2, �

}

=A

�, y

4= max

{

A2

�2, �

}

=A

�.

x4k−3 =

(

A

)22k−2

, y4k−3 =

(

A

)22k−2

x4k−2 =

(

A

)22k−2

, y4k−2 =

(

A

)22k−2

x4k−1 =

(

A

)22k−1

, y4k−1 =

(

A

)22k−1

x4k =

(

A

)22k−2

, y4k =

(

A

)22k−2

.

Page 4 of 11

Williams, Cogent Mathematics (2016), 3: 1269597http://dx.doi.org/10.1080/23311835.2016.1269597

Also, for k + 1 we have the following:

Therefore the result is true for every k ∈ N. This concludes the proof. ✷

Lemma 2.2 Assume that �, �, �,� ≤ −1 and 0 < A < 1. Then ∀n ∈ N0 the following equalities hold:

Proof Show that

We shall proceed by induction on n. Let n = 0, then 𝛽21

= 𝛽2≥ 1 > 0 and A

𝛽20 =

A

𝛽< 0 < 1. Therefore,

max{

�2,

A

}

= �2. So the result holds for n = 0. For n = 1, 1

�22 =

1

�4 ≤ 1. Now suppose for some k ∈ N,

we have

and

Show that

x4k+1 = max

{

y24k−1,

A

y4k−1

}

= max

{

(

A

)22k

, A

(

A

)22k−1}

=

(

A

)22k

y4k+1 = max

{

x24k−1,

A

x4k−1

}

= max

{

(

A

)22k

, A(

A

)22k−1

}

=

(

A

)22k

x4k+2 = max

{

y24k,

A

y4k

}

= max

{

(

A

)22k

, A(

A

)22k−1

}

=

(

A

)22k

y4k+2 = max

{

x24k,

A

x4k

}

= max

{

(

A

)22k

, A(

A

)22k−1

}

=

(

A

)22k

x4k+3 = max

{

y24k+1,

A

y4k+1

}

= max

{

(

A

)22k+1

, A(

A

)22k}

=

(

A

)22k+1

y4k+3 = max

{

x24k+1,

A

x4k+1

}

= max

{

(

A

)22k+1

, A

(

A

)22k}

=

(

A

)22k+1

x4k+4 = max

{

y24k+2,

A

y4k+2

}

= max

{

(

A

)22k+1

, A(

A

)22k}

=

(

A

)22k+1

y4k+4 = max

{

x24k+2,

A

x4k+2

}

= max

{

(

A

)22k+1

, A(

A

)22k}

=

(

A

)22k+1

.

max

{

�22n+1

,A

�22n

}

= �22n+1

max

{

�22n+1

,A

�22n

}

= �22n+1

max

{

�22n+1

,A

�22n

}

= �22n+1

max

{

�22n+1

,A

�22n

}

= �22n+1

.

max

{

�22n+1

,A

�22n

}

= �22n+1

∀n ∈ N0.

�22k+1

≥ 1

1

�22k

≤ 1.

Page 5 of 11

Williams, Cogent Mathematics (2016), 3: 1269597http://dx.doi.org/10.1080/23311835.2016.1269597

Observe,

and

Hence,

Therefore, the result is true ∀n ∈ N0. Similarly, the remaining equalities hold. ✷

Theorem 2.2 Assume that x−1, y

−1, x

0, y

0≤ −1 and 0 < A < 1. Also, let

{

xn, yn}

be a solution of the system of Equations (1.1) with x

−1= �, y

−1= �, x

0= �, and y

0= �. Then all solutions of (1.1) are of the

following:

Proof For n = 1, we have

So the result holds for n = 1. Now suppose the result is true for some k > 0, that is,

Also, for k + 1 we have the following:

max

{

�22k+3

,A

�22k+2

}

= �22k+3

.

�22k+3

= �22k+1

⋅22

= �22k+1

⋅4= �

22k+1

+22k+1

+22k+1

+22k+1

= �22k+1

⋅ �22k+1

⋅ �22k+1

⋅ �22k+1

≥ 1 ⋅ 1 ⋅ 1 ⋅ 1 = 1

A

𝛽22k+2

= A

(

1

𝛽22k⋅22

)

= A

(

1

𝛽22k⋅4

)

= A

(

1

𝛽22k+2

2k+2

2k+2

2k

)

= A

(

1

𝛽22k

)(

1

𝛽22k

)(

1

𝛽22k

)(

1

𝛽22k

)

< A < 1.

max

{

�22k+3

,A

�22k+2

}

= �22k+3

.

x4n−3

= �22n−1

, y4n−3

= �22n−1

x4n−2

= �22n−1

, y4n−2

= �22n−1

x4n−1

= �22n

, y4n−1

= �22n

x4n

= �22n

, y4n

= �22n

.

x1= max

{

�2,A

}

= �2, y

1= max

{

�2,A

}

= �2

x2= max

{

�2,A

}

= �2, y

2= max

{

�2,A

}

= �2

x3= max

{

A

�2, �4

}

= �4, y

3= max

{

A

�2, �4

}

= �4

x4= max

{

A

�4, �

}

= �4, y

4= max

{

A

�4, �

}

= �4.

x4k−3 = �

22k−1

, y4k−3 = �

22k−1

x4k−2 = �

22k−1

, y4k−2 = �

22k−1

x4k−1 = �

22k

, y4k−1 = �

22k

x4k = �

22k

, y4k = �

22n

.

Page 6 of 11

Williams, Cogent Mathematics (2016), 3: 1269597http://dx.doi.org/10.1080/23311835.2016.1269597

Therefore the result is true for every k ∈ N. This concludes the proof. ✷

Theorem 2.3 Let {

xn, yn}

be a solution of the system of Equations (1.1) with x−1

= x0= �, and

y−1

= y0= �. Assume that A2 < 𝜇

3< A and A2 < 𝜆

3< A where 0 < A < 1. Then all solutions of (1.1) are

periodic with period 4 and given by the following:

Proof For n = 1, we have

So the result holds for n = 1. Now suppose the result is true for some k > 0, that is,

Also, for k + 1 we have the following:

x4k+1 = max

{

y24k−1,

A

y4k−1

}

= max

{

�22k+1

,A

�22k

}

= �22k+1

y4k+1 = max

{

x24k−1,

A

x4k−1

}

= max

{

�22k+1

,A

�22k

}

= �22k+1

x4k+2 = max

{

y24k,

A

y4k

}

= max

{

�22k+1

,A

�22k

}

= �22k+1

y4k+2 = max

{

x24k,

A

x4k

}

= max

{

�22k+1

,A

�22k

}

= �22k+1

x4k+3 = max

{

y24k+1,

A

y4k+1

}

= max

{

�22k+2

,A

�22k+1

}

= �22k+2

y4k+3 = max

{

x24k+1,

A

x4k+1

}

= max

{

�22k+2

,A

�22k+1

}

= �22k+2

x4k+4 = max

{

y24k+2,

A

y4k+2

}

= max

{

�22k+2

,A

�22k+1

}

= �22k+2

y4k+4 = max

{

x24k+2,

A

x4k+2

}

= max

{

�22k+2

,A

�22k+1

}

= �22k+2

.

x4n−3

=A

�, y

4n−3=A

x4n−2

=A

�, y

4n−2=A

x4n−1

= �, y4n−1

= �

x4n

= �, y4n

= �.

x1= max

{

�2,A

}

=A

�, y

1= max

{

�2,A

}

=A

x2= max

{

�2,A

}

=A

�, y

2= max

{

�2,A

}

=A

x3= max

{

A2

�2, �

}

= �, y3= max

{

A2

�2, �

}

= �

x4= max

{

A2

�2, �

}

= �, y4= max

{

A2

�2, �

}

= �.

x4k−3 =

A

�, y

4k−3 =A

x4k−2 =

A

�, y

4k−2 =A

x4k−1 = �, y

4k−1 = �

x4k = �, y

4k = �.

Page 7 of 11

Williams, Cogent Mathematics (2016), 3: 1269597http://dx.doi.org/10.1080/23311835.2016.1269597

Therefore the result is true for every k ∈ N. This concludes the proof. ✷

To see the periodic behavior of {

xn, y

n

}

, observe the following three diagrams with x1=

1

4, x

2=

1

4,

y1=

1

3, y

2=

1

3 and A =

1

9:

Lemma 2.3 Assume that −1 ≤ 𝛼, 𝛽, 𝜆,𝜇 < 0 and A ≥ 1. Then ∀n ∈ N0 the following equalities hold:

x4k+1 = max

{

y24k−1,

A

y4k−1

}

= max

{

�2,A

}

=A

y4k+1 = max

{

x24k−1,

A

x4k−1

}

= max

{

�2,A

}

=A

x4k+2 = max

{

y24k,

A

y4k

}

= max

{

�2,A

}

=A

y4k+2 = max

{

x24k,

A

x4k

}

= max

{

�2,A

}

=A

x4k+3 = max

{

y24k+1,

A

y4k+1

}

= max

{

A2

�2, �

}

= �

y4k+3 = max

{

x24k+1,

A

x4k+1

}

= max

{

A2

�2, �

}

= �

x4k+4 = max

{

y24k+2,

A

y4k+2

}

= max

{

A2

�2, �

}

= �

y4k+4 = max

{

x24k+2,

A

x4k+2

}

= max

{

A2

�2, �

}

= �.

max

{

A22n

�22n+1, A

(

�22n

A22n−1

)}

=A2

2n

�22n+1

max

{

A22n

�22n+1, A

(

�22n

A22n−1

)}

=A2

2n

�22n+1

max

{

A22n

�22n+1, A

(

�22n

A22n−1

)}

=A2

2n

�22n+1

max

{

A22n

�22n+1, A

(

�22n

A22n−1

)}

=A2

2n

�22n+1.

Page 8 of 11

Williams, Cogent Mathematics (2016), 3: 1269597http://dx.doi.org/10.1080/23311835.2016.1269597

Proof First, note that �2 ≤ 1 this implies that 1 ≤1

�2. Multiplying by A and using the assumption A ≥ 1

means that A�2 ≥ A ≥ 1. So, for n = 0 we have A

20

�21 =

A

�2 ≥ 1 and A

(

𝛼20

A2−1

)

= A1

2 ⋅ 𝛼 < 0 < 1. Therefore,

max{

A

�2 , A

1

2 ⋅ �

}

=A

�2 . So the result holds for n = 0. Now suppose for some k > 0, we have

and

this means that 𝛼22k

A22k−1 <

1

A≤ 1. Show that

Observe,

and

Hence,

Therefore, the result is true ∀n ∈ N0. Similarly, the remaining equalities hold. ✷

Theorem 2.4 Assume that −1 ≤ x−1, y

−1, x

0, y

0< 0 and A ≥ 1. Also, let

{

xn, yn}

be a solution of the system of Equations (1.1) with x

−1= �, y

−1= �, x

0= �, and y

0= �. Then all solutions of (1.1) are of the following:

For n ∈ N,

A22k

�22k+1

≥ 1

A

(

𝛼22k

A22k−1

)

< 1,

max

{

A22k+2

�22k+3, A

(

�22k+2

A22k+1

)}

=A2

2k+2

�22k+3.

A22k+2

�22k+3

=A2

2k⋅22

�22k+1

⋅22=A2

2k⋅4

�22k+1

⋅4=

A22k+2

2k+2

2k+2

2k+1

�22k+1

+22k+1

+22k+1

+22k+1

=A2

2k

�22k+1

A22k

�22k+1

A22k

�22k+1

A22k

�22k+1

≥ 1

A

(

𝛼22k+2

A22k+1

)

= A

(

𝛼22k+2

2k+2

2k+2

2k

A22k−1

+22k−1

+22k−1

+22k−1

)

= A

(

𝛼22k

A22k−1

)

𝛼22k

A22k−1

𝛼22k

A22k−1

𝛼22k

A22k−1

< 1.

max

{

A22k+2

�22k+3, A

(

�22k+2

A22k+1

)}

=A2

2k+2

�22k+3.

x1= �

2, y1= �

2

x2= �

2, y2= �

2

x4n−1 =

A22n−2

�22n−1

, y4n−1 =

A22n−2

�22n−1

x4n =

A22n−2

�22n−1

, y4n =

A22n−2

�22n−1

x4n+1 =

A22n−1

�22n, y

4n+1 =A2

2n−1

�22n

x4n+2 =

A22n−1

�22n, y

4n+2 =A2

2n−1

�22n.

Page 9 of 11

Williams, Cogent Mathematics (2016), 3: 1269597http://dx.doi.org/10.1080/23311835.2016.1269597

Proof First,

Since, −1 ≤ 𝛼, 𝛽, 𝜆,𝜇 < 0. Next, we shall proceed by induction on n. For n = 1, we have

So the result holds for n = 1. Now suppose the result is true for some k > 0, that is:

Also, for k + 1 we have the following:

Therefore the result is true for every k ∈ N. This concludes the proof. ✷

x1= max

{

�2,A

}

= �2, y

1= max

{

�2,A

}

= �2

x2= max

{

�2,A

}

= �2, y

2= max

{

�2,A

}

= �2.

x3= max

{

�4,A

�2

}

=A

�2, y

3= max

{

�4,A

�2

}

=A

�2

x4= max

{

�4,A

�2

}

=A

�2, y

4= max

{

�4,A

�2

}

=A

�2

x5= max

{

A2

�4, �2

}

=A2

�4, y

5= max

{

A2

�4, �2

}

=A2

�4

x6= max

{

A2

�4, �2

}

=A2

�4, y

6= max

{

A2

�4, �2

}

=A2

�4.

x4k−1 =

A22k−2

�22k−1, y

4k−1 =A2

2k−2

�22k−1

x4k =

A22k−2

�22k−1

, y4k =

A22k−2

�22k−1

x4k+1 =

A22k−1

�22k, y

4k+1 =A2

2k−1

�22k

x4k+2 =

A22k−1

�22k, y

4k+2 =A2

2k−1

�22k.

x4k+3 = max

{

y24k+1,

A

y4k+1

}

= max

{

A22k

�22k+1, A

(

�22k

A22k−1

)}

=A2

2k

�22k+1

y4k+3 = max

{

x24k+1,

A

x4k+1

}

= max

{

A22k

�22k+1, A

(

�22k

A22k−1

)}

=A2

2k

�22k+1

x4k+4 = max

{

y24k+2,

A

y4k+2

}

= max

{

A22k

�22k+1, A

(

�22k

A22k−1

)}

=A2

2k

�22k+1

y4k+4 = max

{

x24k+2,

A

x4k+2

}

= max

{

A22k

�22k+1, A

(

�22k

A22k−1

)}

=A2

2k

�22k+1

x4k+5 = max

{

y24k+3,

A

y4k+3

}

= max

{

A22k+1

�22k+2, A

(

�22k+1

A22k

)}

=A2

2k+1

�22k+2

y4k+5 = max

{

x24k+3,

A

x4k+3

}

= max

{

A22k+1

�22k+2, A

(

�22k+1

A22k

)}

=A2

2k+1

�22k+2

x4k+6 = max

{

y24k+4,

A

y4k+4

}

= max

{

A22k+1

�22k+2, A

(

�22k+1

A22k

)}

=A2

2k+1

�22k+2

y4k+6 = max

{

x24k+4,

A

x4k+4

}

= max

{

A22k+1

�22k+2

, A

(

�22k+1

A22k

)}

=A2

2k+1

�22k+2

.

Page 10 of 11

Williams, Cogent Mathematics (2016), 3: 1269597http://dx.doi.org/10.1080/23311835.2016.1269597

FundingThe author received no direct funding for this research.

Author detailsJ.L. Williams1

E-mail: [email protected] Texas Southern University, 3100 Cleburne, Houston, TX

77004, USA.

Citation informationCite this article as: On a class of nonlinear max-type difference equations, J.L. Williams, Cogent Mathematics (2016), 3: 1269597.

CorrectionThis article was originally published with errors. This version has been amended to remove erroneous text after the first equation on page two of the article.

ReferencesEl-Dessoky, M. M. (2015). On the periodicity of solutions of

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Theorem 2.5 Let {

xn, yn}

be a solution of the system of Equations (1.1) with x−1

= x0= �, and

y−1

= y0= �. Assume that 𝜇3 < A2 < 𝜆

3< A and A5 < 𝜇

6< A4 where 0 < A < 1. Then all solutions of

(1.1) are periodic with period 4 and given by the following:

For n ∈ N,

Proof The result follows by the principle of mathematical induction. ✷

To see the periodic behavior of {

xn, y

n

}

, observe the following three diagrams with x1=

1

2, x

2=

1

2,

y1=

1

3, y

2=

1

3, and A =

1

4:

x1=A

�, y

1=A

x2=A

�, y

2=A

x4n−1 = x4n = �, y

4n−1 = y4n =A2

�2

x4n+1 = x4n+2 =

�2

A, y

4n+1 = y4n+2 =A

�.

Page 11 of 11

Williams, Cogent Mathematics (2016), 3: 1269597http://dx.doi.org/10.1080/23311835.2016.1269597

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Cogent Mathematics (ISSN: 2331-1835) is published by Cogent OA, part of Taylor & Francis Group. Publishing with Cogent OA ensures:• Immediate, universal access to your article on publication• High visibility and discoverability via the Cogent OA website as well as Taylor & Francis Online• Download and citation statistics for your article• Rapid online publication• Input from, and dialog with, expert editors and editorial boards• Retention of full copyright of your article• Guaranteed legacy preservation of your article• Discounts and waivers for authors in developing regionsSubmit your manuscript to a Cogent OA journal at www.CogentOA.com

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Stević, S. (2013). On a symmetric system of max-type difference equations. Applied Mathematics and Computation, 219, 8407–8412.

Stević, S., Alghamdi, M. A., Alotaibi, A., & Shahzad, N. (2014). Boundedness character of a max-type system of

difference equations of second order. Electronic Journal of Qualitative Theory of Differential Equations, 12, 45 pages.

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