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An analysis of exponential kernel fractional difference operator for delta positivity

  • Pshtiwan Othman Mohammed EMAIL logo
Published/Copyright: May 2, 2024
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Abstract

Positivity analysis for a fractional difference operator including an exponential formula in its kernel has been examined. A composition of two fractional difference operators of order (ν,μ) in the sense of Liouville–Caputo type operators has been analysed in cases when νμ and ν=μ . Due to the kernel of the fractional difference operator being convergent, there has been a restriction in the domain of the solution. Incidentally, a negative lower bounded condition has been carried out through analysing the positivity results. For a better understanding, an increasing function has been considered as a test for the main results.

MSC 2010: 26A48; 26A51; 33B10; 39A12; 39B62

1 Introduction

In recent years, discrete fractional calculus has emerged as an important tool to analyse and model real-world phenomena. Fractional difference equations with various types of sums and differences can be used for a wide range of applications in science and engineering, which can be found in previous studies [14]. In particular, to note some of the applications of fractional sum and difference equations with Riemann–Liouville operators, one can refer to applications in logarithmic decay, material mechanics, such as fracture analysis, probability, physics, geology, mechanics, and chemistry [58]. In the meantime, the study of the existence of solutions to boundary value problem for fractional difference equations is one of the most important properties in applications. There are various methods and algorithms used by scholars [913].

The study of the positivity and monotonicity analyses to discrete operator problems for fractional difference equations are two of the most important properties in applications in the context of discrete fractional calculus. The ν -monotonicity concept was first introduced by both mathematicians Atici and Uyanik in [14]. The ν -monotonicity analysis in this article was on the Riemann–Liouville fractional difference operators on the time set Na{a,a+1,} . There are abundant research results regarding positivity and monotonicity analyses for various types of fractional difference operators. However, most of these results have considered the case of Riemann–Liouville fractional difference operators, see, e.g., [1517] and the related references therein. Particularly, ν -monotonicity to analyse Riemann–Liouville fractional difference operators open the door for many new results on positivity and monotonicity analyses for other types of fractional difference operators such as discrete Liouville–Caputo, Attangana–Baleanu and Caputo–Fabrizio operators on Na [1821]. In addition, these results have been extended, and they have been analysed on the time set Nha{a,a+h,a+2h,} [2224]. The extensions and generalisations of positivity and monotonicity analyses using fractional difference operators were presented in previous studies [2530].

By inspiring and motivating the results of the study by Goodrich and Jonnalagadda [31], in the current study, we will work on analysing the discrete Caputo–Fabrizio Δ1cνCFa+1 of another discrete Caputo–Fabrizio Δ1cμCFa in the sense of Liouville–Caputo such that νμ . Specifically, we will analyse these composite operators when the orders are equal ν=μ . In any cases, we use a set of conditions as lower bounds of the inequality. Incidentally, it is worth mentioning that our present work can be considered as an extension of ideas from the study by Goodrich and Jonnalagadda [31] to sequential fractional differences with delta operators. These have been investigated and analysed together with their domain of solutions in Theorems 3.1 and 3.2.

The article’s structure is arranged as follows: In Section 2, the definition of Caputo–Fabrizio fractional difference operator has been recalled and two essential lemmas are given with their proofs. In Section 3, we formulated the domain of solutions and we analysed the proposed model of sequential fractional operators. We discussed an example of an increasing function in Section 4 to validate the main theorems. Finally, concluding remarks and future considerations have been drawn in Section 5.

2 Definition of Caputo–Fabrizio and some lemmas

In the present section, we collect some basic results. Let’s start with the definition of discrete delta Caputo–Fabrizio fractional difference of Liouville–Caputo type of the first order [32]:

(2.1) (Δ1cνCFay)(τ)=B(ν)12ν[τ1s=a(Δsy)(s)(1+λ)τs],

where λ=ν1ν with ν[0,1) . Also, the higher order is defined by [33]:

(2.2) (Δ1cνCFay)(τ)=(Δ1cνqCFaΔqy)(τ)=B(νq)2q+12ν[τ1s=a(Δqsy)(s)(1+λ1)τs],

where λ1=νqq+1ν with ν(q1,q) . Note that (Δy)(τ)=y(τ+1)y(τ) and (Δqy)(τ)=Δ(Δq1y)(τ) for each τNa+1 , and B(ν)>0 .

Lemma 2.1

Let λ1=ν1ν and λ2=μ1μ with 0<ν,μ<12 , and 1ν1ν+μ1μ<32 such that μν . Then, we have

(2.3) P(j)1λ2λ1[λ1(1+λ1)jλ2(1+λ2)j]0,

and

(2.4) Q(j)1λ2λ1[(1+λ2)j(1+λ1)j]>0,

for each jN1 .

Proof

To prove (2.3), we can proceed by induction. For the first step when j=1 , we have

P(1)1λ2λ1[λ1(1+λ1)λ2(1+λ2)]=1λ1λ20,

because ν1ν+μ1μ1 . Let us now assume that

(2.5) P(N)=1λ2λ1[λ1(1+λ1)Nλ2(1+λ2)N]0,

for some NN1 . Then, we have to show that P(N+1)0 . There are two cases to prove it:

Case 1: If ν>μ, we see that 1μ>1νλ2=μ1μ>ν1ν=λ1 . Therefore,

P(N+1)=1λ2λ1[λ1(1+λ1)N+1λ2(1+λ2)N+1]0Iffλ1(1+λ1)N+1λ2(1+λ2)N+10.

Since ν(,0,12) , we can show that 1+λ1=12ν1ν>0 . Therefore, by considering (2.5), we have

λ1(1+λ1)N+1λ2(1+λ2)N(1+λ1)=(1+λ2)N{λ2+λ1λ2}(1+λ2)N{λ2+λ22}[sinceλ2>λ1andλ2<0]λ2(1+λ2)N+1,

which implies that P(N+1)0 for ν>μ .

Case 2: If ν<μ, we have 1ν>1μλ2=μ1μ<ν1ν=λ1 . Therefore,

P(N+1)=1λ2λ1[λ1(1+λ1)N+1λ2(1+λ2)N+1]0Iffλ1(1+λ1)N+1λ2(1+λ2)N+10.

Since μ(,0,12) , we can show that 1+λ2=12μ1μ>0 . Therefore, by considering (2.5), we have

λ2(1+λ2)N+1λ1(1+λ1)N(1+λ2)=(1+λ1)N{λ1+λ1λ2}(1+λ1)N{λ1+λ21}[sinceλ1>λ2andλ1<0]λ1(1+λ1)N+1,

which gives P(N+1)0 for ν<μ . Thus, P(j)0 for all νμ and jN1 . Hence, first part of the lemma is proved.

To prove the second part of the lemma (i.e., (2.4)), we again use two possible cases: The first case when ν>μ, we have λ2>λ1 and 1+λ2>1+λ1 . Therefore, have for each j1:

Q(j)=1λ2λ1[(1+λ2)j(1+λ1)j]>1λ2λ1>0[(1+λ1)j(1+λ1)j]=0=0.

Similarly, we can prove that Q(j)>0 for the case when ν<μ . Thus, the proof of (2.4) is completed. Consequently, the proof of the lemma is done.□

Lemma 2.2

Let λ=ν1ν for ν[,13,12) . Then, we have

(2.6) J(j)(1+λ)j1[λj+(1+λ)]0,

for each jN1 .

Proof

We prove the result by induction: For j=1 , we have

J(1)=2λ+1=13ν1ν0,

since ν[,13,12) and 1ν>0 . Suppose that J(N)0 , that is,

(2.7) (1+λ)N1[λN+(1+λ)]0,

for some NN1 . Then, to show that J(N+1)0 , we use

(1+λ)N[λ(N+1)+(1+λ)]=(1+λ)>0(1+λ)N1[λN(1+λ)]0by claim ()0+λ(1+λ)N<00,

where we have used that λ<0 , and as a result, we obtain J(N+1)0 as required. Consequently, we obtain (2.6) is true for each jN1 . Therefore, we have established the proof.□

Lemma 2.3

For y defined as a function y:NaR , we have

Δ(Δ1cνCFay)(τ)=B(ν)1ν[(Δy)(τ)+λ1+λτ1s=a(Δy)(s)(1+λ)τs],

for ν(,0,12) and τ in Na+1 .

Proof

By taking Δ with respect to τ on both sides of the Eq. (2.1), we have that

Δ(Δ1cνCFay)(τ)=B(ν)12ν[τs=a(Δy)(s)(1+λ)τ+1sτ1s=a(Δy)(s)(1+λ)τs]=B(ν)12ν[(1+λ)(Δy)(τ)+τ1s=a(Δy)(s)(1+λ)τ+1sτ1s=a(Δy)(s)(1+λ)τs].

Rearranging the summations and inside terms to obtain

(2.8) Δ(Δ1cνCFay)(τ)=B(ν)12ν[(1+λ)(Δy)(τ)+τ1s=a(Δy)(s)(1+λ)τs{1+λ1}]=B(ν)1ν[(Δy)(τ)+λ1+λτ1s=a(Δy)(s)(1+λ)τs],

for each τNa+1 , and which completes the proof.□

3 Positivity analyses

This section deals with two important results, which are the main results in this study. The first result for the compositions of two CF operators with two different orders μν with ν,μR , defined on the set D1 , which is

(3.1) D1{(ν,μ);0<ν,μ<12and1ν1ν+μ1μ<32forμν}.

Furthermore, Figure 1 gives further details on the set D1 graphically.

Figure 1 
               Region of the set 
                     
                        
                        
                           
                              
                                 D
                              
                              
                                 1
                              
                           
                        
                        {{\mathscr{D}}}_{1}
                     
                  .
Figure 1

Region of the set D1 .

On the other hand, the second result for the compositions of two CF operators with the same order, defined on the set D2 , which is

(3.2) D2{(ν,μ);0<ν,μ<12and1ν1ν+μ1μ<32forμ=ν}.

Looking at Figure 1, the dashed dot line in the diagonal refers to the set D2 , which is not included from the set D1 .

Remark 3.1

It is important to note that in the delta case, the domain of solutions has been restricted as appeared in (3.1) and (3.2). However, for the nabla case [31] these domains are wider, and they are as follows:

D1{(ν,μ);0<ν,μ<1and1ν+μ<1forμν}

and

D2{(ν,μ);0<ν,μ<1and1ν+μ<2forμ=ν}.

Theorem 3.1

Let ζ0 , λ1=ν1ν , and λ2=μ1μ . If a function y:NaR satisfies

(i)(Δy)(a)0;(ii)(Δ1cνCFa+1Δ1cμCFay)(τ)ζB(ν)B(μ)(12ν)(1μ)(1+λ1)(Δy)(a);(iii)λ2{,(1+λ2)τ1a(1+λ1)τ1aλ2λ1}ζ,

for each (ν,μ)D1 and τNTa+1{a+1,a+2,,T} with some TNa+1 , then, (Δy)(τ1)0 for every τNTa+1 .

Proof

Due to the Eq. (2.1) and Eq. (2.8), we obtain

(3.3) (Δ1cνCFa+1Δ1cμCFay)(τ)=B(ν)12ν[τ1s=a+1(ΔΔ1cμCFay)(s)(1+λ1)τs]=B(ν)12νB(μ)1μ[τ1s=a+1{(Δy)(s)+λ21+λ2s1r=a(Δy)(r)(1+λ2)sr}(1+λ1)τs]=B(ν)B(μ)(12ν)(1μ)[τ1s=a+1(Δy)(s)(1+λ1)τs+λ21+λ2τ1s=a+1s1r=a(Δy)(r)(1+λ2)sr(1+λ1)τs]B(ν)B(μ)(12ν)(1μ)[A1+A2].

We proceed by computing A1 and A2 and we obtain that

(3.4) A1τs=a+1(Δy)(s)(1+λ1)τs=(1+λ1)(Δy)(τ1)+(1+λ1)τ2s=a+1(Δy)(s)(1+λ1)τs1,

and

(3.5) A2λ21+λ2τ1s=a+1s1r=a(Δy)(r)(1+λ2)sr(1+λ1)τs=λ2τ2r=a[(Δy)(r)(1+λ1)τ(1+λ2)rτ1s=r+1(1+λ21+λ1)s]=λ2τ2r=a(Δy)(r)(1+λ1)τ1r1(1+λ21+λ1)τr11+λ21+λ1=λ2τ2r=a(Δy)(r)((1+λ2)τr1(1+λ1)τr1λ2λ1)=λ2(1+λ1)((1+λ2)τ1a(1+λ1)τ1aλ2λ1)(Δy)(a)+λ2(1+λ1)τ2r=a+1(Δy)(r)((1+λ2)τr1(1+λ1)τr1λ2λ1).

This equation is well defined when (ν,μ)D2 . By making use of (3.4)–(3.5) and (ii) in (3.3) with a little simplification, we have

(Δy)(τ1)ζ(Δy)(a)λ2((1+λ2)τ1a(1+λ1)τ1aλ2λ1)(Δy)(a)ζ(Δy)(a)by  (iii)τ2s=a+1(Δy)(s)(1+λ1)τs1λ2τ2r=a+1(Δy)(r)((1+λ2)τr1(1+λ1)τr1λ2λ1)

(3.6) τ2s=a+1(Δy)(s)(1+λ1)τs1λ2τ2r=a+1(Δy)(r)((1+λ2)τr1(1+λ1)τr1λ2λ1)=τ2s=a+1(Δy)(s)(λ1(1+λ1)τs1λ2(1+λ2)τs1λ2λ1).

It is worth mentioning that

λ1(1+λ1)τs1λ2(1+λ2)τs1λ2λ10andλ2{,(1+λ2)τ1a(1+λ1)τ1aλ2λ1}>0,

in view of (2.3) and (2.4), respectively. So, the inequality (3.6) is well defined.

If we use τ=a+2 into (3.6), we obtain

(Δy)(a+1)as=a+1(Δy)(s)(λ1(1+λ1)bs+1λ2(1+λ2)bs+1λ2λ1)=0=0.

Let us try τ=a+3 into (3.6), we see that

(Δy)(a+2)a+1s=a+1(Δy)(s)(λ1(1+λ1)bs+2λ2(1+λ2)bs+2λ2λ1)=(Δy)(a+1)0(λ1(1+λ1)λ2(1+λ2)λ2λ1)0by (2.3)0.

By repeating this action together with the help of (2.3), we attain that (Δy)(τ1)0 for each τNTa+2 . Also, from the assumption (i), we know that (Δy)(a)0 . Consequently, we obtain (Δy)(τ1)0 for each τNTa+1 as desired.□

As we mentioned earlier, our second result is defined on the set D2 and it is not included from the set D1 . Furthermore, we have demonstrated this set in detail in Figure 2.

Figure 2 
               Region of the set 
                     
                        
                        
                           
                              
                                 D
                              
                              
                                 2
                              
                           
                        
                        {{\mathscr{D}}}_{2}
                     
                  .
Figure 2

Region of the set D2 .

Theorem 3.2

Let 13ν<12 , λ=ν1ν , and ζ0 . Assume that the function y defined on Na satisfies

(i)(Δy)(a)0;(ii)(Δ1cνCFa+1Δ1cνCFay)(τ)ζB2(ν)(1ν)(12ν)(Δy)(a);(iii)λ(τ1a)(1+λ)τ2aζ,

for each τNTa+1 with some TNa+1 . Then, (Δy)(τ1)0 for every τNTa+1 .

Proof

By following (2.8) and (2.1), we have

(3.7) (Δ1cνCFa+1Δ1cνCFay)(τ)=B(ν)12ν[τ1s=a+1(ΔΔ1cμCFay)(s)(1+λ)τs]=B(ν)12νB(μ)1ν[τ1s=a+1{(Δy)(s)+λ1+λs1r=a(Δy)(r)(1+λ)sr}(1+λ)τs]=B2(ν)(12ν)(1ν)[τ1s=a+1(Δy)(s)(1+λ)τs+λτ1s=a+1s1r=a(Δy)(r)(1+λ)τr1]B2(ν)(12ν)(1ν)[A3+A4].

Calculating A3 and A4 successfully, we have

(3.8) A3τ1s=a+1(Δy)(s)(1+λ)τs=(1+λ)(Δy)(τ1)+(1+λ)τ2s=a+1(Δy)(s)(1+λ)τs1

and

(3.9) A4λτ1s=a+1s1r=a(Δy)(r)(1+λ)τr1=λτ2r=a[(Δy)(r)(1+λ)τ1rτ1s=r+1(1)]=λτ2r=a(Δy)(r)(1+λ)τ1r(τr1)=λ(τ1a)(1+λ)τ1a(Δy)(a)+τ2r=a+1(Δy)(r)λ(1+λ)τ1r(τr1).

By making use of (3.8)–(3.9) and the assumption (ii) into (3.7) with simplifying the results, we obtain

(3.10) (Δy)(τ1)ζ(Δy)(a)λ(τ1a)(1+λ)τ2a(Δy)(a)ζ(Δy)(a)by (iii)τ2s=a+1(Δy)(s)(1+λ)τs1τ2r=a+1(Δy)(r)λ(1+λ)τ2r(τr1)τ2s=a+1(Δy)(s)(1+λ)τ2s{λ(τs1)+1+λ}.

According to (2.6), we know that

λ(1+λ)τ2r{λ(τs1)+1+λ}0.

Also, we know for each τNa+1 that

λ(τ1a)(1+λ)τ2a=ν1ν>0(τ1a)0(1+λ)τ2a00.

So, these confirm that (3.10) is well defined. Thus, we can continue: by using τ=a+2 into (3.10), we obtain

(Δy)(a+1)λas=a+1()=00.

Use τ=a+3 into (3.10) to obtain

(Δy)(a+2)a+1s=a+1(Δy)(s)(1+λ)a+1s{λ(a+2s)+1+λ}=(Δy)(a+1){2λ+1}0.

We can continue by the same techniques for the next steps with reusing their previous steps and (2.6), and we can deduce that (Δy)(τ)0 for each τNTa+2 . Also, we have (Δy)(a)0 by assumption (i). Thus, (Δy)(τ)0 for each τNTa+1 as required.□

Remark 3.2

The reason why we have two cases for νμ and ν=μ is due to the condition (iii). If we look at the condition (iii) in Theorem 3.1, we see that there are no ν and μ in the inequality. So, we could not conclude a special case when ν=μ . Furthermore, there is no guarantee to have the same condition of Theorems 3.1 in 3.2.

4 Main theorem test

In this section, the results of the proposed Theorems 3.1 and 3.2 are discussed by means of an example. The figures are drawn by using MATLAB R2018b.

Example 4.1

Suppose that y is a function y:N0R defined by

y(τ)=τν+μ̲=Γ(τ+1)Γ(τ+1νμ).

First, for ν=0.40 and μ=0.45 , we see that

1<ν1ν+μ1μ<321<1.4848<32,

which verifies that (ν,μ)D1 .

Now, by choosing ζ=0.001 and τ=a+2 with a=0 , we obtain

(Δ1cνCF1Δ1cμCF0y)(2)=B(ν)B(μ)(12ν)(1μ)[1s=1(Δy)(s)(1+λ1)2s+λ21+λ21s=1s1r=0(Δy)(r)(1+λ2)sr(1+λ1)2s]=0.1418B(ν)B(μ)0.0028B(ν)B(μ).

Similarly, we can deduce that

(Δ1cνCF1Δ1cμCF0y)(τ)0,

for each τN0 , and hence, the second condition of Theorem 3.1 is satisfied. Furthermore, the first condition of Theorem 3.1,

(Δy)(0)=0.91100,

holds. The last condition,

λ2{,(1+λ2)τ1a(1+λ1)τ1aλ2λ1}=0.81820.001,

is satisfied. Hence, τν+μ̲ is increasing on N0 according to Theorem 3.1. Moreover, its plot is shown in Figure 3.

Figure 3 
               Graph of 
                     
                        
                        
                           
                              
                                 τ
                              
                              
                                 
                                    
                                       ν
                                       +
                                       μ
                                    
                                    
                                       ̲
                                    
                                 
                              
                           
                        
                        {\tau }^{\underline{\nu +\mu }}
                     
                   for 
                     
                        
                        
                           ν
                           =
                           0.40
                        
                        \nu =0.40
                     
                   and 
                     
                        
                        
                           μ
                           =
                           0.45
                        
                        \mu =0.45
                     
                  .
Figure 3

Graph of τν+μ̲ for ν=0.40 and μ=0.45 .

Example 4.2

Consider the same function in Example 4.1. Here, if we choose ν=μ=0.4 , ζ=0.001 and τ=a+2 with a=0 , then we have

1<ν1ν+μ1μ<321<1.3333<32,

which verifies that (ν,μ)D2 . Moreover,

(Δy)(0)=0.87130

and

(Δ1cνCF1Δ1cνCF0y)(2)=B2(ν)(12ν)(1μ)[1s=1(Δy)(s)(1+λ)2s+λ1+λ1s=1s1r=0(Δy)(r)(1+λ)sr(1+λ)2s]=0.4034B2(ν)0.0073B2(ν),

and similarly, we can obtain

(Δ1cνCF1Δ1cνCF0y)(τ)0,

for each τN0 . In addition,

λ(τ1a)(1+λ)τ2a=0.0.66670.001.

Thus, all the conditions of Theorem 3.2 are satisfied. Therefore, the increase of τν+μ̲ is proved on N0 . For more clarification, see Figure 4.

Figure 4 
               Graph of 
                     
                        
                        
                           
                              
                                 τ
                              
                              
                                 
                                    
                                       ν
                                       +
                                       μ
                                    
                                    
                                       ̲
                                    
                                 
                              
                           
                        
                        {\tau }^{\underline{\nu +\mu }}
                     
                   for 
                     
                        
                        
                           ν
                           =
                           μ
                           =
                           0.4
                        
                        \nu =\mu =0.4
                     
                  .
Figure 4

Graph of τν+μ̲ for ν=μ=0.4 .

5 Conclusion and future extensions

In this study, we successfully analysed a sequential fractional difference operator (Δ1cνCFa+1Δ1cμCFa) in the sense of Liouville–Caputo type operators for νμ and ν=μ in Theorems 3.1 and 3.2, respectively. In the first theorem, we used the orders to be 0<ν,μ<12 ; however, in the next theorem, we had to use a restriction that 13<ν=μ<12 .

Furthermore, the study investigated the positivity analysis between the sign of the fractional difference operator (Δ1cνCFa+1Δ1cμCFay) and the negative lower boundedness of the function y itself. Based on the example in Section 4, it can be noted that the main theorems are applicable to obtain a monotonicity function.

Our obtained results in this article can be extended to the fractional differences or generalised fractional differences including Mitta-Leffler in their kernels; see studies by Abdeljawad et al. [1,32], for further information about these fractional differences and their main properties.

Acknowledgements

The author is grateful for the reviewer’s valuable comments that improved the manuscript.

  1. Funding information: The author states no funding involved.

  2. Author contributions: The author has accepted responsibility for the entire content of this manuscript and approved its submission.

  3. Conflict of interest: The author states no conflict of interest.

  4. Data availability statement: Data sharing is not applicable to this article as no datasets were generated or analysed during the current study.

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Received: 2023-11-10
Revised: 2024-01-04
Accepted: 2024-01-19
Published Online: 2024-05-02

© 2024 the author(s), published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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