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Research article

Numerical solutions for nonlinear Volterra-Fredholm integral equations of the second kind with a phase lag

  • Correction on: AIMS Mathematics 7: 258-259
  • This study is focused on the numerical solutions of the nonlinear Volterra-Fredholm integral equations (NV-FIEs) of the second kind, which have several applications in physical mathematics and contact problems. Herein, we develop a new technique that combines the modified Adomian decomposition method and the quadrature (trapezoidal and Weddle) rules that used when the definite integral could be extremely difficult, for approximating the solutions of the NV-FIEs of second kind with a phase lag. Foremost, Picard's method and Banach's fixed point theorem are implemented to discuss the existence and uniqueness of the solution. Furthermore, numerical examples are presented to highlight the proposed method's effectiveness, wherein the results are displayed in group of tables and figures to illustrate the applicability of the theoretical results.

    Citation: Gamal A. Mosa, Mohamed A. Abdou, Ahmed S. Rahby. Numerical solutions for nonlinear Volterra-Fredholm integral equations of the second kind with a phase lag[J]. AIMS Mathematics, 2021, 6(8): 8525-8543. doi: 10.3934/math.2021495

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  • This study is focused on the numerical solutions of the nonlinear Volterra-Fredholm integral equations (NV-FIEs) of the second kind, which have several applications in physical mathematics and contact problems. Herein, we develop a new technique that combines the modified Adomian decomposition method and the quadrature (trapezoidal and Weddle) rules that used when the definite integral could be extremely difficult, for approximating the solutions of the NV-FIEs of second kind with a phase lag. Foremost, Picard's method and Banach's fixed point theorem are implemented to discuss the existence and uniqueness of the solution. Furthermore, numerical examples are presented to highlight the proposed method's effectiveness, wherein the results are displayed in group of tables and figures to illustrate the applicability of the theoretical results.



    Fractional difference calculus is a tool used to explain many phenomena in physics, control problems, modeling, chaotic dynamical systems, and various fields of engineering and applied mathematics. In this direction, different kinds of methods and techniques, including numerical and analytical methods, have been utilized by researchers to discuss given fractional discrete and continuous mathematical models and boundary value problems (BVPs) [1,2,3,4]. For some recent developments on the existence, uniqueness, and stability of solutions for fractional differential equations, see, for example, [5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23] and the references therein.

    Discrete fractional calculus and difference equations open a new study context for mathematicians. For this reason, they have received increasing attention in recent years. Some real-world processes and phenomena are analyzed with the aid of discrete fractional operators, since such operators provide an accurate tool to describe memory. A large number of research articles dealing with difference equations and discrete fractional boundary value problems (FBVPs) can be found in [24,25,26,27,28,29,30,31,32].

    In 2020, Selvam et al. [33] proved the existence of a solution to a discrete fractional difference equation formulated as

    {cΔϱξχ(ξ)=Φ(ξ+ϱ1,χ(ξ+ϱ1)),1<ϱ2,Δχ(ϱ2)=M1,χ(ϱ+T)=M2, (1.1)

    for ξ[0,T]N0=[0,1,2,,T], TN, η[ϱ1,T+ϱ1]Nϱ1, M1 and M2 constants, Φ:[ϱ2,ϱ+T]Nϱ2×RR continuous, and where cΔϱξ denotes the ϱth-Caputo difference. Here, motivated by the discrete model (1.1), we shall consider two generalized discrete problems.

    Our first goal consists to study existence and uniqueness of solutions to the following discrete fractional equation that involves Caputo discrete derivatives:

    {cΔϱξχ(ξ)=Φ(ξ+ϱ1,χ(ξ+ϱ1)),2<ϱ3,Δχ(ϱ3)=A1,χ(ϱ+T)=λΔβχ(η+β),Δ2χ(ϱ3)=A2, (1.2)

    for 0<β1, ξ[0,T]N0=[0,1,2,,T], TN, η[ϱ1,T+ϱ1]Nϱ1, λ, A1 and A2 constants, and where Φ:[ϱ3,ϱ+T]Nϱ3×RR is continuous.

    The second goal is to study the stability of solutions to the discrete Riemann-Liouville fractional problem

    {RLΔϱξχ(ξ)=Φ(ξ+ϱ1,χ(ξ+ϱ1)),2<ϱ3,Δχ(ϱ3)=A1,χ(ϱ+T)=λΔβχ(η+β),Δ2χ(ϱ3)=A2, (1.3)

    for 0<β1, ξ[0,T]N0=[0,1,2,,T] and η[ϱ1,T+ϱ1]Nϱ1, where RLΔϱξ is the Riemann-Liouville difference operator.

    The organization of the paper is as follows. In Section 2, we collect some fundamental definitions available from the literature. In Section 3, we prove the existence and uniqueness results for the discrete FBVP (1.2). Hyers-Ulam and Hyers-Ulam-Rassias stability of the solution for the FBVP (1.3) is established in Section 4. In Section 5, two examples are given to illustrate the obtained results. We end with Section 6 of conclusions.

    We begin by recalling some necessary definitions and essential lemmas that will be used throughout the paper.

    Definition 2.1. (See [27]) Let ϱ>0. The ϱ-order fractional sum of Φ is defined by

    ΔϱξΦ(ξ)=1Γ(ϱ)ξϱl=a(ξl1)(ϱ1)Φ(l), (2.1)

    where ξNa+ϱ:={a+ϱ,a+ϱ+1,} and ξ(ϱ):=Γ(ξ+1)Γ(ξ+1ϱ).

    Definition 2.2. (See [27]) Let ϱ>0 and Φ be defined on Na. The ϱ-order Caputo fractional difference of Φ is defined by

    CaΔϱξΦ(ξ)=Δ(nϱ)(ΔnΦ(ξ))=1Γ(nϱ)ξ(nϱ)l=a(ξl1)(nϱ1)ΔnΦ(l), (2.2)

    while the Riemann-Liouville fractional difference of Φ is defined by

    RLaΔϱξΦ(ξ)=ΔnΔ(nϱ)Φ(ξ), (2.3)

    where ξNa+nϱ and n1<ϱn.

    Lemma 2.1. (See [24,27]) For ϱ>0,

    ΔϱCaΔϱξΦ(ξ)=Φ(ξ)+C0+C1ξ++CN1ξ(N1), (2.4)

    where CiR, i=1,2,,N1, Φ is defined on Na, and 0N1<ϱN.

    Lemma 2.2. (See ([32]) Let 0N1<ϱN and Φ be defined on Na. Then,

    ΔϱRL0ΔϱξΦ(ξ)=Φ(ξ)+B1ξϱ1+B2ξ(ϱ2)++BNξ(ϱN), (2.5)

    for B1,,BNR.

    Lemma 2.3. (See [31]) Let ϱ and ξ be any arbitrary real numbers. Then,

    (1)ξϱl=0(ξl1)(ϱ1)=Γ(ξ+1)ϱΓ(ξϱ+1),(2)Ll=0(ξLl1)(ϱ1)=Γ(ϱ+L+1)ϱΓ(L+1).

    Lemma 2.4. (See [31]) For ζR(Z{0}), we have

    Δϱξ(ζ)=Γ(ζ+1)Γ(ζ+ϱ+1)ξ(ζ+ϱ).

    In this section, we prove the existence and uniqueness of solution for the Caputo three-point discrete fractional problem (1.2). To accomplish this, we denote by C(Nϱ3,ϱ+T,R) the collection of all continuous functions χ with the norm

    χ=max{|χ(ξ)|:ξNϱ3,ϱ+T}.

    Lemma 3.1. Let 2<ϱ3 and Φ:[ϱ3,ϱ+T]Nϱ3R. A function χ(ξ) (ξ[ϱ3,ϱ+T]Nϱ3) that satisfies the discrete FBVP

    {cΔϱξχ(ξ)=Φ(ξ+ϱ1),2<ϱ3,Δχ(ϱ3)=A1,χ(ϱ+T)=λΔβχ(η+β),Δ2χ(ϱ3)=A2,0<β1, (3.1)

    is given by

    χ(ξ)=1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1)λK1Γ(ϱ)ηl=ϱlϱξ=0(η+βρ(l))(β1)(lρ(ξ))(ϱ1)Φ(ξ+ϱ1)+Γ(β)K1Γ(ϱ)Tl=0(ϱ+Tρ(l))(ϱ1)Φ(l+ϱ1)+K2+[A1A2(ϱ3)]ξ(1)+A22ξ(2), (3.2)

    with

    K1=ληl=ϱ3(η+βρ(l))(β1)Γ(β), (3.3)

    and

    K2=λK1[A2(ϱ3)A1]ηl=ϱ3(η+βρ(l))(β1)l(1)A22K1ληl=ϱ3(η+βρ(l))(β1)l(2)+Γ(β)K1(ϱ+T)[A1A2(ϱ3)+A22(ϱ+T1)]. (3.4)

    Proof. Let χ(ξ) be a solution to (3.1). Applying Lemma 2.1 and Definition 2.1, we find that

    χ(ξ)=1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1)+C0+C1ξ(1)+C2ξ(2), (3.5)

    for ξ[ϱ3,ϱ+T]Nϱ3, where C0,C1,C2R. By using the difference of order 1 for (3.5), we have

    Δχ(ξ)=1Γ(ϱ1)ξϱ+1l=0(ξρ(l))(ϱ2)Φ(l+ϱ1)+C1+2C2ξ(1),

    and

    Δ2χ(ξ)=1Γ(ϱ2)ξϱ+2l=0(ξρ(l))(ϱ3)Φ(l+ϱ1)+2C2.

    Now, from conditions Δχ(ϱ3)=A1 and Δ2χ(ϱ3)=A2, we obtain that

    C1=A1A2(ϱ3),C2=A22.

    Therefore,

    χ(ξ)=1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1)+C0+[A1A2(ϱ3)]ξ(1)+A22ξ(2), (3.6)

    for ξ[ϱ3,ϱ+T]Nϱ3. By using formula (3.5), one has

    Δβχ(ξ)=C1Γ(β)ξβl=ϱ3(ξρ(l))(β1)l(1)+C2Γ(β)ξβl=ϱ3(ξρ(l))(β1)l(2)+C0Γ(β)ξβl=ϱ3(ξρ(l))(β1)+1Γ(ϱ)Γ(β)ξβl=ϱlϱξ=0(ξρ(l))(β1)(lρ(ξ))(ϱ1)Φ(ξ+ϱ1). (3.7)

    The other condition of (3.1) gives

    λΔβχ(η+β)=λ[A1A2(ϱ3)]Γ(β)ηl=ϱ3(η+βρ(l))(β1)l(1) +λA22Γ(β)ηl=ϱ3(η+βρ(l))(β1)l(2)+λC0Γ(β)ηl=ϱ3(η+βρ(l))(β1) +λΓ(ϱ)Γ(β)ηl=ϱlϱξ=0(η+βρ(l))(β1)(lρ(ξ))(ϱ1)Φ(ξ+ϱ1)=1Γ(ϱ)Tl=0(ϱ+Tρ(l))(ϱ1)Φ(l+ϱ1)+C0 +[A1A2(ϱ3)](ϱ+T)(1)+A22(ϱ+T)(2).

    We have

    C0=Γ(β)K1Γ(ϱ)Tl=0(ϱ+Tρ(l))(ϱ1)Φ(l+ϱ1)+K2λK1Γ(ϱ)ηl=ϱlϱξ=0(η+βρ(l))(β1)(lρ(ξ))(ϱ1)Φ(ξ+ϱ1),

    where K1 and K2 are defined by (3.3) and (3.4), and one obtains (3.2) by substituting the value of C0 into (3.6).

    Now, let us consider the operator H:C(Nϱ3,ϱ+T,R)C(Nϱ3,ϱ+T,R) defined by

    (Hχ)(ξ)=1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1,χ(l+ϱ1))λK1Γ(ϱ)ηl=ϱlϱτ=0(η+βρ(l))(β1)(lρ(τ))(ϱ1)Φ(l+ϱ1,χ(l+ϱ1))+Γ(β)K1Γ(ϱ)Tl=0(ϱ+Tρ(l))(ϱ1)Φ(l+ϱ1,χ(l+ϱ1))+K2+[A1A2(ϱ3)]ξ(1)+A22ξ(2).

    Theorem 3.1. Assume that:

    (H1) Function Φ satisfies |Φ(ξ,χ1)Φ(ξ,χ2)|K|χ1χ2|, where K>0, ξNϱ3,ϱ+T and χ1,χ2C(Nϱ3,ϱ+T,R). The discrete FBVP (3.1) has a unique solution on C(Nϱ3,ϱ+T,R) provided

    Γ(ϱ+T+1)Γ(ϱ+1)Γ(T+1)(1+Γ(β)K1)+MλK1Γ(ϱ)1K (3.8)

    with

    M=|ηl=ϱlϱτ=0(η+βρ(l))(β1)(lρ(τ))(ϱ1)|. (3.9)

    Proof. Let χ1,χ2C(Nϱ3,ϱ+T,R). Then, for each ξNϱ3,ϱ+T, we have

    |(Hχ1)(ξ)(Hχ2)(ξ)|1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)×|Φ(l+ϱ1,χ1(l+ϱ1))Φ(l+ϱ1,χ2(l+ϱ1))|+λK1Γ(ϱ)ηl=ϱlϱτ=0(η+βρ(l))(β1)(lρ(τ))(ϱ1)×|Φ(l+ϱ1,χ1(l+ϱ1))Φ(l+ϱ1,χ2(l+ϱ1))|+Γ(β)K1Γ(ϱ)Tl=0(ϱ+Tρ(l))(ϱ1)×|Φ(l+ϱ1,χ1(l+ϱ1))Φ(l+ϱ1,χ2(l+ϱ1))|.

    It follows that

    (Hχ1)(ξ)(Hχ2)(ξ)Kχ1χ2Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)+λKχ1χ2K1Γ(ϱ)ηl=ϱlϱτ=0(η+βρ(l))(β1)(lρ(τ))(ϱ1)+Γ(β)Kχ1χ2K1Γ(ϱ)Tl=0(ϱ+Tρ(l))(ϱ1)Kχ1χ2Γ(ϱ)Γ(ϱ+T+1)ϱΓ(T+1)+λKχ1χ2K1Γ(ϱ)ηl=ϱlϱτ=0(η+βρ(l))(β1)(lρ(τ))(ϱ1)+Γ(β)Kχ1χ2K1Γ(ϱ)Γ(ϱ+T+1)ϱΓ(T+1)Kχ1χ2[Γ(ϱ+T+1)Γ(ϱ+1)Γ(T+1)+MλK1Γ(ϱ)+Γ(β)Γ(ϱ+T+1)K1Γ(ϱ+1)Γ(T+1)].

    From (3.8), we conclude that H is a contraction. Then, by the Banach contraction principle, the discrete problem (3.1) has a unique solution on C(Nϱ3,ϱ+T,R).

    Theorem 3.2. Suppose that Φ:[ϱ3,ϱ+T]Nϱ3×RR is a continuous function and

    R=max{|Φ(l+ϱ1,χ(l+ϱ1))|,ξNϱ3,ϱ+T,χC(Nϱ3,ϱ+T,R);χ2|K2|}.

    The discrete problem (3.1) has a solution provided that

    R|K2||[A1A2(ϱ3)]|(ϱ+T)(1)|A22|(ϱ+T)(2)Γ(ϱ+T+1)Γ(ϱ+1)Γ(T+1)(1+Γ(β)|K1|)+M|λ|Γ(ϱ)|K1|. (3.10)

    Proof. Let G={χC(Nϱ3,ϱ+T,R);χ2|K2|}. For χ(ξ)G, we get

    |(Hχ)(ξ)|=|1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1,χ(l+ϱ1))+λK1Γ(ϱ)ηl=ϱlϱτ=0(η+βρ(l))(β1)(lρ(τ))(ϱ1)Φ(l+ϱ1,χ(l+ϱ1))Γ(β)K1Γ(ϱ)Tl=0(ϱ+Tρ(l))(ϱ1)Φ(l+ϱ1,χ(l+ϱ1))+K2+[A1A2(ϱ3)]ξ(1)+A22ξ(2)|1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)|Φ(l+ϱ1,χ(l+ϱ1))|+|λ||K1|Γ(ϱ)ηl=ϱlϱτ=0(η+βρ(l))(β1)(lρ(τ))(ϱ1)|Φ(l+ϱ1,χ(l+ϱ1))|+Γ(β)|K1|Γ(ϱ)Tl=0(ϱ+Tρ(l))(ϱ1)|Φ(l+ϱ1,χ(l+ϱ1))|+|K2|+|[A1A2(ϱ3)]ξ(1)|+|A22ξ(2)|RΓ(ϱ)[ξϱl=0(ξρ(l))(ϱ1)+|λ||K1|ηl=ϱlϱτ=0(η+βρ(l))(β1)(lρ(τ))(ϱ1)+Γ(β)|K1|Tl=0(ϱ+Tρ(l))(ϱ1)]+|K2|+|[A1A2(ϱ3)]|(ϱ+T)(1)+|A22|(ϱ+T)(2)RΓ(ϱ)[Γ(ϱ+T+1)ϱΓ(T+1)(1+Γ(β)|K1|)+M|λ||K1|]+|K2|+|[A1A2(ϱ3)]|(ϱ+T)(1)+|A22|(ϱ+T)(2).

    From (3.10), we have Hχ2|K2|, which implies that H:GG. By Brouwer's fixed point theorem, we know that the discrete problem (3.1) has a solution.

    In this section, we study the Hyers-Ulam and Hyers-Ulam-Rassias stability for the solutions of the discrete Riemann-Liouville (RL) FBVP

    {RLΔϱξχ(ξ)=Φ(ξ+ϱ1,χ(ξ+ϱ1)),2<ϱ3,Δχ(ϱ3)=A1,χ(ϱ+T)=λΔβχ(η+β),Δ2χ(ϱ3)=A2,0<β1, (4.1)

    for ξ[0,1,2,,T]=[0,T]N0 and η[ϱ1,T+ϱ1]Nϱ1, where RLΔϱξ is the RL fractional difference operator. We begin by proving the following lemma.

    Lemma 4.1. Suppose that 2<ϱ3 and Φ:[ϱ3,ϱ+T]Nϱ3R. A function χ satisfies the discrete problem

    {RLΔϱξχ(ξ)=Φ(ξ+ϱ1),2<ϱ3,Δχ(ϱ3)=A1,χ(ϱ+T)=λΔβχ(η+β),Δ2χ(ϱ3)=A2,0<β1, (4.2)

    if, and only if, χ(ξ), ξ[ϱ3,ϱ+T]Nϱ3, has the form

    χ(ξ)=1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1)+{[A2A1(ϱ3)]Γ(ϱ)+fΦ+dϱhϱ(ϱ3)2(ϱ1)}ξ(ϱ1)+[A11hϱ[fΦ+dϱ](ϱ3)Γ(ϱ2)]Γ(ϱ1)ξ(ϱ2)+fΦ+dϱhϱξ(ϱ3), (4.3)

    where

    hϱ=ϱ3ϱ2(ϱ+T)(ϱ2)ϱ32(ϱ1)(ϱ+T)(ϱ1)(ϱ+T)(ϱ3) (4.4)
    +λ(ϱ3)Γ(β)2(ϱ1)ηl=ϱ3(η+βρ(l))(β1)l(ϱ1)λ(ϱ3)Γ(β)(ϱ2)ηl=ϱ3(η+βρ(l))(β1)l(ϱ2)+λΓ(β)ηl=ϱ3(η+βρ(l))(β1)l(ϱ3),dϱ=A1(ϱ+T)(ϱ2)Γ(ϱ1)[A2A1(ϱ3)]λΓ(ϱ)Γ(β)ηl=ϱ3(η+βρ(l))(β1)l(ϱ1) (4.5)
    A1λΓ(ϱ1)Γ(β)ηl=ϱ3(η+βρ(l))(β1)l(ϱ2)+[A2A1(ϱ3)]Γ(ϱ)(ϱ+T)(ϱ1),fΦ=λΓ(ϱ)Γ(β)ηl=ϱlϱτ=0(η+βρ(l))(β1)(lρ(τ))(ϱ1)Φ(τ+ϱ1) (4.6)
    +1Γ(ϱ)Tl=0(ϱ+Tρ(l))(ϱ1)Φ(l+ϱ1).

    Proof. Let χ(ξ) be a solution to (4.2). Applying Lemma 2.2 and Definition 2.1, we obtain that the general solution of (4.2) is given by

    χ(ξ)=1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1)+B1ξ(ϱ1)+B2ξ(ϱ2)+B3ξ(ϱ3), (4.7)

    ξ[ϱ3,ϱ+T]Nϱ3, where B1,B2,B3R. The first order difference of (4.7) is

    Δχ(ξ)=1Γ(ϱ1)ξϱ+1l=0(ξρ(l))(ϱ2)Φ(l+ϱ1)+B1(ϱ1)ξ(ϱ2)+B2(ϱ2)ξ(ϱ3)+B3(ϱ3)ξ(ϱ4),

    while

    Δ2χ(ξ)=1Γ(ϱ2)ξϱ+2l=0(ξρ(l))(ϱ3)Φ(l+ϱ1)+B1(ϱ1)(ϱ2)ξ(ϱ3)+B2(ϱ2)(ϱ3)ξ(ϱ4)+B3(ϱ3)(ϱ4)ξ(ϱ5).

    From the conditions Δχ(ϱ3)=A1 and Δ2χ(ϱ3)=A2, we obtain that

    B2=1Γ(ϱ1)[A1B3(ϱ3)Γ(ϱ2)],

    and

    B1=1Γ(ϱ)[A2A1(ϱ3)]+B3(ϱ3)2(ϱ1).

    Now, by using the difference of order β for (4.7), it follows that

    Δβχ(ξ)=1Γ(β){1Γ(ϱ)[A2A1(ϱ3)]+B3(ϱ3)2(ϱ1)}ξβl=ϱ3(ξρ(l))(β1)l(ϱ1)+B3Γ(β)ξβl=ϱ3(ξρ(l))(β1)l(ϱ3)+[A1B3(ϱ3)Γ(ϱ2)]Γ(ϱ1)Γ(β)ξβl=ϱ3(ξρ(l))(β1)l(ϱ2)+1Γ(ϱ)Γ(β)ξβl=ϱlϱτ=0(ξρ(l))(β1)(lρ(τ))(ϱ1)Φ(τ+ϱ1). (4.8)

    Based on condition (4.1), we have

    λΔβχ(η+β)=λΓ(β){1Γ(ϱ)[A2A1(ϱ3)]+B3(ϱ3)2(ϱ1)}ηl=ϱ3(η+βρ(l))(β1)l(ϱ1)+λΓ(ϱ1)Γ(β)[A1B3(ϱ3)Γ(ϱ2)]ηl=ϱ3(η+βρ(l))(β1)l(ϱ2)+B3λΓ(β)ηl=ϱ3(η+βρ(l))(β1)l(ϱ3)+λΓ(ϱ)Γ(β)ηl=ϱlϱτ=0(η+βρ(l))(β1)(lρ(τ))(ϱ1)Φ(τ+ϱ1)=1Γ(ϱ)Tl=0(ϱ+Tρ(l))(ϱ1)Φ(l+ϱ1)+1Γ(ϱ1)[A1B3(ϱ3)Γ(ϱ2)](ϱ+T)(ϱ2)+{1Γ(ϱ)[A2A1(ϱ3)]+B3(ϱ3)2(ϱ1)}(ϱ+T)(ϱ1)+B3(ϱ+T)(ϱ3).

    Then,

    B3=1hϱ[fΦ+dϱ],B2=1Γ(ϱ1)[A11hϱ[fΦ+dϱ](ϱ3)Γ(ϱ2)],B1=1Γ(ϱ)[A2A1(ϱ3)]+1hϱ[fΦ+dϱ](ϱ3)2(ϱ1),

    where hϱ, dϱ and fΦ are defined by (4.4)-(4.6), respectively. Substituting the values of the constants B1, B2 and B3 into (4.7), we obtain (4.3) and our proof is complete.

    From Lemma 4.1, the solution of the discrete RL problem (4.1) is given by the formula

    χ(ξ)=1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1,χ(l+ϱ1))+{[A2A1(ϱ3)]Γ(ϱ)+fχ+dϱhϱ(ϱ3)2(ϱ1)}ξ(ϱ1)+[A11hϱ[fΦ+dϱ](ϱ3)Γ(ϱ2)]Γ(ϱ1)ξ(ϱ2)+fχ+dϱhϱξ(ϱ3), (4.9)

    where dρ and hρ are defined by (4.4) and (4.5), respectively, and

    fχ=λΓ(ϱ)Γ(β)ηl=ϱlϱτ=0(η+βρ(l))(β1)(lρ(τ))(ϱ1)Φ(τ+ϱ1,χ(τ+ϱ1))+1Γ(ϱ)Tl=0(ϱ+Tρ(l))(ϱ1)Φ(l+ϱ1,χ(l+ϱ1)). (4.10)

    Lemma 4.2. If χ is a solution of (4.3), then

    χ(ξ)=1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1)+Q(ξ)+fχK(ξ), (4.11)

    where

    Q(ξ)={[A2A1(ϱ3)]Γ(ϱ)+dϱ(ϱ3)2hϱ(ϱ1)}ξ(ϱ1)+[A1dϱhϱ(ϱ3)Γ(ϱ2)]Γ(ϱ1)ξ(ϱ2)+dϱhϱξ(ϱ3),

    and

    K(ξ)=(ϱ3)2hϱ(ϱ1)ξ(ϱ1)(ϱ3)hϱ(ϱ2)ξ(ϱ2)+ξ(ϱ3)hϱ.

    Proof. Take χ as a solution of (4.2). For ξ[ϱ3,ϱ+T]Nϱ3, then

    χ(ξ)=1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1)+{[A2A1(ϱ3)]Γ(ϱ)+fχ+dϱhϱ(ϱ3)2(ϱ1)}ξ(ϱ1)+[A11hϱ[fχ+dϱ](ϱ3)Γ(ϱ2)]Γ(ϱ1)ξ(ϱ2)+fχ+dϱhϱξ(ϱ3)=1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1)+{[A2A1(ϱ3)]Γ(ϱ)+dϱ(ϱ3)2hϱ(ϱ1)}ξ(ϱ1)+[A1dϱhϱ(ϱ3)Γ(ϱ2)]Γ(ϱ1)ξ(ϱ2)+dϱhϱξ(ϱ3)+fχ[(ϱ3)2hϱ(ϱ1)ξ(ϱ1)(ϱ3)hϱ(ϱ2)ξ(ϱ2)+ξ(ϱ1)hϱ]=1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1)+Q(ξ)+fχK(ξ).

    The proof is complete.

    Definition 4.1. We say that the discrete RL problem (4.1) is Hyers-Ulam stable if for each function νC(Nϱ3,ϱ+T,R) of

    |RLΔϱξν(ξ)Φ(ξ+ϱ1,ν(ξ+ϱ1))|ϵ,ξ[0,T]N0, (4.12)

    and ϵ>0, there exists χC(Nϱ3,ϱ+T,R) solution of (4.1) and δ>0 such that

    |ν(ξ)χ(ξ)|δϵ,ξ[ϱ3,ϱ+T]Nϱ3. (4.13)

    Definition 4.2. We say that the discrete RL problem (4.1) is Hyers-Ulam–Rassias stable if for each function νC(Nϱ3,ϱ+T,R) of

    |RLΔϱξν(ξ)Φ(ξ+ϱ1,ν(ξ+ϱ1))|ϵθ(ξ+ϱ1),ξ[0,T]N0, (4.14)

    and ϵ>0, there exists χC(Nϱ3,ϱ+T,R) solution of (4.1) and δ2>0 such that

    |ν(ξ)χ(ξ)|δ2ϵθ(ξ+ϱ1),ξ[ϱ3,ϱ+T]Nϱ3. (4.15)

    Remark 4.1. A function χ(ξ)C(Nϱ3,ϱ+T,R) is a solution of (4.12) if, and only if, there exists μ:[ϱ3,ϱ+T]Nϱ3R satisfying:

    (H2) |μ(ξ+ϱ1)|ϵ,ξ[0,T]N0;

    (H3) RLΔϱξν(ξ)=Φ(ξ+ϱ1,ν(ξ+ϱ1))+μ(ξ+ϱ1),ξ[0,T]N0.

    Remark 4.2. A function χ(ξ)C(Nϱ3,ϱ+T,R) is a solution of (4.14) if, and only if, there exists μ:[ϱ3,ϱ+T]Nϱ3R satisfying

    (H4) |μ(ξ+ϱ1)|ϵθ(ξ+ϱ1),ξ[0,T]N0,

    (H5) RLΔϱξν(ξ)=Φ(ξ+ϱ1,ν(ξ+ϱ1))+μ(ξ+ϱ1),ξ[0,T]N0.

    Lemma 4.3. If ν satisfies (4.12), then

    |ν(ξ)1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1,ν(l+ϱ1))Q(ξ)fνK(ξ)|ϵΓ(ϱ+T+1)Γ(ϱ+1)Γ(T+1).

    Proof. Using our hypothesis, and based on Remark 4.1, the solution to (H3) satisfies

    ν(ξ)=1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1,ν(l+ϱ1))+Q(ξ)+fνK(ξ)+1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)μ(l+ϱ1).

    Hence,

    |ν(ξ)1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1,ν(l+ϱ1))Q(ξ)fνK(ξ)|=|1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)μ(l+ϱ1)|1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)|μ(l+ϱ1)|ϵΓ(ϱ+T+1)Γ(ϱ+1)Γ(T+1),

    and the desired inequality is derived.

    Theorem 4.1. If condition (H1) holds and (4.13) is satisfied, then the discrete RL problem (4.1) is Hyers-Ulam stable under the condition

    KΓ(β)Γ(T+1)Γ(ϱ+1)2M1Γ(ϱ+T+1)Γ(β)+MM1λϱΓ(T+1), (4.16)

    where M1=max(1,|K(ξ)|).

    Proof. Let ξ[ϱ3,ϱ+T]Nϱ3. From Lemma 8, we have

    |ν(ξ)χ(ξ)||ν(ξ)1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1,χ(l+ϱ1))Q(ξ)fχK(ξ)||ν(ξ)1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1,ν(l+ϱ1))Q(ξ)fνK(ξ)|+1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)|Φ(l+ϱ1,χ(l+ϱ1))Φ(l+ϱ1,ν(l+ϱ1))|+|K(ξ)||fνfχ|.

    It follows that

    |ν(ξ)χ(ξ)|ϵΓ(ϱ+T+1)Γ(ϱ+1)Γ(T+1)+KΓ(ϱ)ξϱl=0(ξρ(l))(ϱ1)|χ(l+ϱ1)ν(l+ϱ1)|+|K(ξ)|K{λΓ(ϱ)Γ(β)ηl=ϱlϱτ=0(η+βρ(l))(β1)(lρ(τ))(ϱ1)|ν(l+ϱ1)χ(l+ϱ1)|+1Γ(ϱ)Tl=0(ϱ+Tρ(l))(ϱ1)|χ(l+ϱ1)ν(l+ϱ1)|}ϵΓ(ϱ+T+1)Γ(ϱ+1)Γ(T+1)+KχνΓ(ϱ)Γ(ξ+1)ϱΓ(ξ+1ϱ)+|K(ξ)|Kχν[MλΓ(ϱ)Γ(β)+1Γ(ϱ)Γ(ϱ+T+1)ϱΓ(T+1)]ϵΓ(ϱ+T+1)Γ(ϱ+1)Γ(T+1)+2KM1Γ(ϱ+1)Γ(ϱ+T+1)Γ(T+1)χν+χνKMM1λΓ(ϱ)Γ(β).

    Therefore,

    νχϵΓ(ϱ+T+1)Γ(ϱ+1)Γ(T+1)+νχ[2KM1Γ(ϱ+1)Γ(ϱ+T+1)Γ(T+1)+KMM1λΓ(ϱ)Γ(β)].

    Moreover, νχϵδ, where

    δ=Γ(β)Γ(ϱ+T+1)Γ(β)Γ(T+1)Γ(ϱ+1)2KM1Γ(ϱ+T+1)Γ(β)KMM1λϱΓ(T+1)>0.

    Thus, the discrete RL problem (4.1) is Hyers-Ulam stable.

    Lemma 4.4. If v solves (4.14) under the condition:

    (H6) The function θ:[ϱ3,ϱ+T]Nϱ3R is increasing and there exists a constant γ>0 such that

    1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)θ(l+ϱ1)γθ(ξ+ϱ1),ξ[0,T]N0,

    then

    |ν(ξ)1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1,ν(l+ϱ1))Q(ξ)fϕνK(ξ)|γθ(ξ+ϱ1).

    Proof. Let ν satisfy (4.14). From Remark 4.2, the solution to (H5) satisfies

    ν(ξ)=1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1,ν(l+ϱ1))+Q(ξ)+fνK(ξ)+1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)μ(l+ϱ1).

    Hence,

    |ν(ξ)1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)Φ(l+ϱ1,ν(l+ϱ1))Q(ξ)fνK(ξ)|=|1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)μ(l+ϱ1)|1Γ(ϱ)ξϱl=0(ξρ(l))(ϱ1)|μ(l+ϱ1)|ϵΓ(ϱ)ξϱl=0(ξρ(l))(ϱ1)|θ(l+ϱ1)|γϵθ(l+ϱ1),

    and the desired inequality is derived.

    Remark 4.3. About the restrictiveness of hypotheses (H1)(H6), and the bounds imposed on the family of discrete systems that satisfy them, one should note that such hypotheses are the usual conditions for proving existence, uniqueness or stability of solutions. In fact, the conditions (H2)(H6) are considered as the fundamental conditions in the definition of Hyers-Ulam-Rassias stability. Condition (H1) is a standard Lipschitz condition while other constants are computed based on the given fractional system. Therefore, these conditions are natural and, in real systems, with specified numerical data, their expressions are reduced to numerical bounds.

    Theorem 4.2. If the inequality (4.16) and the hypotheses (H1) and (H6) are satisfied, then the discrete RL problem (4.1) is Hyers-Ulam-Rassias stable.

    Proof. From Lemmas 4.4 and 2.3, we obtain that

    νχδ2ϵθ(ξ+ϱ1),

    where

    δ2=Γ(ϱ+1)Γ(β)Γ(T+1)Γ(ϱ+1)Γ(β)Γ(T+1)2KM1Γ(β)Γ(ϱ+T+1)KMM1λϱΓ(T+1)>0.

    Thus, the discrete RL problem (4.1) is Hyers-Ulam-Rassias stable.

    In this section, we consider two examples to illustrate the obtained results.

    Example 5.1. Let

    {Δϱξχ(ξ)=Φ(ξ+ϱ1,χ(ξ+ϱ1)),ξN0,4,Δχ(ϱ3)=1,χ(ϱ+4)=0.3Δ0.5χ(η+0.5),Δ2χ(ϱ3)=0, (5.1)

    where Δϱξ denotes the operator cΔϱξ or RLΔϱξ. Set β=0.5, T=4, λ=0.7, A1=1, A2=0, and

    Φ(ξ+1.5,χ(ξ+1.5))=137105sin(χ(ξ+1.5)).

    If Δϱξχ(ξ)=cΔ52ξχ(ξ) and η=52, then we obtain that

    K1=ληl=ϱ3(η+βρ(l))(β1)Γ(β)=λΓ(η+βϱ+4)βΓ(ηϱ+4)Γ(β)=0.9416,
    M=|ηl=ϱlϱξ=0(η+βρ(l))(β1)(lρ(ξ))(ϱ1)|=2.3562. (5.2)

    Hence, the inequality (3.8) takes the form

    Γ(ϱ+T+1)Γ(ϱ+1)Γ(T+1)(1+Γ(β)K1)+MλK1Γ(ϱ)68.94031K729.9270,

    such that

    K=137105.

    From Theorem 3.1, the discrete problem (5.1) has a unique solution.

    In the case Δϱξχ(ξ)=RLΔ3ξχ(ξ) and η=3, we obtain

    M=3.5449,M1=1.8824,hϱ=λΓ(η+βϱ+4)Γ(β+1)Γ(ηϱ+4)1=0.5313,K1=λΓ(η+βϱ+4)βΓ(ηϱ+4)Γ(β)=0.9416.

    Also,

    Γ(β)Γ(T+1)Γ(ϱ+1)2M1Γ(ϱ+T+1)Γ(β)+MM1λϱΓ(T+1)0.0075. (5.3)

    If K=0.0014<0.0075 and

    |RLΔ3ξν(ξ)Φ(ξ+2,v(ξ+2))|ϵ,ξ[0,4]N0, (5.4)

    holds, then, by Theorem 4.1, the discrete RL problem (5.1) is Hyers-Ulam stable.

    Example 5.2. Let

    {cΔ2.4ξχ(ξ)=1107χ4(ξ+1.4),ξN0,2,Δχ(0.4)=2,χ(3.4)=0.8Δ1/3χ(1/3+2.4),Δ2χ(0.6)=0. (5.5)

    After some calculations, we find that

    M=3.277,K1=ληl=ϱ3(η+βρ(l))(β1)Γ(β)=1.0253,K2=A1Γ(β)K1(ϱ+T)λA1K1(ηβ(3ϱ))Γ(ηϱ+β+4)β(β+1)Γ(ηϱ+4)=16.2963.

    We define the following Banach space:

    C(Nϱ3,ϱ+T,R)={χ(t)|[0.5,6.5]N0.5R,χ2|K2|=32.5927}.

    Note that

    |K2||[A1A2(ϱ3)]|(ϱ+T)(1)|A22|(ϱ+T)(2)Γ(ϱ+T+1)Γ(ϱ+1)Γ(T+1)(1+Γ(β)|K1|)+M|λ|Γ(ϱ)|K1|=0.3262.

    It is clear that |Φ(t,χ)|0.05860.3262 whenever χ[32.5927,32.5927]. Therefore, by Theorem 3.2, we find out that the discrete FBVP (5.5) has a solution.

    We proved existence and uniqueness of solution to discrete fractional boundary value problems (FBVPs) involving fractional difference operators via the Brouwer fixed point theorem and the Banach contraction principle. Different versions of stability criteria were obtained for a discrete FBVP involving Riemann-Liouville difference operators. The results were illustrated by suitable examples. The approach of this paper is new and can be a beginning method for discussing different real-world models in the context of discrete behavior structures. In particular, our results can contribute for the development of discrete fractional boundary value problems describing discrete dynamics of some physical applications. In future works, we plan to extend our approach to other types of discrete differential inclusions or fully-hybrid discrete fractional differential equations.

    The third and fourth authors would like to thank Azarbaijan Shahid Madani University. The fifth author was supported by the Portuguese Foundation for Science and Technology (FCT) and CIDMA through project UIDB/04106/2020. This research received funding support from the NSRF via the Program Management Unit for Human Resources & Institutional Development, Research and Innovation (Grant number B05F650018).

    The authors declare no conflict of interest.



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