Research article Special Issues

Positive solutions to integral boundary value problems for singular delay fractional differential equations

  • Delay fractional differential equations play very important roles in mathematical modeling of real-life problems in a wide variety of scientific and engineering applications. The objective of this manuscript is to study the existence and uniqueness of positive solutions for singular delay fractional differential equations with integral boundary data. To investigate the described system, we construct a u0-positive operator first. New research technique of by constructing u0-positive operator is used to overcome the difficulties caused by both the delays and the boundary value conditions. Then the sufficient conditions for the existence and uniqueness of positive solutions of a class of the singular delay fractional differential equations with integral boundary is proved by using the fixed point theorem in cone.

    Citation: Xiulin Hu, Lei Wang. Positive solutions to integral boundary value problems for singular delay fractional differential equations[J]. AIMS Mathematics, 2023, 8(11): 25550-25563. doi: 10.3934/math.20231304

    Related Papers:

    [1] Najla Alghamdi, Bashir Ahmad, Esraa Abed Alharbi, Wafa Shammakh . Investigation of multi-term delay fractional differential equations with integro-multipoint boundary conditions. AIMS Mathematics, 2024, 9(5): 12964-12981. doi: 10.3934/math.2024632
    [2] Asghar Ahmadkhanlu, Hojjat Afshari, Jehad Alzabut . A new fixed point approach for solutions of a $ p $-Laplacian fractional $ q $-difference boundary value problem with an integral boundary condition. AIMS Mathematics, 2024, 9(9): 23770-23785. doi: 10.3934/math.20241155
    [3] Yige Zhao, Yibing Sun, Zhi Liu, Yilin Wang . Solvability for boundary value problems of nonlinear fractional differential equations with mixed perturbations of the second type. AIMS Mathematics, 2020, 5(1): 557-567. doi: 10.3934/math.2020037
    [4] Md. Asaduzzaman, Md. Zulfikar Ali . Existence of positive solution to the boundary value problems for coupled system of nonlinear fractional differential equations. AIMS Mathematics, 2019, 4(3): 880-895. doi: 10.3934/math.2019.3.880
    [5] Yujun Cui, Chunyu Liang, Yumei Zou . Existence and uniqueness of solutions for a class of fractional differential equation with lower-order derivative dependence. AIMS Mathematics, 2025, 10(2): 3797-3818. doi: 10.3934/math.2025176
    [6] Chengbo Zhai, Yuanyuan Ma, Hongyu Li . Unique positive solution for a p-Laplacian fractional differential boundary value problem involving Riemann-Stieltjes integral. AIMS Mathematics, 2020, 5(5): 4754-4769. doi: 10.3934/math.2020304
    [7] Iyad Suwan, Mohammed S. Abdo, Thabet Abdeljawad, Mohammed M. Matar, Abdellatif Boutiara, Mohammed A. Almalahi . Existence theorems for $ \Psi $-fractional hybrid systems with periodic boundary conditions. AIMS Mathematics, 2022, 7(1): 171-186. doi: 10.3934/math.2022010
    [8] Limin Guo, Lishan Liu, Ying Wang . Maximal and minimal iterative positive solutions for $ p $-Laplacian Hadamard fractional differential equations with the derivative term contained in the nonlinear term. AIMS Mathematics, 2021, 6(11): 12583-12598. doi: 10.3934/math.2021725
    [9] Djamila Chergui, Taki Eddine Oussaeif, Merad Ahcene . Existence and uniqueness of solutions for nonlinear fractional differential equations depending on lower-order derivative with non-separated type integral boundary conditions. AIMS Mathematics, 2019, 4(1): 112-133. doi: 10.3934/Math.2019.1.112
    [10] Dumitru Baleanu, Babak Shiri . Generalized fractional differential equations for past dynamic. AIMS Mathematics, 2022, 7(8): 14394-14418. doi: 10.3934/math.2022793
  • Delay fractional differential equations play very important roles in mathematical modeling of real-life problems in a wide variety of scientific and engineering applications. The objective of this manuscript is to study the existence and uniqueness of positive solutions for singular delay fractional differential equations with integral boundary data. To investigate the described system, we construct a u0-positive operator first. New research technique of by constructing u0-positive operator is used to overcome the difficulties caused by both the delays and the boundary value conditions. Then the sufficient conditions for the existence and uniqueness of positive solutions of a class of the singular delay fractional differential equations with integral boundary is proved by using the fixed point theorem in cone.



    The fractional differential equations and delays arise naturally in a wide range of real-world phenomena and processes. Theory and applications of fractional differential system in different areas were considered by many researchers. For more details one can refer the books [1,2,3]. Some real-world models by fractional derivatives in engineering systems are presented in the book [4]. HIV/AIDS transmission models are investigated in [5]. Accelerated mass-spring systems are studied in [6]. Biochemical reaction models are studied in [7]. Chemical graph theory is given in [8,9]. During the last few decades, a lot of papers have been devoted to investigate the positive solutions of boundary value problems for fractional differential equations, such as [10,11,12,13,14,15,16,17]. The systems they studied are delay-free and most of them investigated the existence of positive solutions by using the classical fixed pointed methods. However, to our knowledge, on account of the need for resolving the difficulties caused by both the delays and the boundary value conditions, few results on the boundary value problems for fractional differential equations with time delays are appeared. For example, Qiao and Zhou [18] studied a class of boundary value problems for a fractional differential equation with integral boundary conditions but without time delays

    {Dp0+x(t)+p(t)f(t,x(t))+q(t)=0,t(0,1),x(0)=x(0)=0,x(1)=10l(s)x(s)ds, (1.1)

    where f:[0,1]×R(0,+) is continuous, q(t),l(t)C((0,1),[0,+)). Liao and Ye [19] investigated the existence and uniqueness of positive solutions for a class of nonlinear delay fractional differential equations

    {L(D)[x(t)x(0)]=f(t,xt),t(0,T],x(t)=ϕ(t),t[r,0], (1.2)

    where f:[0,1]×CR+ is continuous, in which R+=[0,+),C=C([r,0],R+) is the space of continuous functions from [r,0] to R+,r>0, L(D)=Dsnan1Dsn1a1Ds1, 0<sj<sj+1<1,aj>0,j=1,2,,n1. Dsj denotes the standard Riemann-Liouville fractional derivative. Using Krasnosel'skii fixed point theorem, Su in [20] examined the positive solutions to the singular delay fractional differential equations with easy boundary data

    {Ddx(t)+f(t,x(tτ))=0,t(0,1){τ},x(t)=η(t),t[τ,0],x(1)=0, (1.3)

    where f:(0,1)×R+R is continuous and may be singular at t=0,t=1,x=0, 1<d2 is a real number, Dd is the Riemann-Liouville fractional derivative, R+=[0,+). Li et al. [21] and Agarwal and Hristova [22] studied boundary value problems of some fractional functional differential equations involving the Caputo fractional derivative. However, the boundary value conditions in the above mentioned results for delay fractional differential equations are not concerned with the integral data. Despite many excellent works on integral boundary value problems for ordinary differential equations are available, there are only relatively scare results on the integral boundary value problems for delay fractional differential equations.

    Inspired by the works mentioned above, the present paper is related to studying the existence and uniqueness of positive solutions for the following delay fractional differential equations

    Dd0+x(t)+f(t,x(tτ))=0,t(0,1){τ} (1.4)

    with the more complicated integral boundary value conditions

    {x(t)=p(t),t[τ,0],x(0)=0,x(1)=10q(s)x(s)ds, (1.5)

    where Dd0+ is a standard Riemann-Liouville fractional derivative and d is a real number with 2<d3. The time delay τ is a constant which admits 0<τ<1. Throughout the present paper, the integral boundary value problems (IBVPs) (1.4) and (1.5) refers to the Eq (1.4) with boundary data (1.5). The functions f,p,q involved in IBVPs (1.4) and (1.5) are assumed to satisfy the following conditions:

    (H1) f:(0,1)×R+R+ is continuous, may be singular at t=0,t=1 and x=0.

    (H2) p(t)C([τ,0]),p(t)>0 for t[τ,0), and p(0)=0,p(0)=0, where p(0) denotes the left derivative of p at t=0.

    (H3) q:(0,1)R+ is continuous, and satisfies

    0Q:=10td1q(t)dt<1.

    A function x is said to be a positive solution of IBVPs (1.4) and (1.5) if x(t) is nonnegative on [τ,1], x(t)>0 for t[τ,1]{0} and it admits the Eq (1.4).

    The novelty of the present paper is twofold. First, IBVPs (1.4) and (1.5) under consideration involve not only the past time delay but also the fractional derivative with the order 2<d3. Second, the technique used in this paper is to construct a u0-positive operator as to overcome the difficulties caused by the singularity of the function f. Based on a fixed point theorem, some new existence and uniqueness criteria of positive solutions are established.

    The rest of this study is organized as follows. In Section 2, some definitions and lemmas are reviewed. In Section 3, we construct a u0-positive operator to demonstrate our main results. Then, the criteria to existence and uniqueness of positive solutions for IBVPs (1.4) and (1.5) can be established. We make a conclusion in Section 4.

    In this section, we resume with several necessary definitions and lemmas from fractional calculus theory.

    Definition 2.1. (e.g., [1,2,3]) The Riemann-Liouville fractional integral of a function u:(0,+)R with order d>0 is given by

    Id0+u(t)=1Γ(d)t0(ts)d1u(s)ds,

    provided that the right-hand side is pointwise defined on (0,+).

    In this section, we resume with several necessary definitions and lemmas from fractional calculus theory.

    Definition 2.2. (e.g., [1,2,3]) The Riemann-Liouville fractional integral of a function u:(0,+)R with order d>0 is given by

    Id0+u(t)=1Γ(d)t0(ts)d1u(s)ds,

    provided that the right-hand side is pointwise defined on (0,+).

    Definition 2.3. (e.g., [1,2,3]) The Riemann-Liouville fractional derivative of a continuous function u:(0,+)R with order d>0 is given by

    Dd0+u(t)=1Γ(nd)dndtnt0(ts)nd1u(s)ds,

    where n1d<n, provided that the right-hand side is pointwise defined on (0,+).

    The definition of a u0-positive operator is given as follows.

    Definition 2.4. (e.g., [23]) Let X be a Banach space, and P a cone in X. A bounded linear operator S:XX is said to be a u0-positive operator on the cone P if there exists u0P{θ} such that for every uP{θ}, there exists a natural number n and positive constants α(x),β(x) such that the following symmetric inequality is satisfied

    α(x)u0Snuβ(x)u0.

    Lemma 2.5. ([24]) Let d>0 and u(t) be an integrable function. Then,

    Id0+Dd0+u(t)=u(t)+c1td1+c2td2++cntdn,

    where ciR(i=1,2,,n), and n is the smallest integer greater than or equal to d.

    The following is an existence and uniqueness result of solutions for a linear boundary value problem, which is paramount for us in the following analysis.

    Lemma 2.6. Assume that ρC(0,1)L(0,1),2<d3. Then, the unique solution of the following BVPs

    {Dd0+x(t)+ρ(t)=0,t(0,1),x(0)=x(0)=0,x(1)=10q(s)x(s)ds, (2.1)

    is described by

    x(t)=10G(t,s)ρ(s)ds10(1sq(t)(ts)d1ρ(s)dt)ds(1Q)Γ(d)td1, (2.2)

    in which the constant

    Q:=10td1q(t)dt[0,1),

    and

    G(t,s)={1Γ(d)[td1(1s)d11Q(ts)d1],0st11Γ(d)td1(1s)d11Q,0ts1 (2.3)

    is called the Green function of the BVPs (2.1).

    Proof. Deduced from Lemma 2.5, we have

    x(t)=Id0+ρ(t)+c1td1+c2td2+c3td3.

    So, the solution of Eq (2.1) is

    x(t)=1Γ(d)t0(ts)d1ρ(s)ds+c1td1+c2td2+c3td3,

    where 2<d3. By the conditions x(0)=x(0)=0, we have that c2=c3=0. On the other hand, the condition x(1)=10q(s)x(s)ds yields

    1Γ(d)10(1s)d1ρ(s)ds+c1=10q(s)[1Γ(d)s0(sτ)d1ρ(τ)dτ+c1sd1]ds.

    By swapping the upper and lower limits, we have

    c1=10(1s)d1ρ(s)ds10[1tq(s)(st)d1ρ(t)ds]dt(1Q)Γ(d),

    where Q:=10td1q(t)dt[0,1). Therefore, the solution of BVPs (2.1) is

    x(t)=1Γ(d)t0(ts)d1ρ(s)ds+td1(1Q)Γ(d)10(1s)d1ρ(s)ds10[1tq(s)(st)d1ρ(t)ds]dt(1Q)Γ(d)td1=t01Γ(d)[td1(1s)d1(1Q)(ts)d1]ρ(s)ds+tt1Γ(d)td1(1s)d1(1Q)ρ(s)ds10[1tq(s)(st)d1ρ(t)ds]dt(1Q)Γ(d)td1=10G(t,s)ρ(s)ds10[1sq(t)(ts)d1ρ(s)dt]ds(1Q)Γ(d)td1.

    This completes the proof. ■

    Setting

    L(s)=1sq(t)(ts)d1dt(1Q)Γ(d). (2.4)

    Then, the solution of the BVPs (2.1) can be written as

    x(t)=10[G(t,s)L(s)td1]ρ(s)ds.

    We enjoy the following Lemma.

    Lemma 2.7. The Green function G(t,s) defined by (2.3) admits the following inequality

    G(t,s)L(s)td10,fort,s(0,1).

    Proof. From (2.3) and (2.4), for 0st1, one can calculate directly that

    G(t,s)L(s)td1=1Γ(d)[td1(1s)d11Q(ts)d1]1sq(t)(ts)d1dt(1Q)Γ(d)td11Γ(d)[td1(1s)d11Q(tts)d1]1sq(t)(ts)d1dt(1Q)Γ(d)td1=td1(1Q)Γ(d)[(1s)d1Q1sq(t)(ts)d1dt]td1(1Q)Γ(d)[10q(t)td1(1s)d1dt10q(t)(ts)d1dt]0.

    On the other hand, for 0ts1, noticing that 0Q<1, one can deduce that

    G(t,s)L(s)td1=1Γ(d)td1(1s)d11Q1sq(t)(ts)d1dt(1Q)Γ(d)td1>td1(1Q)Γ(d)[(1s)d1Q1sq(t)(ts)d1dt]td1(1Q)Γ(d)[10q(t)td1(1s)d1dt10q(t)(ts)d1dt]0.

    Hence, for any t,s(0,1), we have G(t,s)L(s)td10, which is the desired results. ■

    To proceed, we recall a result in [23].

    Lemma 2.8. (e.g., [23]) Let X be a Banach space, and P a cone in X. Suppose that S:XX is a completely continuous linear operator and S(P)P. If there exists ψX(P) and a constant c>0 such that cSψψ, then the spectral radius r(S)0, and S has a positive eigenfunction φ corresponding to its first eigenvalue λ1=1r(S), that is, φ=λ1Sφ.

    In this section, we begin with constructing a u0-positive operator; followed by the obtained results, the existence and uniqueness of positive solutions for IBVPs (1.4) and (1.5) is discussed in the succeeding subsection.

    We also need to define a space

    E={x(t):xC([τ,1],R+),x(t)=0fort[τ,0]}, (3.1)

    with the norm

    x∥=supt[τ,1]x(t)∣=supt[0,1]x(t).

    Then, it is not difficult to find that (E,) is a Banach space. A cone in the space E can be described as

    P={xE:x(t)0fort[τ,1]}.

    Let ρC(0,1)L(0,1) be a nonnegative function. We define the functions

    ¯p(t)={p(t),t[τ,0],0,t[0,1],
    ν(t)={0,t[τ,0],10[G(t,s)L(s)td1]ρ(s)ds,t[0,1],

    and, for any xP,

    x(t)=max{x(t)+¯p(t)ν(t),0}={p(t),t[τ,0],max{x(t)ν(t),0},t[0,1].

    The following is naturally followed by Lemma 2.6.

    Remark 3.1. The restriction of the function ν on [0,1]

    ν[0,1]=10[G(t,s)L(s)td1]ρ(s)ds

    is exactly the solution of the BVPs (2.1).

    To proceed, define an operator A in P as

    (Ax)(t)={0,t[τ,0],10[G(t,s)L(s)td1][f(s,x(sτ))+ρ(s)]ds,t(0,1]. (3.2)

    Lemma 2.6 means that if ˜x is a fixed point of the operator A, then ˜x is the solution of the following integral BVPs

    {Dd0+˜x(t)+f(t,˜x(tτ))+ρ(t)=0,t(0,1){τ},˜x(t)=0,t[τ,0],˜x(0)=0,˜x(1)=10q(s)˜x(s)ds.

    Hence, if the following inequality ˜x(tτ)+¯p(tτ)ν(tτ)0 fulfills for t[0,1], then

    ˜x(tτ)=˜x(tτ)+¯p(tτ)ν(tτ).

    Let

    x(t)=˜x(t)+¯p(t)ν(t), (3.3)

    where ˜x(t) is a fixed point of the operator A.

    By the definitions of the functions ¯p(t),ν(t), it is easy to conclude that x(t)=˜x(t)+¯p(t)ν(t)=p(t), for any t[τ,0]. By Remark 3.1, ν(1)=10q(s)ν(s)ds. Then, from the variable substitution (3.3) we have x(1)=˜x(1)+¯p(1)ν(1)=10q(s)˜x(s)ds10q(s)ν(s)ds=10q(s)x(s)ds. Hence, by the condition p(0)=0 in (H2), we conclude that the function x defined in (3.3) is the solution of IBVPs (1.4) and (1.5). As a result, in what follows one can just need to focus our study on finding the fixed points of the operator A defined by (3.2).

    Define another operator T be defined in P by

    (Ty)(t)={0,t[τ,0],10[G(t,s)L(s)td1]y(sτ)ds,t(0,1]. (3.4)

    By Lemma 2.7, it is not difficult to see that T:EE is a linear completely continuous operator and T(P)P.

    The u0-positive operator of the operator T defined by (3.4) can be constructed in the following theory.

    Theorem 3.2. The operator T defined by (3.4) is a u0-positive operator with u0(t)=td1.

    Proof. First, by the definition of the constant Q and the function L(s) defined in Lemma 2.6, we easily possess

    Q(1s)d1(1Q)Γ(d)L(s)=(1s)d1(1Q)Γ(d)10td1q(t)dt1s(ts)d1q(t)dt(1Q)Γ(d)=1(1Q)Γ(d)[10td1(1s)d1q(t)dt1s(ts)d1q(t)dt]1(1Q)Γ(d)[10(ts)d1q(t)dt1s(ts)d1q(t)dt]0,

    for t,s(0,1). Notice that 0Q<1. Thus, the following inequality

    (1s)d1(1Q)Γ(d)L(s)Q(1s)d1(1Q)Γ(d)L(s)0

    holds for t,s(0,1).

    For any yP{θ}, by (3.4) and (2.3), one can calculate that

    (Ty)(t)=t0{1Γ(d)[td1(1s)d11Q(ts)d1]L(s)td1}y(sτ)ds+1t[1Γ(d)td1(1s)d11QL(s)td1]y(sτ)ds=t0td1(1s)d1(1Q)Γ(d)y(sτ)dst0(ts)d1Γ(d)y(sτ)dst0L(s)td1y(sτ)ds+1ttd1(1s)d1(1Q)Γ(d)y(sτ)ds1tL(s)td1y(sτ)ds10td1(1s)d1(1Q)Γ(d)y(sτ)ds10L(s)td1y(sτ)ds=10[(1s)d1(1Q)Γ(d)L(s)]y(sτ)dstd1,t,s(0,1).

    On the other hand, for 0Q<1, one can deduce that

    (Ty)(t)=t0{1Γ(d)[td1(1s)d11Q(ts)d1]L(s)td1}y(sτ)ds+1t[1Γ(d)td1(1s)d11QL(s)td1]y(sτ)dst0{1Γ(d)[td1(1s)d11Q(tts)d1]L(s)td1}y(sτ)ds+1t[1Γ(d)td1(1s)d11QL(s)td1]y(sτ)ds=t0[Qtd1(1s)d1(1Q)Γ(d)L(s)td1]y(sτ)ds+1t[td1(1s)d1(1Q)Γ(d)L(s)td1]y(sτ)ds10Qtd1(1s)d1(1Q)Γ(d)y(sτ)ds10L(s)td1y(sτ)ds=10[Q(1s)d1(1Q)Γ(d)L(s)]y(sτ)dstd1,t,s(0,1).

    Therefore, for any yP{θ}, one can deduce that

    α(y)u0(Ty)(t)β(y)u0,

    where

    α(y)=10[Q(1s)d1Γ(d)(1Q)L(s)]y(sτ)ds,
    β(y)=10[(1s)d1Γ(d)(1Q)L(s)]y(sτ)ds.

    This implies that the operator T is a u0-operator with u0(t)=td1. ■

    By the proof of Theorem 3.2 and Lemma 2.8, we have the following lemma.

    Lemma 3.3. The spectral radius of the operator T admits r(T)0 and T has a positive eigenfunction φ(t) corresponding to its first eigenvalue λ1=(r(T))1.

    Proof. Let

    ψ(t)={0,t[τ,0],td1,t[0,1],

    and a constant

    c={10[Q(1s)d1Γ(d)(1Q)L(s)]ψ(sτ)ds}1>0.

    Then, from the proof of Theorem 3.2, we find that

    c(Tψ)(t)ψ(t).

    Thus, by Lemma 2.8, the spectral radius r(T)0 and T has a positive eigenfunction φ(t) corresponding to its first eigenvalue λ1=(r(T))1, that is φ(t)=λ1(Tφ)(t).

    The following result can be used in the proof of the main result in this paper.

    Remark 3.4. Let φ(t) be the positive eigenfunction of operator T corresponding to λ1, that is,

    λ1(Tφ)(t)=φ(t).

    Then, by Theorem 3.2 and Definition 2.4, there exists k1(φ),k2(φ) such that

    k1(φ)u0Tφ=1λ1φk2(φ)u0,φP{θ}.

    Hence, we obtain that T defined by (3.4) is a u0-positive operator with u0(t)=φ(t).

    In this subsection, based on a fixed point theorem, we study the existence and uniqueness of positive solutions for IBVPs (1.4) and (1.5) by using the u0-positive operators. The following theorem is the main result in this paper.

    Theorem 3.5. Assume that conditions (H1)(H3) hold and there exists a constant k[0,1) such that

    f(t,u)f(t,v)∣≤kλ1uv,foranyt[0,1],u,vR, (3.5)

    where λ1 is the first eigenvalue of the operator T defined by (3.4). Then, IBVPs (1.4) and (1.5) has a unique positive solution x. Moreover, for any x0P, the iterative sequence xn=Axn1(n=1,2,) converges to x.

    Proof. Owing to the continuity of f and the fact that T is a linear completely continuous operator, it is not difficult to verify that the operator A:EE defined by (3.2) is completely continuous and satisfies A(P)P.

    For any given x0P, define the iterative sequence xn=Axn1(n=1,2,). Since A(P)P, it follows that {xn}P.

    Since λ1 is the first eigenvalue of T, that is T(φ(t))=1λ1φ(t), by the linearity of the operator T, stepwise recursive yields

    Tn1(φ(t))=Tn2(1λ1φ(t))=1λ1Tn2(φ(t))==1λn11φ(t).

    Thus, for nN+, by (3.1), one can deduce that

    xn+1(t)xn(t)=∣(Axn)(t)(Axn1)(t)=∣10[G(t,s)L(s)td1][f(s,xn(sτ))+ρ(s)]ds10[G(t,s)L(s)td1][f(s,xn1(sτ))+ρ(s)]ds1τ[G(t,s)L(s)td1]f(s,xn(sτ)ν(sτ))f(s,xn1(sτ)ν(sτ))dskλ11τ[G(t,s)L(s)tα1]xn(sτ)xn1(sτ)dskλ1T(xnxn1)(t)knλn1Tn(x1x0)(t).

    By Theorem 3.2 and Remark 3.4, there is a constant δ1=δ1(x1x0)>0 such that

    T(x1x0)(t)δ1φ(t),t[0,1],

    where φ(t) is the positive eigenfunction of operator T corresponding to λ1. Then, for nN+, we have

    xn+1(t)xn(t)knλn1Tn1(δ1φ(t))=δ1knλn1Tn1(φ(t))=δ1knλn11λn11φ(t)=δ1λ1knφ(t).

    It follows that for any mN+

    xn+m(t)xn(t)≤∣xn+m(t)xn+m1(t)++xn+1(t)xn(t)δ1λ1(kn+m1++kn)φ(t)=δ1λ1kn(1km)1kφ(t)δ1λ1kn1kφ(t),

    which means that

    xn+mxn∥≤δ1λ1kn1kφ.

    Note that limnβ1λ1kn1kφ(t)=0. Thus, {xn} is a Cauchy sequence. Therefore, from the completeness of the space E and the closeness of the operator P, there exists xP such that

    limnxn=x.

    Since the operator A is continuous, taking the limit into xn=Axn1 demonstrate that x is a fixed point of A in P.

    Next, we demonstrate that A has at most one fixed point in P. Suppose that there exist two elements x,yX with x=Ax and y=Ay. Then, by the condition (3.1), for any nN+, one can calculate

    x(t)y(t)=∣(Anx)(t)(Any)(t)=∣[A(An1x)](t)[A(An1y)](t)=∣10[G(t,s)L(s)td1][f(s,(An1x)(sτ))+ρ(s)]ds10[G(t,s)L(s)td1][f(s,(An1y)(sτ))+ρ(s)]ds1τ[G(t,s)L(s)td1]f(s,(An1x)(sτ)ν(sτ))f(s,(An1y)(sτ)ν(sτ))dskλ11τ[G(t,s)L(s)td1](An1x)(sτ)(An1y)(sτ)dskλ1T(An1xAn1y)(t)knλn1Tn(xy)(t).

    Invoking again Theorem 3.2 and Corollary 3.4, there exists a constant δ2=δ2(xy)>0 such that

    T(xy)(t)δ2φ(t),t[0,1].

    Hence, we obtain

    x(t)y(t)knλn1Tn(xy)(t)knλn1Tn1(δ2φ(t))=δ2knλn11λn11φ(t)=δ2λ1knφ(t),
    T(x1x0)(t)δ1φ(t),t[0,1],

    where φ(t) is the positive eigenfunction of operator T corresponding to the first eigenvalueλ1. It follows that

    xy∥≤δ2λ1knφ.

    Observing that k[0,1), we have

    limn+δ2λ1knφ=0,

    so xy∥≤0, and thus x=y.

    Based on the above analysis, x is a unique fixed point of A in P, i.e., x is the unique positive solution of IBVP (1.4) and (1.5). ■

    In this paper, a novel technique of u0-positive operator is invoked to establish the existence and uniqueness of positive solutions for a class of the singular delay fractional differential equations with integral boundary, that is, IBVPs (1.4) and (1.5), which involves not only the past time delay but also the fractional derivative with the order 2<d3. We first get the corresponding Green's function. Consequently, the u0-positive operator T is derived by the equivalent integral equation of IBVP (1.4) and (1.5). Hence, the sufficient conditions for the existence and uniqueness of positive solutions of the problem is proved by using the fixed point theorem in cone.

    On open questions for further research, it would be interesting to see what happen when the equation includes this term x(t) in the function f, i.e., f(t,x(t),x(tτ)). Another potentially interesting research direction would be to take d(1,2].

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    This research was supported by the University Science Research Key Project of Anhui Province under Grant No. KJ2021A1000 and No. KJ2021A0996, Talent Research Fund of Hefei University under Grant No. 20RC26.

    The authors declare no conflicts of interest regarding this article.



    [1] A. A. Kilbas, H. M. Srivastava, J. J. Trujillo, Theory and applications of fractional differential equations, Elsevier, B. V. Amsterdam, 2006.
    [2] I. Podlubny, Fractional differential equations, Academic Press, San Diego, 1999.
    [3] A. A. Kilbas, O. I. Marichev, S. G. Samko, Fractional integral and derivatives: Theory and applications, Gordon and Breach, Yverdon, 1993.
    [4] R. L. Magin, Fractional calculus in bioengineering, Begell House Publishers, Redding, CT, USA, 2006.
    [5] D. Baleanu, M. Hasanabadi, A. M. Vaziri, A. Jajarmi, A new intervention strategy for an HIV/AIDs transmission by a general fractional modeling and an optimal control approach, Chaos Soliton. Fract., 167 (2023), 113078. https://doi.org/10.1016/j.chaos.2022.113078 doi: 10.1016/j.chaos.2022.113078
    [6] O. Defterli, D. Baleanu, A. Jajarmi, S. S. Sajjadi, N. Alshaikh, J. H. Asad, Fractional treatment: An accelerated mass-spring system, Romanian Rep. Phys., 74 (2022), 122.
    [7] A. Akgül, S. A. Khoshnaw, Application of fractional derivative on non-linear biochemical reaction models, Int. J. Intell. Networks, 1 (2020), 52–58. https://doi.org/10.1016/j.ijin.2020.05.001 doi: 10.1016/j.ijin.2020.05.001
    [8] A. Turab, Z. D. Mitroviˊc, A. Saviˊc, Existence of solutions for a class of nonlinear boundary value problems on the hexasilinane graph, Adv. Differ. Equ., 2021 (2021), 494. https://doi.org/10.1186/s13662-021-03653-w doi: 10.1186/s13662-021-03653-w
    [9] M. M. Moutamal, C. Joseph, Optimal control of fractional Sturm-Liouville wave equations on a star graph, Optimization, 2022. http://dx.doi.org/10.1080/02331934.2022.2088370
    [10] N. Bouteraa, S. Benaicha, A study of existence and multiplicity of positive solutions for nonlinear fractional differential equations with non-local boundary conditions, Stud. Univ. Babes-Bol. Math., 66 (2021), 361–380. http://dx.doi.org/10.24193/subbmath.2021.2.1 doi: 10.24193/subbmath.2021.2.1
    [11] Y. Cui, Uniqueness of solution for boundary value problems for fractional differential equations, Appl. Math. Lett., 51 (2016), 48–54. https://doi.org/10.1016/j.aml.2015.07.002 doi: 10.1016/j.aml.2015.07.002
    [12] R. Agarwal, Y. Liu, D. O'Regan, C. Tian, Positive solutions of two-point boundary value problems for fractional singular differential equations, Differ. Equ., 48 (2012), 619–629.
    [13] I. Bachar, H. Mˆaagli, F. Toumi, Z. Z. Abidine, Existence and global asymptotic behavior of positive solutions for sublinear and superlinear fractional boundary value problems, Chinese Ann. Math. B, 37 (2016), 1–28. https://doi.org/10.1007/s11401-015-0943-3 doi: 10.1007/s11401-015-0943-3
    [14] Y. Xu, Fractional boundary value problems with integral and anti-periodic boundary conditions, B. Malays. Math. Sci. So., 39 (2016), 571–587. https://doi.org/10.1007/s40840-015-0126-0 doi: 10.1007/s40840-015-0126-0
    [15] H. Feng, C. Zhai, Existence and uniqueness of positive solutions for a class of fractional differential equation with integral boundary conditions, Nonlinear Anal.-Model., 22 (2017), 160–172. https://doi.org/10.15388/NA.2017.2.2 doi: 10.15388/NA.2017.2.2
    [16] Y. Cui, W. Ma, Q. Sun, X. Su, New uniqueness results for boundary value problem of fractional differential equation, Nonlinear Anal.-Model., 23 (2018), 31–39. https://doi.org/10.15388/NA.2018.1.3 doi: 10.15388/NA.2018.1.3
    [17] W. Liu, L. Liu, Existence and stability analysis of solutions for a new kind of boundary value problems of nonlinear fractional differential equations, Nonlinear Anal.-Model., 27 (2022), 1068–1087. https://doi.org/10.15388/namc.2022.27.29420 doi: 10.15388/namc.2022.27.29420
    [18] Y. Qiao, Z. Zhou, Existence and uniqueness of positive solutions for a fractional differential equation with integral boundary conditions, Adv. Differ. Equ., 2016 (2016), 106–113. https://doi.org/10.1186/s13662-016-0772-z doi: 10.1186/s13662-016-0772-z
    [19] C. Liao, H. Ye, Existence of positive solutions of nonlinear fractional delay differential equations, Positivity, 13 (2009), 601–609. https://doi.org/10.1007/s11117-008-2251-6 doi: 10.1007/s11117-008-2251-6
    [20] X. Su, Positive solutions to singular boundary value problems for fractional functional differential equations with changing sign nonlinearity, Comput. Math. Appl., 64 (2012), 3425–3435. https://doi.org/10.1016/j.camwa.2012.02.043 doi: 10.1016/j.camwa.2012.02.043
    [21] Y. Li, S. Sun, D. Yang, Z. Han, Three-point boundary value problems of fractional functional differential equations with delay, Bound. Value Probl., 38 (2013), 1–15. https://doi.org/10.1186/1687-2770-2013-38 doi: 10.1186/1687-2770-2013-38
    [22] R. P. Agarwal, S. Hristova, Boundary value problem for multi-term nonlinear delay generalized proportional Caputo fractional differential equations, Fractal Fract., 6 (2022), 691. https://doi.org/10.3390/fractalfract6120691 doi: 10.3390/fractalfract6120691
    [23] M. A. Krasnosel'skii, Positive solutions of operator equations, Noordhoff, Groningen, The Netherlands, 1964.
    [24] D. Jiang, C. Yuan, The positive properties of the green function for Dirichlet-type boundary value problems of nonlinear fractional differential equations and its applications, Nonlinear Anal.-Theor., 72 (2010), 710–719. https://doi.org/10.1016/j.na.2009.07.012 doi: 10.1016/j.na.2009.07.012
  • Reader Comments
  • © 2023 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(1474) PDF downloads(187) Cited by(0)

Other Articles By Authors

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog