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Research article

Multiple solutions for a class of boundary value problems of fractional differential equations with generalized Caputo derivatives

  • Received: 03 August 2021 Accepted: 09 September 2021 Published: 14 September 2021
  • MSC : 34B18, 34A34, 26A33

  • This paper is mainly concerned with the existence of multiple solutions for the following boundary value problems of fractional differential equations with generalized Caputo derivatives:

    {C0Dαgx(t)+f(t,x)=0, 0<t<1;x(0)=0, C0D1gx(0)=0, C0Dνgx(1)=10h(t)C0Dνgx(t)g(t)dt,

    where 2<α<3, 1<ν<2, αν1>0, fC([0,1]×R+,R+), g>0, hC([0,1],R+), R+=[0,+). Applying the fixed point theorem on cone, the existence of multiple solutions for considered system is obtained. The results generalize and improve existing conclusions. Meanwhile, the Ulam stability for considered system is also considered. Finally, three examples are worked out to illustrate the main results.

    Citation: Yating Li, Yansheng Liu. Multiple solutions for a class of boundary value problems of fractional differential equations with generalized Caputo derivatives[J]. AIMS Mathematics, 2021, 6(12): 13119-13142. doi: 10.3934/math.2021758

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  • This paper is mainly concerned with the existence of multiple solutions for the following boundary value problems of fractional differential equations with generalized Caputo derivatives:

    {C0Dαgx(t)+f(t,x)=0, 0<t<1;x(0)=0, C0D1gx(0)=0, C0Dνgx(1)=10h(t)C0Dνgx(t)g(t)dt,

    where 2<α<3, 1<ν<2, αν1>0, fC([0,1]×R+,R+), g>0, hC([0,1],R+), R+=[0,+). Applying the fixed point theorem on cone, the existence of multiple solutions for considered system is obtained. The results generalize and improve existing conclusions. Meanwhile, the Ulam stability for considered system is also considered. Finally, three examples are worked out to illustrate the main results.



    The fractional calculus is a branch of mathematics, which studies the integration and differentiation of any order in real or complex field. In 1832, the fractional derivative was first formally proposed by Liouville. See [1,2] for more knowledge on fractional calculus. The fractional order differential equation (FDE, for short) is a generalization of classical integer order differential equation as well, which can describe complex with simple modeling, clear physical meaning of parameters, accurate selection and so on. Hence, it becomes an important tool for mathematical modeling of complex machines, physical processes, fluid dynamics, finance and other areas of applications (see [3,4] and references therein). In recent decades, more and more researchers pay much attention to the fractional differential equations and have obtained substantial achievements. For example, S. Salahshour and A. Ahmadian et al. researched the heat transfer problem with a approach of fractional modeling [5], successive approximation method for Caputo q-fractional IVPs [6] and M-fractional derivative under interval uncertainty [7]. N. Sene investigated chaotic system involving Caputo fractional derivatives in [8,9]. [10,11,12] were concerned with fractional diffusion equation. [13,14] studied infinitely many solutions for impulsive fractional boundary value problem with p-Laplacian and for fractional schrodinger-maxwell equations, respectively. [15,16,17] analyzed the Ulam stability of nonlinear FDEs. [18,19] investigated the controllability for two classes of semilinear fractional evolution systems.

    In the last few years, boundary value problems of fractional differential equations (FBVPs, for short) have been extensively studied. Most of them have been considered in the frame of standard fractional derivatives such as Rieman-Liouvile and Caputo derivatives. For instance, [20] is concerned with positive solutions of a two-point boundary value problem for singular fractional differential equations in Banach space. [21,22,23] developed bifurcation techniques for FBVPs. [24,25,26] investigated positive solutions for FBVPs. [27,28] dealt with coupled fractional differential systems with nonlocal boundary conditions. [29,30,31] studied FBVPs via critical point theory. [32,33] were concerned with the solvability for multi-order nonlinear fractional systems and periodic boundary value problems of nonlinear fractional hybrid differential equations. [34] investigated positive solutions for nonlinear discrete FBVPs with a p-laplacian operator.

    More generally, A. Babakhani in [35] considered

    {ddtCDα0+u(t)+q(t)f(u(t),u(t))=0, 0t1, 1<α<2,u(0)=0, u(1)=v>0, (CDα0+u)(1)=10(CDα0+u)(s)dg(s),

    where CDα0+ is the Caputo fractional derivative of order α, f:[0,1]×R2R is a given continuous function and g:[0,1][0,+) is nondecreasing function. By constructing a special cone, the existence of at least one positive solution was obtained under some suitable assumptions. In [36], Y. Li studied the following fractional q-difference equations involving q-integral boundary conditions:

    {Dαqx(t)+f1(t,y(t))=0, 0<t<1;Dαqy(t)+f2(t,x(t))=0, 0<t<1;x(0)=0, D1qx(0)=0, Dνqx(1)=10h(t)Dνqx(t)dqt;y(0)=0, D1qy(0)=0, Dνqy(1)=10h(t)Dνqy(t)dqt,

    where 2<α<3, 1<ν<2, Dνq is α-order Riemann-Liouville's fractional q-derivative. The existence of nontrivial solutions is obtained by using topological degree theory.

    With the development of investigation on fractional derivatives, new concepts are constantly being put forward. For instance, F. Jarad et al. proposed a new kind of generalized fractional derivatives and studied their properties in [37,38]. N. Sene investigates fractional advection-dispersion equation described by the Caputo left generalized fractional derivative in [39]. [40] studied Ulam stabilities of fractional differential equations including generalized Caputo fractional derivative. However, to our best knowledge, there are few studies on the existence of multiple solutions and Ulam-Hyers stability for integral boundary value problems of FDES with generalized Caputo derivatives. The purpose of present paper is to fill this gap.

    Motivated by the above discussions, this paper studies multiple solutions and Ulam-Hyers stability for the following FBVPs with generalized Caputo derivatives

    {C0Dαgx(t)+f(t,x)=0, 0<t<1;x(0)=0, C0D1gx(0)=0, C0Dνgx(1)=10h(t)C0Dνgx(t)g(t)dt, (1.1)

    where 2<α<3, 1<ν<2, αν1>0, fC([0,1]×R+,R+), g>0, hC([0,1],R+), R+=[0,+). The main features of this paper are as follows. Firstly, compared with the above mentioned references, BVP (1.1) is studied in the sense of generalized Caputo fractional derivatives, which is also different from fractional q-difference equations in [36]. Secondly, the fractional boundary value condition we consider here is of integral form, and that makes BVP (1.1) more widely applicable in solving practical problems. Thirdly, the used approach in this paper has certain advantages over some references listed as above. In detail, the distinctive tool used here is the first eigenvalue of corresponding linear operator. At the same time, a suitable cone is established by researching properties of Green's function deeply. So the positive solutions can be obtained by means of the cone expansion and compression fixed point theorem and Leggett-Williams theorem. Finally, the Ulam-Hyers stability and generalized Ulam-Hyers stability for BVP (1.1) are also studied under some suitable assumptions.

    The remainder of this paper is organized as follows: Some basic knowledge of fractional calculous and some preliminary results are given in Section 2. The existence results will be given and proved in Section 3. And in Section 4, the Ulam-Hyers stability and generalized Ulam-Hyers stability will be established. Three examples are worked out to illustrate the main results in Section 5. Finally, the conclusion and some future works are given in Section 6.

    Definition 2.1. [38] (1) Let gCn[a,b] such that g(t)>0 on [a,b]. Define

    ACng=:{f:[a,b]C and f[n1]AC[a,b]},

    where f[n1]=(1g(t)ddt)n1f.

    (2)

    Cε,g[a,b]=:{f:(a,b]R such that (g(t)g(a))εf(t)C[a,b]},

    where C0,g=C[a,b].

    (3)

    Cnε,g[a,b]=:{f:(a,b]R such that f[n1]C[a,b] and f[n]Cε,g[a,b]},

    where Cn0,g=C[a,b].

    Definition 2.2. [38] (1) The Riemann-Liouville fractional integral of order αR+ of a function f on a finite or infinite interval (a,b) is defined as follows:

    (aIαy)(t)=1Γ(α)ta(ts)α1y(s)ds.

    (2) The Riemann-Liouville fractional derivative of order αR+ of a function f on a finite or infinite interval (a,b) is defined as follows:

    (aDαy)(t)=1Γ(nα)(ddt)nta(ts)nα1y(s)ds,

    where n=[α]+1, g(i)0,i=1,2,...,n.

    Definition 2.3. [38] The Caputo fractional derivative of order αR+ of a function f on a finite or infinite interval (a,b) is defined as follows:

    (CaDαy)(t)=1Γ(nα)ta(ts)nα1y(n)(s)ds.

    Definition 2.4. [38] (1) The generalized Riemann-Liouville fractional integral of order αR+ of a function f with respect to the function g on a finite or infinite interval (a,b) is defined as follows:

    (aIαgy)(t)=1Γ(α)ta(g(t)g(s))α1y(s)g(s)ds.

    (2) The generalized Riemann-Liouville fractional derivative of order αR+ of a function f with respect to the function g on a finite or infinite interval (a,b) is defined as follows:

    (aDαgy)(t)=1Γ(nα)(1g(t)ddt)nta(g(t)g(s))nα1y(s)g(s)ds,

    where n=[α]+1, g(i)0,i=2,...,n.

    Definition 2.5. [38] The generalized Caputo fractional derivative of order αR+ of a function f with respect to another function g on a finite or infinite interval (a,b) is defined as follows:

    (CaDαgy)(t)=1Γ(nα)ta(g(t)g(s))nα1y[n](s)g(s)ds,

    where y[n]=(1g(t)ddt)n, n=[α]+1, g(i)0,i=2,...,n.

    Remark 2.6. From the Definition 2.4 (1) and Definition 2.5 above, we can see that

    (CaDαgy)(t)=1Γ(nα)ta(g(t)g(s))nα1y[n](s)g(s)ds= aInαgy[n](t).

    Lemma 2.7. [38] Let gCn[a,b] such that g(t)>0 on [a,b]. Then yACng if and only if it can be written as that

    y(t)=1(n1)!ta(g(t)g(s))n1y[n](s)g(s)ds+n1k=0y[k](a)k!(g(t)g(a))k. (2.1)

    Lemma 2.7. [38] Let α>0, n=[α]+1 and yACng[a,b]. Then the fractional derivative of y with respect to g exists almost everywhere and

    (aDαgy)(t)=1Γ(nα)ta(g(t)g(s))nα1y[n](s)g(s)ds+n1k=0y[k](a+)Γ(kα1)(g(t)g(a))kα. (2.2)

    Remark 2.9. [38] Equation (2.2) can be written as that

    (aDαgy)(t)=(aInαg)y[n](t)+n1k=0y[k](a+)Γ(kα1)(g(t)g(a))kα,

    and thus, one can define the Caputo fractional derivative of a function with respect to another function as

    (CaDαgy)(t)=(aDαgy)(t)n1k=0y[k](a+)Γ(kα1)(g(t)g(a))kα= aDαg(y(s)n1k=0y[k](a+)k!(g(t)g(a))k)(t).

    Similar to Caputo fractional derivative, we can easily obtain the following properties.

    Lemma 2.10. Let α>0, CaDαg be a generalized Caputo fractional derivative of α, y(t)C[0,1]. Then,

    aIαg CaDαgy(t)=y(t)n1k=0y[k](a)k!(g(t)g(a))k,

    where g(k)0, \ k=0, 1, 2, , n, \ n=[α]+1.

    Proof. The proof is done by using Remark 2.6 and Lemma 2.7.

    aIαg CaDαgy(t)= aIαg aInαgy[n](t)= aIngy[n](t)= y(t)n1k=0y[k](a)k!(g(t)g(a))k,

    where g(k)0, k=0, 1, 2, , n, n=[α]+1.

    The proof is completed.

    Lemma 2.11. Let A=110h(t)(g(t)g(0)g(1)g(0))αv1g(t)dt0. Then the following boundary value problem

    {(C0Dαgx)(t)+y(t)=0, 0<t<1;x(0)=0, C0D1gx(0)=0, C0Dνgx(1)=10h(t)C0Dνgx(t)g(t)dt, (2.3)

    has a unique solution

    x(t)=10G(t,s)y(s)g(s)ds:=Sy(t),

    where

    B=(g(1)g(0))αv1A, L=Γ(3)Γ(3ν),
    G(t,s)=G0(t,s)+(g(t)g(0))2BLΓ(αν)10h(t)G1(t,s)g(t)dt,
    G0(t,s)={1LΓ(αν)(g(t)g(0))2(g(1)g(s))αv1(g(1)g(0))2ν1Γ(α)(g(t)g(s))α1,0st1;1LΓ(αν)(g(t)g(0))2(g(1)g(s))αv1(g(1)g(0))2ν,0ts1,
    G1(t,s)=1LΓ(αν){(g(t)g(0))2ν(g(1)g(s))αv1(g(1)g(0))2ν(g(t)g(s))αν1,0st1;(g(t)g(0))2ν(g(1)g(s))αv1(g(1)g(0))2ν,0ts1.

    Proof. Using Definition 2.4 and Definition 2.5, one can obtain that

    x(t)=c0+c1(g(t)g(0))+c2(g(t)g(0))2 0Iαgy(t).

    Noticing that x(0)=(C0D1gx)(0)=0, one can deduce that c0=c1=0. Hence,

    x(t)=c2(g(t)g(0))2 0Iαgy(t). (2.4)

    By (2.4), one can easily get that

    (C0Dνgx)(t)= C0Dνg[c2(g(t)g(0))2 0Iαgy(t)]=c2Γ(3)Γ(3ν)(g(t)g(0))2ν(C0Dνg)(0Iαgy)(t)=c2Γ(3)Γ(3ν)(g(t)g(0))2ν(0Iανgy)(t)=c2Γ(3)Γ(3ν)(g(t)g(0))2ν1Γ(αν)t0(g(t)g(s))αν1y(s)g(s)ds.

    Obviously,

    (C0Dνgx)(1)=c2Γ(3)Γ(3ν)(g(1)g(0))2ν1Γ(αν)10(g(1)g(s))αν1y(s)g(s)ds. (2.5)

    Applying

    (C0Dνgx)(1)=10h(t)C0Dνgx(t)g(t)dt

    and (2.5), it is immediate to see that

    (C0Dνgx)(1)=10h(t)C0Dνgx(t)g(t)dt=c2Γ(3)Γ(3ν)10h(t)(g(t)g(0))2νg(t)dt1Γ(αν)10h(t)[t0(g(t)g(s))αν1y(s)g(s)ds]g(t)dt.

    Hence, we deduce that

    c2=1BLΓ(αν)10(g(1)g(s))αν1y(s)g(s)ds1BLΓ(αν)10h(t)[t0(g(t)g(s))αν1y(s)g(s)ds]g(t)dt.

    Moreover, by (2.4), one can get that

    x(t)=1BLΓ(αν)10(g(t)g(0))2(g(1)g(s))αν1y(s)g(s)ds(g(t)g(0))2BLΓ(αν)10h(t)[t0(g(t)g(s))αν1y(s)g(s)ds]g(t)dt1Γ(α)t0(g(t)g(s))α1y(s)g(s)ds=1BLΓ(αν)10(g(t)g(0))2(g(1)g(s))αν1y(s)g(s)ds(g(t)g(0))2BLΓ(αν)10h(t)[t0(g(t)g(s))αν1y(s)g(s)ds]g(t)dt1Γ(α)t0(g(t)g(s))α1y(s)g(s)ds+1L(g(1)g(0))2νΓ(αν)10(g(t)g(0))2(g(1)g(s))αν1y(s)g(s)ds1L(g(1)g(0))2νΓ(αν)10(g(t)g(0))2(g(1)g(s))αν1y(s)g(s)ds=10G0(t,s)y(s)g(s)ds+(g(1)g(0))2νBLΓ(αν)10(g(t)g(0))2(g(1)g(s))αν1(g(1)g(0))2νy(s)g(s)ds(g(t)g(0))2BLΓ(αν)10h(t)[t0(g(t)g(s))αν1y(s)g(s)ds]g(t)dtBBLΓ(αν)10(g(t)g(0))2(g(1)g(s))αν1(g(1)g(0))2νy(s)g(s)ds=10G0(t,s)y(s)g(s)ds(g(t)g(0))2BLΓ(αν)10h(t)[t0(g(t)g(s))αν1y(s)g(s)ds]g(t)dt+(g(1)g(0))2ν(g(t)g(0))2BLΓ(αν)10(g(1)g(s))αν1(g(1)g(0))2νy(s)g(s)dsB(g(t)g(0))α1BLΓ(α)10(g(1)g(s))αν1(g(1)g(0))2νy(s)g(s)ds]=10G0(t,s)y(s)g(s)ds(g(t)g(0))2BLΓ(αν)10h(t)[t0(g(t)g(s))αν1y(s)g(s)ds]g(t)dt+(g(t)g(0))2BLΓ(αν)10h(t)(g(t)g(0))2νg(t)dt10(g(1)g(s))αν1(g(1)g(0))2νy(s)g(s)ds=10G0(t,s)y(s)g(s)ds+(g(t)g(0))2BLΓ(αν)10[10h(t)(g(t)g(0))2ν(g(1)g(s))αν1(g(1)g(0))2νg(t)dt1sh(t)(g(t)g(s))αν1g(t)dt]y(s)g(s)ds=10G0(t,s)y(s)g(s)ds+(g(t)g(0))2BLΓ(αν)10[10h(t)G1(t,s)g(t)dt]y(s)g(s)ds=10G(t,s)y(s)g(s)ds.

    The proof is completed.

    Suppose that (2ν)(g(t)g(s))(αν1)(g(t)g(0)), for 0st1 in the rest of the paper. $

    Lemma 2.12. The functions Gi(i=0,1) has the following properties:

    (1) G0(t,s)0 for s, t[0,1];

    (2) G1(t,s)0 for s, t[0,1];

    (3) G0(t,s)G0(1,s) for s, t[0,1];

    (4) G0(t,s)(g(t)g(0)g(1)g(0))2G0(1,s) for s, t[0,1].

    Proof. (1) On the one hand, for 0st1, we know

    G0(t,s)=1LΓ(αν)(g(t)g(0))2(g(1)g(s))αv1(g(1)g(0))2ν1Γ(α)(g(t)g(s))α1.

    By careful calculation, we can see

    G[3]0(t,s)=(1g(t)ddt)3G0(t,s)=1Γ(α)(α1)(α2)(α3)(g(t)g(s))α30.

    With the property of g(t), it implies that

    G[2]0(t,s)G[2]0(s,s)0.

    Similarly,

    G[1]0(t,s)G[1]0(s,s)0.

    Thus, it is easy to see that

    G0(t,s)G0(s,s)=1LΓ(αν)(g(s)g(0))2(g(1)g(s))αv1(g(1)g(0))2ν0.

    On the other hand, for 0ts1, it is easy to see that from Lemma 2.10, G0(t,s)0  for s, t[0,1].

    (2) For 0st1, from (2ν)(g(t)g(s))(αν1)(g(t)g(0)), (g(t)g(s))αν1(g(t)g(0))2ν is a nondecreasing function for t \ on\ [0,1].

    Then,

    G1(t,s)=1LΓ(αν)[(g(t)g(0))2ν(g(1)g(s))αv1(g(1)g(0))2ν(g(t)g(s))αν1]=1LΓ(αν)[(g(t)g(0))2ν((g(1)g(s))αν1(g(1)g(0))2ν(g(t)g(s))αν1(g(t)g(0))2ν)]0.

    On the other hand, for 0ts1, it is easy to see that from Lemma 2.10 the conclusion is obviously established. Therefore, G1(t,s)0 for s,t[0,1].

    (3) For s,t[0,1], from (1) and Lemma 2.10, one can easily obtain that G0(t,s) is an increasing function with respect to t. Then, G0(t,s)G0(1,s).

    (4) For 0st1, from (2ν)(g(t)g(s))(αν1)(g(t)g(0)), (g(t)g(s))α1(g(t)g(0))2 is a nondecreasing function with respect to t.

    G0(t,s)G0(1,s)=1LΓ(αν)(g(t)g(0))2(g(1)g(s))αν1(g(1)g(s))α11Γ(α)(g(t)g(s))α11LΓ(αν)(g(1)g(0))2(g(1)g(s))αν1(g(1)g(s))α11Γ(α)(g(1)g(s))α1=(g(t)g(0))2[1LΓ(αν)(g(1)g(s))αν1(g(1)g(s))α11Γ(α)(g(t)g(s))α1(g(t)g(0))2](g(1)g(0))2[1LΓ(αν)(g(1)g(s))αν1(g(1)g(s))α11Γ(α)(g(1)g(s))α1(g(1)g(0))2]((g(t)g(0))(g(1)g(0)))2.

    On the other hand, for 0ts1, it is easy to see that

    G0(t,s)G0(1,s)=((g(t)g(0))(g(1)g(0)))2.

    Therefore, (g(t)g(0)g(1)g(0))2G0(1,s)G0(t,s) for s, t[0,1].

    The proof is completed.

    By Lemma 2.12, the following conclusion is established obviously.

    Lemma 2.13. Under the assumption in Lemma 2.12, the function G has the following properties:

    G(t,s)0, for s, t[0,1];
    (g(t)g(0)g(1)g(0))2φ(s)G(t,s)φ(s), for s, t[0,1].

    where φ(s)=G0(1,s)+(g(1)g(0))2BLΓ(αν)10h(t)G1(t,s)g(t)dt.

    The following lemmas will be used in the proof of the main results.

    Lemma 2.14. [41] Let ΩE be a bounded open set and 0Ω. T:P¯ΩP be a completely continuous operator. If T satisfies

    xμTx, xPΩ, 0<μ1,

    then i(T,PΩ,p)=1.

    Lemma 2.15. [41] Let ΩE be a bounded open set and 0Ω. T:P¯ΩP be a completely continuous operator. If there is φP,φ0 such that T satisfies

    xTxμφ, xPΩ, μ0,

    then i(T,PΩ,p)=0.

    Lemma 2.16. [42] (Leggett-Williams theorem) Let P be a cone in a real Banach space E, Pc={xP| ||x||<c}, θ be a nonnegative continuous concave functional on P such that θ(x)||x||, for xPc; and P(θ,b,d)={xP| bθ(x), ||x||d}. Suppose that T:PcPc is completely continuous and there exist constants 0<a<b<dc such that

    (A1) {xP(θ,b,d)| θ(x)>b} and θ(Tx)>b for xP(θ,b,d);

    (A2) ||Tx||<a for xa;

    (A3) θ(Tx)>b for xP(θ,b,c) with ||Tx||>d.

    Then T has at least three fixed points x1, x2, x3 with ||x1||<a; b<θ(x2); a<||x3|| and θ(x3)<b.

    In this section, we establish the existence and multiplicity results for BVP (1.1). Let E=C[0,1], ||x||:=maxt[0,1]|x(t)| and P:={xE:x(t)0, t[0,1]}. Then (E, ||||) is a real Banach space and P is a cone on E. Hence E is an ordered Banach space and the cone P is normal. Obviously, the normal constant is N=1. Define operator T:PP as follows:

    Tx(t):=10G(t,s)f(s,x(s))g(s)ds, xP. (3.1)

    For any xP, by the continuity of G,f and g, Tx is well defined. Since f is bounded, It is easy to see that T is also bounded. By Lemma (2.11), one can easily see that the existence of solutions for BVP (1.1) is equivalent to the existence of positive fixed point of T. Therefore, we need only to find the positive fixed point of T in the following work.

    Subsequently, for simplicity and convenience, set

    M=(10φ(s)g(s)ds)1, N=(10(g(12)g(0)g(1)g(0))2φ(s)g(s)ds)1.

    Let r(S) be the spectral radius of the linear bounded operator S defined by

    (Sx)(t)=10G(t,s)x(t)g(s)ds, t[0,1], xE.

    From the Krein-Rutman theorem, we know that r(S) is positive and S has a positive eigenfunction φ1 corresponding to λ1 such that λ1S(φ1)=φ1, where λ1 is the first eigenvalue of S and λ1=(r(S))1.

    Now let's list the following assumptions satisfied throughout the paper.

    (H1) limx0+supt[0,1]f(t,x)x<λ1.

    (H2) limx+inft[0,1]f(t,x)x>λ1.

    (H3) limx0+inft[0,1]f(t,x)x>λ1.

    (H4) limx+supt[0,1]f(t,x)x<λ1.

    By the Arzela-Ascoli theorem, the following conclusion is established obviously.

    Lemma 3.1. The operator T: PP is completely continuous.

    Now we are in a position to give our main results.

    Theorem 3.2. Under the assumptions (H1) and (H2), BVP (1.1) admits at least one positive solution.

    Proof. For the sake of obtaining the desired result, we need only to prove T has at least a positive fixed point in P(B¯R1¯Br1).

    First, the assumption (H1) implies that there exist r1>0 and ε0(0,λ1) such that

    f(t,x)<(λ1ε0)x, t[0,1], x[0,r1].

    We claim that for μ(0,1],

    x(t)μTx(t), xPBr1, t[0,1]. (3.2)

    Suppose on the contrary that there exist x0PBr1, μ0(0,1] such that

    x0(t)=μ0Tx0(t), t[0,1].

    Then,

    x0(t)=μ0Tx0(t)10G(t,s)f(s,x0(s))g(s)ds<(λ1ε0)10G(t,s)x0(s)g(s)ds=(λ1ε0)Sx0(t).

    By nth iteration, we can get that

    x0(t)<(λ1ε0)Sx0(t)<(λ1ε0)2S2x0(t)<<(λ1ε0)nSnx0(t).

    From the definition of the norm , one can deduce that

    ||x0||<(λ1ε0)n||Sn||||x0||.

    It is easy to see that

    (λ1ε0)n||Sn||>1.

    Hence we have

    limnn||Sn||(λ1ε0)1.

    This is a contradiction with

    limnn||Sn||(λ1ε0)=(λ1ε0)r(S)<1,

    which means that (3.2) holds. By Lemma 2.14, we get

     i(T,PBr1,P)=1. (3.3)

    Second, the assumption (H2) implies that there exist ε1>0 and R1>0 such that

    f(t,x)>(λ1+ε1)x, t[0,1], |x|R1.

    Let ˜M=maxt[0,1],x[0,R1][f(t,x)+(λ1+ε1)x], we can see

    f(t,x)>(λ1+ε1)x˜M, t[0,1], x[0,+).

    Choose ¯R1>max{r1,R1,˜M[(λ1+ε1)SI]1M}. We claim that for μ[0,+),

    x(t)Tx(t)μφ1(t), xPB¯R1, t[0,1]. (3.4)

    Suppose on the contrary that there exist x1PB¯R1 and μ10 such that

    x1(t)Tx1(t)=μ1φ1(t), t[0,1].

    Therefore,

    x1(t)=Tx1(t)+μ1φ1(t)=10G(t,s)f(s,x1(s))g(s)ds+μ1φ1(t)>10G(t,s)[(λ1+ε1)x1(s)˜M]g(s)ds+μ1φ1(t)=(λ1+ε1)10G(t,s)x1(s)g(s)ds10G(t,s)˜Mg(s)ds+μ1φ1(t)=(λ1+ε1)Sx1(t)10G(t,s)˜Mg(s)ds+μ1φ1(t).

    Thus, we can see

    [(λ1+ε1)SI]x1(t)<10G(t,s)˜Mg(s)dsμ1φ1(t)<10G(t,s)˜Mg(s)ds.

    Since λ1+ε1>λ1, [(λ1+ε1)SI] is a positive linear operator. Hence, it has the inverse operator [(λ1+ε1)SI]1. By normality of cone P, we know

    ¯R1=x1<[(λ1+ε1)SI]110G(t,s)˜Mg(s)ds<˜M(10φ(s)g(s)ds)[(λ1+ε1)SI]1=˜M[(λ1+ε1)SI]1M<¯R1.

    This is a contradiction, which implies that (3.4) hold. By Lemma 2.15, one can get that

    i(T,PB¯R1,P)=0. (3.5)

    Together with (3.3) and according to the regional additivity of the fixed point index, we have

    i(T,P(B¯R1¯Br1),P)=01=1. (3.6)

    The proof is completed.

    Theorem 3.3. Under the assumptions (H3) and (H4), BVP (1.1) admits at least one positive solution.

    Proof. For the sake of obtaining the desired result, we need only to prove that T has a positive fixed point in P(B¯R2¯Br2).

    First, the assumption (H3) implies that there exist ε2>0 and r2>0 such that

    f(t,x)>(λ1+ε2)x, t[0,1], x[0,r2]. (3.7)

    Now we claim that for μ[0,+),

    x(t)Tx(t)μφ1(t), xPBr2, t[0,1]. (3.8)

    Hence, suppose on the contrary that there exist x2PBr2 and μ20 such that

    x2(t)Tx2(t)=μ2φ1(t), t[0,1].

    Without loss of generality, suppose μ2>0. Then,

    x2(t)=Tx2(t)+μ2φ1(t)μ2φ1(t).

    Taking μ=sup{μ | x2μφ1, μ>0}, we have 0<μ2μ<+ and x2(t)μφ1(t). By the positivity of operator S, we know

    λ1Sx2λ1S(μφ1)=μφ1.

    This together with (3.7) guarantees that

    x2(t)=Tx2(t)+μ2φ1(t)=10G(t,s)f(s,x2(s))g(s)ds+μ2φ1(t)>(λ1+ε2)10G(t,s)x2(s)g(s)ds+μ2φ1(t)=(λ1+ε2)Sx2(t)+μ2φ1(t)>(μ+μ2)φ1(t),

    which is a contradiction with the definition of μ. Therefore, (3.8) is valid. According to Lemma 2.15, we have

    i(T,PBr2,P)=0. (3.9)

    Second, the assumption (H4) implies that there exist ε3(0,λ1) and R2>0 such that

    f(t,x)<(λ1ε3)x, t[0,1], |x|>R2.

    Let ˜N=maxt[0,1],x[0,R2][f(t,x)+(λ1ε3)x], we can see

    f(t,x)<(λ1ε3)x+˜N, t[0,1], x[0,+).

    Choose ¯R2>max{r2,R2,˜N[1(λ1ε3)S]1M}. We claim that for μ(0,1],

    x(t)μTx(t), xPB¯R2, t[0,1]. (3.10)

    If it is not true, there exist x3PB¯R2 and μ3(0,1] such that

    x3(t)=μ3Tx3(t), t[0,1].

    Then,

    x3(t)=μ3Tx3(t)10G(t,s)f(s,x3(s))g(s)ds<10G(t,s)[(λ1ε3)x3(s)+˜N]g(s)ds=(λ1ε3)Sx3(t)+10˜NG(t,s)g(s)ds,

    which means

    [I(λ1ε3)S]x3(t)<˜N10φ(s)g(s)ds.

    Because of 0<||(λ1ε3)S||<1, [I(λ1ε3)S] has the bounded and inverse operator [I(λ1ε3)S]1 and

    [I(λ1ε3)S]1=n=0[(λ1ε3)S]n.

    By normality of cone P, we have

    ¯R2=||x3||<||[I(λ1ε3)S]110φ(s)˜Ng(s)ds||˜N||[I(λ1ε3)S]1||10φ(s)g(s)ds˜N[1(λ1ε3)S]1M<¯R2.

    This is a contraction, which means that (3.10) is valid. By Lemma 2.14,

    i(T,PB¯R2,P)=1. (3.11)

    It together with (3.9) and the regional additivity of the fixed point index guarantees that

    i(T,P(B¯R2¯Br2),P)=10=1. (3.12)

    The proof is completed.

    Now we are in a position to give the multiple solutions for BVP (1.1).

    Theorem 3.4. Assume that (H2) and (H3) hold. In addition, suppose that there exists R>0 such that

    f(t,x)<MR, x[0,R], t[0,1].

    Then BVP (1.1) has at least two positive solutions.

    Proof. For the sake of obtaining our conclusion, we first claim that for μ(0,1],

    x(t)μTx(t), xPBR, t[0,1]. (3.13)

    Suppose on the contrary that there exist x4PBR and μ4(0,1] such that

    x4(t)=μ4Tx4(t), t[0,1]. (3.14)

    Then,

    x4(t)=μ4Tx4(t)10G(t,s)f(s,x4(s))g(s)ds<10φ(s)MRg(s)ds=R.

    This is a contradiction, which means that (3.13) is valid. By Lemma 2.14, we have

    i(T,PBR,P)=1. (3.15)

    Next, similar to the process of proving (3.3) and (3.8), there exist r(0,R) and ˜Rmax{R,¯R1} such that (3.4) and (3.9) hold.

    Together with (3.15), Lemma 2.14 and Lemma 2.15, one can immediately obtain that

    i(T,P(B˜R¯BR),P)=i(T,PB˜R,P)i(T,PBR,P)=01=1,
    i(T,(PBR¯Br),P)=i(T,PBR,P)i(T,PBr,P)=10=1.

    Namely, there exist x1P(B˜R¯BR) and x2P(BR¯Br) satisfying Txi=xi(i=1,2).

    To sum up, Theorem 3.4 is proved.

    Now we are in a position to give at least three solutions for BVP (1.1).

    Theorem 3.5. Assume that there exist positive constants a, b, c with 0<a<b<c such that

    (H5) f(t,x)<Ma,(t,x)[0,1]×[0,a];

    (H6) f(t,x)>Nb,(t,x)[12,1]×[b,c];

    (H7) f(t,x)Mc,(t,x)[0,1]×[0,c].

    Then BVP(1.1) has at least three nonnegative solutions x1,x2,x3 satisfying ||x1||<a; b<mint[12,1]|x2(t)|<x2c, a<x3c and mint[12,1]|x3(t)|b.

    Proof. We shall prove assumptions of Lemma 2.16 are valid.

    Let θ(x)=mint[12,1]|x(t)|. Hence, θ(x) is a nonnegative continuous concave functional on P.

    First, we prove T:PcPc is completely continuous. In fact, for x¯Pc, from (H7) and Lemma 2.16, one can deduce that

    Tx=maxt[0,1]|10G(t,s)f(s,x(s))g(s)ds|10φ(s)f(s,x(s))g(s)dsMc10φ(s)g(s)ds=c.

    Thus, T:¯Pc¯Pc. In addition, by the continuity of G, f and g, we can conclude that T:PcPc is completely continuous.

    Let x(t)=b+c2 for t[0,1], it is not difficult to see

    x(t)=b+c2P(θ,b,c), θ(x)=θ(b+c2)>b.

    This means {xP(θ,b,c)| θ(x)>b}. By condition (H6), for xP(θ,b,c), we have

    θ(Tx)=mint[12,1]|(Tx)(t)|=mint[12,1]|10G(t,s)f(s,x(s))g(s)ds|>10(g(12)g(0)g(1)g(0))2φ(s)Nbg(s)ds=b,

    which means that (A1) in Lemma (2.16) is valid.

    By similar analysis, by (H5), one can see that

    Tx<a, x¯Pa.

    That is, (A2) in Lemma (2.16) holds. Taking c=d, (A3) is valid obviously.

    To sum up, all assumptions of Lemma 2.16 are valid. Therefore, BVP (1.1) has at least three nontrivial solutions x1, x2, x3 satisfying ||x1||<a; b<mint[12,1]|x(t)|<x2c, a<x3c and mint[12,1]|x(t)|b.

    In this section, we shall give the criteria of Ulam stability for BVP (1.1). First, let us list the following assumption.

    (H8) For all x,yR+, there exists a positive constant 0<L<M such that

    |f(t,x)f(t,y)|L|xy|, t[0,1].

    Next, for some ϵ>0, consider the following differential inequalities

    |C0Dαgx(t)f(t,x(t))|ϵ, t[0,1]. (4.1)

    Definition 4.1. [17] BVP (1.1) is Ulam-Hyers stable if there exists a real number Cf>0 such that for each ϵ>0 and for each solution xE of the inequality 4.1, there exists a solution ¯xE of BVP (1.1) with

    |x(t)¯x(t)|Cfϵ, t[0,1].

    Definition 4.2 [17] BVP (1.1) is generalized Ulam-Hyers stable if there exist ΦfC(R+,(0,+)), Φf(0)=0 such that for each solution xE of the inequality 4.1, there exists a solution ¯xE of BVP (1.1) with

    |x(t)¯x(t)|Φf(ϵ), t[0,1].

    Now, we are in a position to prove the main stable theorem of this section.

    Theorem 4.3. Under the assumptions (H1), (H4) and (H8), BVP (1.1) is Ulam-Hyers stable.

    Proof. Under the assumptions (H1) and (H4), by process similar to proving Theorems 3.2 and 3.3, BVP (1.1) has at least one positive solution.

    Let ¯xE be the solution of BVP (1.1) and xE be a solution of

    {|C0Dαgx(t)f(t,x)|ϵ, 0<t<1;x(0)=0, C0D1gx(0)=0, C0Dνgx(1)=10h(t)C0Dνgx(t)g(t)dt, (4.2)

    Then, by Lemma 2.10,

    ¯x(t)=10G(t,s)f(s,¯x(s))g(s)ds,

    and

    x(t)=10G(t,s)(f(s,x(s))+E(s))g(s)ds,

    where E(t)= C0Dαgx(t)f(t,x). By (4.2), it is easy to see |E(t)|<ϵ.

    Then,

    |x(t)¯x(t)|=|x(t)10G(t,s)f(s,¯x(s))g(s)ds||x(t)10G(t,s)f(s,x(s))g(s)ds|+|10G(t,s)f(s,x(s))g(s)ds10G(t,s)f(s,¯x(s))g(s)ds|=|10G(t,s)E(s)g(s)ds|+|10G(t,s)f(s,x(s))g(s)ds10G(t,s)f(s,¯x(s))g(s)ds|1Mϵ+L(maxt[0,1]10G(t,s)|x(s)¯x(s)|g(s)ds)=1Mϵ+LMx¯x.

    Hence,

    x¯x1MLϵ.

    Therefore, BVP (1.1) is Ulam-Hyers stable.

    In addition, set Φf(z)=Lz, then Φf(0)=0. By Definition 4.2, BVP (1.1) is generalized Ulam-Hyers stable.

    The proof is completed.

    In this section, three illustrative examples are worked out to show the effectiveness of the obtained results.

    Example 5.1. Consider the following BVP

    {C0D2.95g+f(t,x)=0, 0<t<1;x(0)=0, C0D1gx(0)=0, C0D1.05gx(1)=10h(t)C0D1.05gx(t)g(t)dt, (5.1)

    where g(t)=et2, h(t)=1 and

    f(t,x)={(1+t)(x)12, 0<x1, 0t1;(1+t)(x)2, x>1, 0t1.

    Conclusion: BVP (5.1) has at least two positive solutions.

    Proof. BVP (5.1) can be regarded as a BVP of the form (1.1).

    By careful calculation and Lemma 2.11, one can obtain that

    G(t,s)=G0(t,s)+(et21)2BLΓ(1.90)10G1(t,s)g(t)dt, L=Γ(3)Γ(1.95),
    G0(t,s)={Γ(1.95)Γ(1.9)Γ(3)(et21)2(e12es2)0.90(e121)0.951Γ(2.95)(et2es2)1.95,0st1;Γ(1.95)Γ(1.9)Γ(3)(et21)2(e12es2)0.90(e121)0.95,0ts1.
    G1(t,s)=Γ(1.95)Γ(1.9)Γ(3){(et21)0.95(e12es2)0.90(e121)0.95(et2es2)0.90,0st1;(et21)0.95(e12es2)0.90(e121)0.95,0ts1.

    By calculation, we get that

    limx0+inft[0,1]f(t,x)x=limx0+inft[0,1]x12=+>λ1,
    limx+inft[0,1]f(t,x)x=limx+inft[0,1]x=+>λ1.

    In addition, notice that M=(10φ(s)g(s)ds)111.42 and choose R=5.

    Thus,

    0f(t,x)maxt[0,1]f(t,x)2R2<MR, t[0,1], x[0,R].

    Consequently, all conditions in Theorem 3.5 hold, which means that our conclusion follows.

    Example 5.2. Consider the following BVP

    {C0D2.95g+f(t,x)=0, 0<t<1;x(0)=0, C0D1gx(0)=0, C0D1.05gx(1)=10h(t)C0D1.05gx(t)g(t)dt, (5.2)

    where g(t)=et2, h(t)=1 and

    f(t,x)={14t+x2, 0<x1, 0<t<1;500+14t+x, x>1, 0<t<1.

    Conclusion: BVP (5.2) has at least three nonnegative solutions.

    Proof. BVP (5.2) can be regarded as a BVP of the form (1.1). The function G, G0, G1 for BVP (5.2) is the same as that of BVP (5.1) in Example 5.1.

    In addition, notice that

    M=(10φ(s)g(s)ds)111.42,
    N=(10(g(12)g(0)g(1)g(0))2φ(s)g(s)ds)159.52.

    Choosing a=110, b=1, c=30, we have

    f(t,x)=14t+x20.26<Ma1.142, t[0,1], x[0,110];
    f(t,x)=300+14t+x301.12>Nb59.52, t[12,1], x[1,30];
    f(t,x)=300+14t+x330.25<Mc342.60, t[0,1], x[0,30].

    By Theorem 3.5, BVP (5.3) has at least three nonnegative solutions x1, x2, x3 with ||x1||<110; 1<mint[12,1]|x(t)|<x230; 110<x330 and mint[12,1]|x(t)|1.

    Example 5.3. Consider the following BVP

    {C0D2.95g+f(t,x)=0, 0<t<1;x(0)=0, C0D1gx(0)=0, C0Dνgx(1)=10h(t)C0D1.05gx(t)g(t)dt, (5.3)

    where g(t)=et2, h(t)=1 and f(t,x)=etln(1+x2).

    Conclusion: BVP (5.3) has at least one positive solutions and the solution of BVP (5.3) is Ulam-Hyers stable and generalized Ulam-Hyers stable.

    Proof. BVP (5.3) can be regarded as a BVP of the form (1.1). The function G, G0, G1 for BVP (5.3) is the same as that of BVP (5.1) in Example 5.1. By calculation, we get that

    limx0+supt[0,1]f(t,x)x=limx0+supt[0,1]etln(1+x2)x=+>λ1,
    limx+supt[0,1]f(t,x)x=limx+supt[0,1]etln(1+x2)x=0<λ1,

    which implies that (H1) and (H4) hold.

    In addition, notice that for all x,yR+,

    |f(t,x)f(t,y)|=et|ln(1+x2)ln(1+y2)|e|xy|.

    This means that (H8) are satisfied if we set L=e.

    Consequently, by Theorem 4.3, BVP (5.3) has at least one positive solutions and the solution of BVP (5.3) is Ulam-Hyers stable and generalized Ulam-Hyers stable.

    The proof is completed.

    The existence of solutions is of the fundamental problems for FDEs. This work studies the existence of positive solutions and multiple positive solutions for a class of FBVPs with generalized Caputo derivatives. Taking full advantage of the properties of Green's function, a suitable cone is established. The positive solutions and multiple positive solutions are obtained by means of the first eigenvalue of corresponding linear operator and the cone expansion and compression fixed point theorem. At the same time, by using Leggett-Williams theorem, we obtain that BVP (1.1) has at least three nonnegative solutions. Moreover, Ulam-Hyers stability and generalized Ulam-Hyers stability are also studied under some suitable assumptions.

    For our subsequent work, the following issues will continue to be focused on:

    (i) The systems studied on this topic will be more and more extensive and complicated. Therefore, it is valuable to investigate impulsive FDEs with generalized derivatives or hybrid FDEs with delay.

    (ii) As an important component of technology and mathematical control theory, controllability has already gained considerable attention. Hence, the controllability for fractional differential system with generalized derivatives may be an interesting issue.

    (iii) With the development of the theoretical study on FDEs, application area of FDEs with generalized derivatives in reality needs to be investigated in depth.

    The authors are thankful to the editor and anonymous referees for their valuable comments and suggestions. This research was funded by NNSF of China (62073202), Natural Science Foundation of Shandong Province (ZR2020MA007).

    The authors declare that there are no conflicts of interest.



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