Research article

Mild solutions for a multi-term fractional differential equation via resolvent operators

  • Received: 10 October 2020 Accepted: 15 December 2020 Published: 18 December 2020
  • MSC : 33E12, 34A08, 45N05, 47D06, 34K30

  • This paper is concerned with multi-term fractional differential equations. With the help of the theory of fractional resolvent families, we establish the existence of mild solutions to a multi-term fractional differential equation.

    Citation: Yong-Kui Chang, Rodrigo Ponce. Mild solutions for a multi-term fractional differential equation via resolvent operators[J]. AIMS Mathematics, 2021, 6(3): 2398-2417. doi: 10.3934/math.2021146

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  • This paper is concerned with multi-term fractional differential equations. With the help of the theory of fractional resolvent families, we establish the existence of mild solutions to a multi-term fractional differential equation.



    In the last two decades, differential equations involving fractional derivatives, have been used in many mathematical models to describe a wide variety of phenomena, including problems in viscoelasticity, signal and image processing, engineering, economics, epidemiology and among others, and the study of this kind of equations has been a topic of interest in recent years. See [9,16,19,25,37,41,42,43,45] and the references therein.

    In this paper, we consider the following multi-term fractional differential equations

    αu(t)=Au(t)+αβf(t,u(t)),tR, (1.1)

    and

    αtu(t)=Au(t)+αβtf(t,u(t)),t[0,T], (1.2)

    where A is a closed linear operator defined in a Banach space X,1<α,β<2,T>0, and f is a suitable continuous function. Here, for γ>0 the derivatives γu and γtu, denote the Weyl and Caputo fractional derivatives, respectively.

    Although the definition of the fractional derivatives in the sense of Weyl (defined on R) and Caputo (defined on [0,)) are different, we notice that the mild solution to Eqs (1.1) and (1.2) can be written in terms of the same resolvent family. In fact, if A is the generator of the fractional resolvent family {Sα,1(t)}t0 (see its definition in Section 2) then the mild solutions to Eqs (1.1) and (1.2) are defined, respectively, by

    u(t)=tSα,β(ts)f(s,u(s))ds,tR,

    and

    u(t)=Sα,1(t)x+Sα,2(t)y+t0Sα,β(ts)f(s,u(s))ds,t>0,

    where x=u(0) and y=u(0) are the initial conditions in Eq (1.2), and the families {Sα,β(t)}t0, and {Sα,2(t)}t0, are given respectively by

    Sα,β(t)=(gβ1Sα,1)(t), and Sα,2(t)=(g1Sα,1)(t).

    Here, the denotes the usual finite convolution and for γ>0 the function gγ is defined by gγ(t):=tγ1/Γ(γ), where Γ() is the Gamma function. The fractional resolvent family {Sα,1(t)}t0 is defined by

    Sα,1(t):=12πiΓeλtλα1(λαA)1dλ,t0,

    where Γ is a suitable complex path where the resolvent operator (λαA)1 is well defined. By the uniqueness of the Laplace transform it is easy to see that

    Sα,2(t)=12πiΓeλtλα2(λαA)1dλ and Sα,β(t)=12πiΓeλtλαβ(λαA)1dλ,

    for all t0. The existence of mild solutions to Eq (1.1) in case β=1 has been widely studied in the last years, see for instance [4,12,13,24] and references therein. In these mentioned papers, the operator A is assumed to be an ω-sectorial operator of angle θ (see definition in Section 2). In this case, A generates a resolvent family {Eα(t)}t0 (see [11,28]) which satisfies

    Eα(t)C1+|ω|tα, for all t0,

    where C is a positive constant depending only on α and θ. This decay of {Eα(t)}t0 provides also some tools to obtain many and interesting consequences on the study of qualitative properties of solutions to fractional (and integral) differential (and difference) equations. See for instance [4,7,8,29,31,44] and the references therein for further details. We notice that, by the uniqueness of the Laplace transform, the resolvent families {Eα(t)}t0 and {Sα,1(t)}t0 are the same for 1<α<2.

    On the other hand, the existence of mild solutions to fractional differential equations with nonlocal conditions has been studied by several authors in the last years. The concept of nonlocal initial condition was introduced by L. Byszewski [6] to extend the study of classical initial value problems. This notion results more suitable to describe more precisely several phenomena in applied sciences, because it considers additional information in the initial data. More concretely, the nonlocal conditions have the form u(0)+g(u)=u0 instead u(0)=u0, where g is an appropriate function that represents the additional information in the system and provides a better description of the initial state of the system than the classical initial value problem. The theory of nonlocal Cauchy problems has been developed rapidly and has been studied widely in the last years, see for instance [3,33,38] and the references therein for more details.

    There exists a wide recent literature on the existence of mild solutions to fractional differential equations with nonlocal initial conditions. More specifically, the problem

    {αtu(t)=Au(t)+f(t,u(t)),t[0,T]u(0)+g(u)=u0, (1.3)

    where T>0,A is a closed linear operator defined in a Banach space X,0<α1,u0X,f is a suitable semilinear continuous function has been studied extensively in recent years. See for instance [1,2,10,26,30,35]. Since the fractional derivative αt for α=1 is the usual derivative ddt, the case α=1 in (1.3) corresponds precisely to the semilinear Cauchy problem introduced in the seminal paper [6] and the theory of C0-semigroups of linear operators is the main tool to obtain the existence of solutions in this case. Similarly, for α>0 the theory of fractional resolvent families represents one of the main tools to study the existence of mild solutions to (1.3). Indeed, if 0<α1 and A generates a resolvent family {Sα,α(t)}t0, then the mild solution to (1.3) is given by

    u(t)=Sα,1(u0g(u))+t0Sα,α(ts)f(s,u(s))ds (1.4)

    where Sα,1(t):=(g1αSα,α)(t), see for instance [30]. We notice that the variation of constant formula (1.4) coincides with the case α=1 introduced in [6,Section 3]. Similarly, for 1<α<2 and β=1 or β=α, the Eq (1.2) subject to the nonlocal conditions u(0)+g(u)=u0, and u(0)+h(u)=u1, where g,h:C(I,X)X are continuous and u0,u1 belong to X, (I:=[0,T]) has been considered by several authors in the last years. See for instance [2,22] for the case β=1 and [33,34] in case β=α.

    In this paper, our concern is the study of existence of mild solutions to the fractional differential Eqs (1.1) and (1.2). Here, we assume certain conditions on the operator A and on the parameters α and β in order to ensure that A is the generator of a fractional resolvent family {Sα,β(t)}t0.

    More specifically, in Eq (1.1) we consider the Weyl fractional derivative, because it is defined for functions on R. More precisely, we show that if the function f in (1.1) is an almost periodic or an almost automorphic (among others) vector-valued function, then the Eq (1.1) has a unique almost periodic or almost automorphic function mild solution, respectively, which is given in terms of {Sα,β(t)}t0.

    On the other hand, in Eq (1.2) the derivative is taken in the sense of Caputo, because it is defined on the positive real axis [0,). Under the the nonlocal conditions u(0)+g(u)=u0, and u(0)+h(u)=u1 we prove that (1.2) has at least one mild solution. Here, the properties of the fractional resolvent family {Sα,β(t)}t0 are again an important tool to obtain the result.

    This paper is organized as follows. The Section 2 gives the preliminaries on fractional calculus, sectorial operators, fractional resolvent families and some subspaces of bounded and continuous functions. Section 3 is devoted to the existence of mild solutions to (1.1). In Section 4 is studied the existence of mild solutions to the nonlocal problem (1.2). Finally, in Section 5 we give some examples.

    For a Banach space (X,), the space of all bounded and linear operators form X into X is denoted by B(X). If A is a closed linear operator defined on X we denote by ρ(A) the resolvent set of A and R(λ,A)=(λA)1 its resolvent operator, which is defined for all λρ(A). For 1p<,Lp(R+,X) denotes the space of all Bochner measurable functions g:R+X such that

    gp:=(0g(t)pdt)1/p<.

    We recall that a strongly continuous family {S(t)}t0B(X) is said to be exponentially bounded if there exist two constants M>0 and wR such that S(t)Mewt for all t>0.

    A closed and densely defined operator A, defined on a Banach space (X,), is said to be ω -sectorial of angle ϕ, if there exist ϕ[0,π/2) and ωR such that its resolvent exists in the sector ω+Σϕ:={ω+λ:λC,|arg(λ)|<π2+ϕ}{ω} and R(λ,A)M|λω| for all λω+Σϕ. See [17] and [18] for further details.

    Now, we review some results on fractional calculus. We recall that for γ>0, the function gγ is defined by gγ(t)=tγ1Γ(γ) for all t0. For γ>0,γ denotes the smallest integer greater than or equal to γ, and [γ] denotes the integer part of γ. As usual, the finite convolution of f and g is defined by (fg)(t)=t0f(ts)g(s)ds.

    Definition 1. Let α>0 and n=α. The Caputo fractional derivative of order α of a function u:[0,)X is defined by

    αtu(t):=t0gnα(ts)u(n)(s)ds.

    Definition 2. Let α>0 and n=[α]+1. The Weyl fractional derivative of order α of a function u:RX is defined by

    αu(t):=dndtn(nα)u(t),

    where for γ>0,γu(t):=tgγ(ts)u(s)ds for all tR.

    It is a well known fact that if αN, then nt=n=dndtn, that is, the Caputo and Weyl fractional derivatives coincide with the usual derivative if αN. Moreover, if α,βR, then αβu=βαu=α+βu. See [25,41] and [42] for more details and applications on fractional differential calculus.

    Now, we recall the resolvent families of operators generated by an operator A.

    Definition 3. Let A be closed linear operator with domain D(A), defined on a Banach space X,1α2 and 0<β2. We say that A is the generator of an (α,β)-resolvent family, if there exists ν0 and a strongly continuous and exponentially bounded function Sα,β:[0,)B(X) such that {λα:Reλ>ν}ρ(A), and for all xX,

    λαβ(λαA)1x=0eλtSα,β(t)xdt,Reλ>ν.

    In this case, {Sα,β(t)}t0 is called the (α,β)-resolvent family generated by A.

    If we compare Definition 3 with the notion of (a,k)-regularized families introduced in [21], then we notice that tSα,β(t), is a (gα,gβ)-regularized family. Moreover, the family {Sα,β(t)}t0 is well known in some cases. For example, S1,1(t) is a C0-semigroup, S2,1(t), corresponds to a cosine family and S2,2(t) is a sine family. In the scalar case, that is, when A=ϱI, where ϱC and I denotes the identity operator, then by the uniqueness of the Laplace transform, Sα,β(t) corresponds to the function tβ1Eα,β(ϱtα), where for zC the generalized Mittag-Leffler function is defined by Eα,β(z)=k=0zkΓ(αk+β), see for instance [39,40]. See also [41] and [42] for an interesting and recent discussion on the theory of general fractional derivatives and its applications.

    We have also the following result. Its proof follows similarly as in [20,Proposition 3.7].

    Proposition 4. Let 1α,β2. Let Sα,β(t) be the (α,β)-resolvent family generated by A. Then:

    1. Sα,β(t)xD(A) and Sα,β(t)Ax=ASα,β(t)x for all xD(A) and t0.

    2. If xD(A) and t0, then

    Sα,β(t)x=gβ(t)x+t0gα(ts)ASα,β(s)xds (2.1)

    3. If xX,t0, then t0gα(ts)Sα,β(s)xdsD(A) and Sα,β(t)x=gβ(t)x+At0gα(ts)Sα,β(s)xds.

    In particular, Sα,β(0)=gβ(0)I.

    The next result gives sufficient conditions on α,β and A to obtain generators of (α,β)-resolvent families.

    Theorem 5. [28] Let 1<α<2 and β1 such that αβ+1>0. Assume that A is ω-sectorial of angle (α1)π2, where ω<0. Then A generates an exponentially bounded (α,β)-resolvent family.

    Theorem 6. [28] Let 1<α<2 and β1 such that αβ+1>0. Assume that A is ω-sectorial of angle (α1)2π, where ω<0. Then, there exists a constant C>0, depending only on α and β, such that

    Sα,β(t)Ctβ11+|ω|tα,for allt>0. (2.2)

    Finally, we recall some spaces of functions. For a given Banach space (X,), let BC(X):={f:RX:f:=suptRf(t)<} be the Banach space of all bounded and continuous functions. For T>0 fixed, PT(X) denotes the space of all vector-valued periodic functions, that is, PT(X):={fBC(X):f(t+T)=f(t), for all tR}. We denote by AP(X) to the space of all almost periodic functions (in the sense of Bohr), which consists of all fBC(X) such that for every ε>0 there exists l>0 such that for every subinterval of R of length l contains at least one point τ such that f(t+τ)f(t)ε. A function fBC(X) is said to be almost automorphic if for every sequence of real numbers (sn)nN there exists a subsequence (sn)nN(sn)nN such that

    g(t):=limnf(t+sn)

    is well defined for each tR, and

    f(t)=limng(tsn), for each tR.

    We denote by AA(X) the Banach space of all almost automorphic functions.

    On the other hand, the space of compact almost automorphic functions is the space of all functions fBC(X) such that for all sequence (sn)nN of real numbers there exists a subsequence (sn)nN(sn)nN such that g(t):=limnf(t+sn) and f(t)=limng(tsn) uniformly over compact subsets of R.

    We notice that PT(X),AP(X),AA(X) and AAc(X) are Banach spaces under the norm |||| and

    PT(X)AP(X)AA(X)AAc(X)BC(X).

    We notice that all these inclusions are proper. Now we consider the set C0(X):={fBC(X):lim|t|||f(t)||=0}, and define the space of asymptotically periodic functions as APT(X):=PT(X)C0(X). Analogously, we define the space of asymptotically almost periodic functions,

    AAP(X):=AP(X)C0(X),

    the space of asymptotically compact almost automorphic functions,

    AAAc(X):=AAc(X)C0(X),

    and the space of asymptotically almost automorphic functions,

    AAA(X):=AA(X)C0(X).

    We have the following natural proper inclusions

    APT(X)AAP(X)AAAc(X)AAA(X)BC(X).

    For more details on this function spaces, we refer to reader to [23,27].

    Throughout, we will use the notation N(X) to denote any of the function spaces APT(X),AAP(X),AAAc(X) and AAA(X) defined above. Finally, we define the set N(R×X;X) which consists of all functions f:R×XX such that f(,x)N(X) uniformly for each xK, where K is any bounded subset of X. Moreover, we have the following result.

    Theorem 7. [23] Let {S(t)}t0B(X) be a strongly continuous and uniformly 1-integrable family, that is 0S(t)dt<. If fN(X), then the function u:RX defined by

    u(t):=tS(ts)f(s)ds,

    belongs to N(X).

    Let 1<α<2 and β1. In this section, we first consider the linear version of the Eq (1.1), that is,

    αu(t)=Au(t)+αβf(t),tR. (3.1)

    Definition 8. A function uC(R,X) is called a mild solution to Eq (3.1) if the function sSα,β(ts)f(s) is integrable on (,t) for each tR and

    u(t)=tSα,β(ts)f(s)ds,tR. (3.2)

    We notice that (3.1) can be considered as the limiting equation of the following integro-differential equation with singular kernels

    {v(t)=t0(ts)α2Γ(α1)Av(s)+(ts)β2Γ(β1)f(s)ds,t0v(0)=v0,v0X, (3.3)

    in the sense that the mild solution to Eq (3.3) converges to the mild solution of (3.1) as t. In fact, if ω<0 and A is an ω-sectorial operator of angle θ=(α1)2π, then taking Laplace transform in (3.3) we obtain

    λˆv(λ)v(0)=1λα1Aˆv(λ)+1λβ1ˆf(λ),Reλ>0,

    which is equivalent to

    (λαA)ˆv(λ)=λα1v(0)+λαβˆf(λ),Reλ>0.

    Therefore the solution of problem (3.3) can be written as

    v(t)=Sα,1(t)v0+t0Sα,β(ts)f(s)ds,t0, (3.4)

    where {Sα,β(t)}t0 is the family of operators given by

    Sα,β(t):=(gβ1Sα,1)(t).

    On the other hand, by [28,Corollary 3.9] the function tSα,β(t) is uniformly 1-integrable and therefore if f is a bounded continuous function (for example, if f belongs to N(X)), then the mild solution to Eq (1.1) is given by

    u(t)=tSα,β(ts)f(s)ds.

    Since

    v(t)u(t)=Sα,1(t)v0tSα,β(s)f(ts)ds,

    we conclude by [28,Corollary 3.8], that v(t)u(t)0 as t.

    Let 1<α<2,β1 such that αβ+1>0, ω<0 and assume that A is an ω-sectorial operator of angle θ=(α1)2π. By Theorem 5, the operator A generates a resolvent family {Sα,β(t)}t0. Take a bounded and continuous function f:RX, (for example, we can take fN(X)). Define the function ϕ(t) by

    ϕ(t):=tSα,β(ts)f(s)ds,tR. (3.5)

    By Theorem 6 we have ||ϕ||||Sα,β||1||f||. If f(t)D(A) for all tR, then ϕ(t)D(A) for all tR (see [5,Proposition 1.1.7]). Assume that αϕ exists. The Proposition 4 and Fubini's theorem imply that

    αϕ(t)=dndtntgnα(ts)ϕ(s)ds=dndtntgnα(ts)sSα,β(sr)f(r)drds=dndtntgnα(ts)s[gβ(sr)f(r)+(gαASα,β)(sr)f(r)]drds=dndtntgnα(ts)βf(s)ds+dndtntgnα(ts)ssr0gα(srv)ASα,β(v)f(r)dvdrds=αβf(t)+dndtntgnα(ts)ssrgα(sw)ASα,β(wr)f(r)dwdrds=αβf(t)+dndtntgnα(ts)swgα(sw)ASα,β(wr)f(r)drdwds=αβf(t)+dndtntgnα(ts)sgα(sw)Aϕ(w)dwds=αβf(t)+Aϕ(t),

    for all tR. This means that, ϕ is a (strong) solution to Eq (3.1). We recall that a function uC(R,X) is called a strong solution of (3.1) on R if uC(R,D(A)), the fractional derivative of u,αu, exists and (3.1) holds for all tR. If merely u(t) belongs to X instead of the D(A), then u is a mild solution to the Eq (3.1) according to Definition 8. As consequence of the above computation we have the following result.

    Theorem 9. Let 1β<α<2 and ω<0. Assume that A is an ω-sectorial operator of angle θ=(α1)2π. Then for each fN(X) there is a unique mild solution uN(X) of Eq (3.1) which is given by

    u(t)=tSα,β(ts)f(s)ds,tR.

    Proof. By Theorem 5, the operator A generates a resolvent family {Sα,β(t)}t0 and by [28,Corollary 3.9] the function tSα,β(t) is uniformly 1-integrable. By Theorem 7 the function u(t)=tSα,β(ts)f(s)ds belongs to N(X) and it is the mild solution to (3.1).

    Next, we consider the semilinear Eq (1.1).

    Definition 10. A function uC(R,X) is called a mild solution to Eq (1.1) if the function sSα,β(ts)f(s,u(s)) is integrable on (,t) for each tR and

    u(t)=tSα,β(ts)f(s,u(s))ds,tR. (3.6)

    Theorem 11. Let 1β<α<2,ω<0 and A is an ω-sectorial operator of angle θ=(α1)2π. If fN(R×X,X) satisfies

    f(t,u)f(t,v)Luv,for alltR,andu,vX, (3.7)

    where L<αC|ω|β/αB(βα,1βα)1, and C is the constant given in Theorem 6, and B(,) denotes the Beta function, then the Eq (1.1) has a unique mild solution uN(X).

    Proof. Define the operator F:N(X)N(X) by

    (Fϕ)(t):=tSα,β(ts)f(s,ϕ(s))ds,tR. (3.8)

    By [28,Corollary 3.9] we have

    0Sα,β(t)dtCα|ω|β/αB(βα,1βα)<, (3.9)

    and [23,Theorems 3.3 and 4.1], F is well defined, that is, FϕN(X) for all ϕN(X). For ϕ1,ϕ2N(X) and tR, by (3.9), we have:

    (Fϕ1)(t)(Fϕ2)(t)tSα,β(ts)[f(s,ϕ1(s))f(s,ϕ2(s))]dstLSα,β(ts)ϕ1(s)ϕ2(s)dsLϕ1ϕ20Sα,β(r)drLCα|ω|β/αB(βα,1βα)ϕ1ϕ2.

    This proves that F is a contraction, so by the Banach fixed point theorem there exists a unique uN(X) such that Fu=u.

    Theorem 12. Let 1β<α<2,ω<0 and A is an ω-sectorial operator of angle θ=(α1)2π. If fN(R×X,X) satisfies

    f(t,u)f(t,v)L(t)uv,for alltR,andu,vX,

    where L()L1(R,R+), then the Eq (1.1) admits a unique mild solution uN(X).

    Proof. It easily follows by Theorem 6 that Sα,β(t)˜C:=max{C,C|ω|}. Define the operator F as (3.8). For u,vN(X) and tR, we have

    ||(Fu)(t)(Fv)(t)||t||Sα,β(ts)[f(s,u(s))f(s,v(s))]||ds˜Cuv0L(tξ)dξ=˜CuvtL(s)ds.

    Generally, we have

    (Fnu)(t)(Fnv)(t)uv(˜C)n(n1)!(tL(s)(sL(ξ)dξ)n1ds)uv(˜C)nn!(tL(s)ds)nuv(L1˜C)nn!.

    Since (L1˜C)nn!<1 for sufficiently large n, by the contraction principle F admits a unique fixed point uN(X).

    Assume that A is an ω-sectorial operator of angle θ=(α1)2π. By Theorem 5 the operator A generates a resolvent family {Sα,β(t)}t0. If h:C(I,X)X is a continuous function, f(0,u(0))=0 and u1X, then it is well known that the mild solution to problem

    {αtu(t)=Au(t)+αβtf(t,u(t)),0tTu(0)=0,u(0)+h(u)=u1, (4.1)

    is given by means of the variation-of-constant formula

    u(t)=Sα,2(t)[u1h(u)]+t0Sα,β(ts)f(s,u(s))ds,t[0,T].

    We assume the following

    H1. The function f satisfies the Carathéodory condition, that is f(,u) is strongly measurable for each uX and f(t,) is continuous for each tI:=[0,T].

    H2. There exists a continuous function μ:IR+ such that

    f(t,u)μ(t)u,tI,uC(I,X)

    and f(0,u(0))=0.

    H3. The function h:C(I,X)X is continuous and there exists Lh>0 such that

    h(u)h(v)<Lhuv,u,vC(I,X).

    H4. The set K={Sα,β(ts)f(s,u(s)):uC(I,X),0st} is relatively compact for each tI.

    Proposition 13. Let 1<α<2 and 1<β2 such that αβ+1>0. If A is an ω-sectorial operator of angle θ=(α1)2π, where ω<0, then the function tSα,β(t) is continuous in B(X) for all t>0.

    Proof. It proof follows similarly to [30,Proposition 11]. We omit the details.

    We recall the following results.

    Lemma 14 (Mazur's Theorem). If K is a compact subset of a Banach space X, then its convex closure ¯conv(K) is compact.

    Lemma 15 (Leray-Schauder Alternative Theorem). Let C be a convex subset of a Banach space X. Suppose that 0C. If F:CC is a completely continuous map, then either F has a fixed point, or the set {xC:x=λF(x),0<λ<1} is unbounded.

    Lemma 16 (Krasnoselskii Theorem). Let C be a closed convex and nonempty subset of a Banach space X. Let Q1 and Q2 be two operators such that

    i) If u,vC, then Q1u+Q2vC.

    ii) Q1 is a mapping contraction.

    iii) Q2 is compact and continuous.

    Then, there exists zC such that z=Q1z+Q2z.

    We have the following existence theorem.

    Theorem 17. Let 1<α<2 and 1<β<2 such that αβ+1>0. Assume that A is an ω-sectorial operator of angle θ=(α1)2π, where ω<0. Under assumptions H1-H4, the problem (4.1) has at least one mild solution.

    Proof. By Theorem 5, the operator A generates a resolvent family {Sα,1(t)}t0. By the uniqueness of the Laplace transform we have Sα,2(t)=(g1Sα,1)(t) and Sα,β(t)=(gβ1Sα,1)(t) for all t0. Moreover, by Theorem 6 there exists a constant M>0 such that Sα,2(t)M and Sα,β(t)M for all t0. Now, we define the operator Γ:C(I,X)C(I,X) by

    (Γu)(t):=Sα,2(t)[u1h(u)]+t0Sα,β(ts)f(s,u(s))ds,t[0,T].

    Let Br:={uC(I,X):ur}, where r>0. We shall prove that Γ has at least one fixed point by the Leray-Schauder fixed point theorem. We will consider several steps in the proof.

    Step 1. The operator Γ sends bounded sets of C(I,X) into bounded sets of C(I,X). In fact, take uBr and G:=supuBrh(u). Then

    Γu(t)Sα,2(t)(u1+h(u))+t0Sα,β(ts)f(s,u(s))dsM(u1+G)+Mt0μ(s)u(s)dsM(u1+G)+Mrt0μ(s)dsM(u1+G)+MrμT:=R.

    Therefore ΓBrBR.

    Step 2. Γ is a continuous operator.

    Let un,uBr such that unu in C(I,X). Then we have

    Γun(t)Γu(t)Sα,2(t)(h(un)h(u))+t0Sα,β(ts)f(s,un(s))f(s,u(s))dsMLhunu+Mt0f(s,un(s))f(s,u(s))dsMLhunu+Mt0μ(s)(un(s)+u(s))dsMLhunu+2rMt0μ(s)ds.

    We notice that the function sμ(s) is integrable on I. By the Lebesgue's Dominated Convergence Theorem, t0f(s,un(s))f(s,u(s))ds0 as n. Since unu we obtain that Γ is continuous in C(I,X).

    Step 3 The operator Γ sends bounded sets of C(I,X) into equicontinuous sets of C(I,X).

    In fact, let uBr, with r>0 and take t1,t2I with t2<t1. Then we have

    Γu(t1)Γu(t2)(Sα,2(t1)Sα,2(t2))(u1h(u))+t1t2Sα,β(t1s)f(s,u(s))ds+t20(Sα,β(t1s)Sα,β(t2s))f(s,u(s))ds:=I1+I2+I3.

    Observe that

    I1(Sα,2(t1)Sα,2(t2))(u1h(u)).

    Using the norm continuity of tSα,2(t) (see Proposition 13) we obtain that limt1t2I1=0.

    On the other hand,

    I2Mt1t2μ(s)u(s)dsrMμ(t1t2),

    and therefore limt1t2I2=0. Finally, for I3 we have

    I3t20Sα,β(t1s)Sα,β(t2s)f(s,u(s))dst20Sα,β(t1s)Sα,β(t2s)μ(s)u(s)dsrt20Sα,β(t1s)Sα,β(t2s)μ(s)ds.

    Since

    Sα,β(t1)Sα,β(t2)μ()2Mμ()L1(I,R),

    and Sα,β(t1s)Sα,β(t2s)0 in B(X), as t1t2 (see Proposition 13) we obtain by the Lebesgue's dominated convergence theorem that limt1t2I3=0. The proof of the claim is finished.

    Step 4. The function Γ maps Br into relatively compact sets in X.

    The hypothesis and Lemma 14 imply that ¯conv(K) is compact. Moreover, for uBr, by the Mean-Value Theorem for the Bochner integral (see [15,Corollary 8,p. 48]), we get

    Γ(u(t))t¯conv(K),

    for all t[0,T]. Thus the set ¯{Γu(t);uBr} is compact in X for every t[0,T].

    We conclude from Steps 1–4, that Γ is continuous and compact by the Arzela-Ascoli's theorem, which means that the function Γ is completely continuous.

    Step 5. The set Ω:={uBr:u=λΓu,0<λ<1} is bounded. In fact, since 0Ω we obtain that Ω. For uΩ we have

    u(t)λ[M(u1+h(u))+Mt0f(s,u(s)ds]λ[M(u1+G)+Mt0μ(s)u(s)ds][M(u1+G)+MrμT],

    for all t[0,T], which means that Ω is a bounded set.

    Therefore, by Lemma 15 we conclude that Γ has a fixed point, and the proof of the Theorem is finished.

    The same method of proof can be used to prove the next result. We omit the details.

    Theorem 18. Let 1<α<2. Assume that A generates the resolvent family {Sα,1(t)}t0. Under assumptions H1–H4, the problem (4.1) has at least one mild solution.

    Now, we consider the problem

    {αtu(t)=Au(t)+αβtf(t,u(t)),0tTu(0)+g(u)=u0,u(0)+h(u)=u1, (4.2)

    where g,h:C(I,X)X are continuous, f(0,u(0))=0 and u0,u1X. By (2.2) in Theorem 6, there exists a constant M>0 such that

    Sα,1(t)M1+|ω|tα,Sα,2(t)Mt1+|ω|tα,Sα,β(t)Mtβ11+|ω|tα,t0. (4.3)

    Thus

    Sα,1(t)M,Sα,2(t)MT,Sα,β(t)MTβ1,t[0,T]. (4.4)

    Under the same assumptions H1–H3 and

    H3'. The function g:C(I,X)X is continuous and there exists Lg>0 such that

    g(u)g(v)<Lguv,u,vC(I,X).

    we have the following result.

    Theorem 19. Let 1<α<2 and 1<β<2 such that αβ+1>0. Assume that A is an ω-sectorial operator of angle θ=(α1)2π, where ω<0. Suppose that MμTβ<1 and M(Lg+TLh)<1, where M is the constant in (4.4). Assume that (λαA)1 is compact for all λ>ν1/α, where ν is a positive constant. Under assumptions H1–H3 and H3', the problem (4.2) has at least one mild solution.

    Proof. By Theorem 5, the operator A generates the resolvent family {Sα,1(t)}t0, and Sα,2(t)=(g1Sα,1)(t) and Sα,β(t)=(gβ1Sα,1)(t) for all t0. Then, the mild solution to problem (4.2) is given by

    u(t)=Sα,1(t)[u0g(u)]+Sα,2(t)[u1h(u)]+t0Sα,β(ts)f(s,u(s))ds,t[0,T].

    Let Br:={uC(I,X):ur}, where

    r:=M(u0+g(u))+MT(u1+h(u))1MμTβ.

    On Br we define the operators Γ1,Γ2 by

    (Γ1u)(t):=Sα,1(t)[u0g(u)]+Sα,2(t)(u1h(u))t[0,T](Γ2u)(t):=t0Sα,β(ts)f(s,u(s))ds,t[0,T],

    where uBr. We claim that Γ:=Γ1+Γ2 has at least one fixed. To prove this, we will consider several steps.

    Step 1. We claim that if u,vBr, then Γ1u+Γ2vBr. In fact,

    (Γ1u)(t)+(Γ2v)(t)
    Sα,1(t)u0g(u)+Sα,2(t)u1h(u)+t0Sα,β(ts)f(s,v(s))dsM(u0+g(u))+MT(u1+h(u))+Mt0(ts)β1μ(s)v(s)dsM(u0+g(u))+MT(u1+h(u))+MTβμr=r.

    Thus Γ1u+Γ2vBr for all u,vBr.

    Step 2. Γ1 is a contraction on Br. In fact, if u,vBr, then

    Γ1u(t)Γ1v(t)Sα,1(t)g(u)g(v)+Sα,2(t)h(u)h(v)(MLg+MTLh)uv

    Since M(Lg+TLh)<1, we get that Γ1 is a contraction.

    Step 3. Γ2 is completely continuous.

    Firstly, we prove that Γ2 is a continuous operator on Br. Let un,uBr such that unu in Br. We notice that by (4.3)

    Γ2un(t)Γ2u(t)t0Sα,β(ts)f(s,un(s))f(s,u(s))ds2MrTβt0μ(s)ds.

    Moreover, the function sμ(s) is integrable on [0,T]. The Lebesgue's Dominated Convergence Theorem implies that t0f(s,un(s))f(s,u(s))ds0 as n. Since unu we obtain that Γ2 is continuous in Br.

    Now, we prove that {Γ2u:uBr} is a relatively compact set. In fact, by the Ascoli-Arzela theorem we only need to prove that the family {Γ2u:uBr} is uniformly bounded and equicontinuous, and the set {Γ2u(t):uBr} is relatively compact in X for each t[0,T]. For each uBr we have Γ2uMTβrμ, which implies that {Γ2u:uBr} is uniformly bounded.

    Next, we prove the equicontinuity. For uBr and 0t2<t1T we have

    Γ2u(t1)Γ2u(t2)t1t2Sα,β(t1s)f(s,u(s))ds+t20(Sα,β(t1s)Sα,β(t2s))f(s,u(s))ds=:I1+I2.

    Observe that for I1, by (4.3) we have I1MTβt1t2μ(s)u(s)dsMTβrμ(t1t2), and thus limt1t2I1=0. On the other hand, for I2 we have

    I2t20Sα,β(t1s)Sα,β(t2s)f(s,u(s))dsrt20μ(s)Sα,β(t1s)Sα,β(t2s)ds.

    By (4.4) we have μ()Sα,β(t1)Sα,β(t2)2Tβ1Mμ()L1([0,T],R), and by Proposition 13 the function tSα,β(t) is norm continuous. This implies that if t1t2, then Sα,β)(t1s)Sα,β)(t2s)0 in B(X). By the Lebesgue's dominated convergence theorem we conclude that limt1t2I2=0. Therefore, {Γ2u:uBr} is an equicontinuous family.

    Finally, we prove that H(t):={Γ2u(t):uBr} is relatively compact in X for each t[0,T]. Clearly, H(0) is relatively compact in X. Now, we take t>0. For 0<ε<t we define on Br the operator

    (Γε2u)(t):=tε0Sα,β(ts)f(s,u(s))ds.

    By [30,Theorem 14] we have that Sα,β(t) is a compact operator for all t>0. Thus Kε:={Sα,β(ts)f(s,u(s)):uBr,0stε} is a compact set for all ε>0. By Lemma 14, ¯conv(Kε) is also a compact set. The Mean-Value Theorem for the Bochner integrals (see [15,Corollary 8,p. 48]), implies that (Γε2u)(t)t¯conv(Kε), for all t[0,T]. Therefore, the set Hε(t):={(Γε2u)(t):uBr} is relatively compact in X for all ε>0. Since

    (Γ2u)(t)(Γε2u)(t)ttεSα,β(ts)f(s,u(s))dsMTβ1rttεμ(s)ds

    and the function sμ(s) belongs to L1([tε,t],R+) we conclude by the Lebesgue dominated convergence Theorem that limε0(Γ2u)(t)(Γε2u)(t)=0. Therefore the set {Γ2u(t):uBr} is relatively compact in X for each t(0,T]. The Ascoli-Arzela theorem implies that the set {Γ2u:uBr} is relatively compact. We conclude that Γ2 is a completely continuous operator. By Lemma 16 we have that Γ=Γ1+Γ2 has a fixed point on Br, and therefore the problem (4.2) has a mild solution.

    Example 20.

    On the Banach space X=C, let A be the scalar operator A=ϱI, where ϱR. Consider the multi-term fractional differential equation

    αu(t)=Au(t)+αβf(t),tR, (5.1)

    where 1β<α<2 and f(t) is the almost periodic function f(t)=sin(t)+sin(2t), see [14,p. 80]. By Theorem 9 the solution u to (5.1) is an almost periodic function, and it is given by

    u(t)=tSα,β(ts)f(s)ds,tR.

    where Sα,β(t)=tβ1Eα,β(ϱtα). By Theorem 6, we can write

    u(t)=tSα,β(ts)f(s)ds=k=0ϱkt(ts)αk+β1Γ(αk+β)f(s)ds.

    Now, we notice that if g(t)=eμt, where μC and δ>0, then

    1Γ(δ)t(ts)δ1g(s)ds=μ1δΓ(δ)t[μ(ts)δ1]eμsds=μδΓ(δ)eμt0rδ1erdr=μδeμt,

    and therefore, for h(t)=sin(at)=eaiteait2i, where a>0, we have

    1Γ(δ)t(ts)δ1h(s)ds=aδsin(atπ2δ).

    This implies that

    u(t)=k=0ϱk[sin(tπ2(αk+β))+12αk+βsin(2tπ2(αk+β))].

    In Figure 1, we have the solution u for (5.1) for ϱ=1 and α=1.5,β=1.3 on the interval [30,30].

    Figure 1.  Solution u(t) for (5.1) on the interval [30,30].

    Example 21.

    Consider the following partial differential equation with fractional temporal derivatives

    {αtu(t,x)=2x2u(t,x)+αβtsin(u(t,x)),(t,x)[0,T]×Ru(0,x)=0,xRu(0,x)+ni=1ciu(ti,x)=u1(x),xR (5.2)

    where 1<α,β<2,0t1<...<tnT,u1L2(R), and ci are real constants.

    On the Banach space X=L2(R), let A be the second order operator Av=v with domain D(A)=W2,2(R). By [36,Example 1.2.2,p. 3063], A generates a cosine family {S2,1(t)}tR on X, and by the Subordination Principle [32,Corollary 3.3], A is the generator of the resolvent family {Sα,1(t)}t0 given by

    Sα,1(t)x:=0ψα2,1α2(t,s)S2,1(s)xds,t0,xX, (5.3)

    where ψα2,1α2 is the Wright type function defined by

    ψα2,1α2(t,s)=1π0ρα21esρα2cosα2(πθ)tρcosθ×sin(tρsinθsρα2sinα2(πθ)+α2(πθ))dρ,

    for θ(π2α,π/2). Define,

    u(t)x=u(t,x)f(t,u(t))(x)=sin(u(t,x))h(u)(x)=ni=1ciu(ti,x).

    Then, (5.2) can be reformulated as the abstract problem (4.1). Moreover, an easy computation shows that the hypotheses H1H3 hold with μ(t)=1 and Lh=ni=1|ci|. Since

    Sα,β(t)=(gβ1Sα,1)(t),

    we obtain by (2.2) that the set K={Sα,β(ts)sin(s,u(s)):uC(I,X),0st} is relatively compact for each tI, and therefore H4 holds. We conclude, by Theorem 18, that the problem (4.1) has at least one mild solution u.

    In this paper, some sufficient conditions are established for the existence of mild and bounded solutions to a multi-term fractional differential equation. Under the theory of fractional resolvent families in Banach spaces, the mild solutions are given in term of these operator families. The main results are given for the Caputo and Weyl fractional derivatives.

    The authors thank the anonymous referees for reading the manuscript and for making suggestions that have improved the previous version of this paper. This work was partially supported by NSF of Shaanxi Province (2020JM-183).

    The authors declare no conflict of interest.



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    沈阳化工大学材料科学与工程学院 沈阳 110142

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