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Measure of noncompactness and fractional integro-differential equations with state-dependent nonlocal conditions in Fréchet spaces

  • This paper deals with the existence of mild solutions for non-linear fractional integrodifferential equations with state-dependent nonlocal conditions. The technique used is a generalization of the classical Darbo fixed point theorem for Frechet spaces associated with the concept of measures ′ of noncompactness. An application of the main result has been included.

    Citation: Mouffak Benchohra, Zohra Bouteffal, Johnny Henderson, Sara Litimein. Measure of noncompactness and fractional integro-differential equations with state-dependent nonlocal conditions in Fréchet spaces[J]. AIMS Mathematics, 2020, 5(1): 15-25. doi: 10.3934/math.2020002

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  • This paper deals with the existence of mild solutions for non-linear fractional integrodifferential equations with state-dependent nonlocal conditions. The technique used is a generalization of the classical Darbo fixed point theorem for Frechet spaces associated with the concept of measures ′ of noncompactness. An application of the main result has been included.



    In this paper we discuss the existence of mild solutions defined on an unbounded interval for semilinear integro-differential equations of fractional order of the form

    y(t)t0(ts)α2Γ(α1)Ay(s)ds=f(t,yρ(t,yt)),   a.e.  tR+:=[0,+), (1.1)
    y0=G(σ(y),y)C:=C([r,0],E), (1.2)

    where 1<α<2 and A:D(A)EE is a closed linear operator, and (E,) is a Banach space. The convolution integral in the equation is known as the Riemann–Liouville fractional integral, f:R+×CE, σ:C([r,+),E)R+, G:R+×C([r,+),E)C and ρ:R+×CR+, are suitable functions. For any continuous function y defined on [r,+) and any t[0,+), we denote by yt the element of C defined by yt(θ)=y(t+θ) for θ[r,0].

    In this paper we discuss some existence results for fractional integro-differential equations with state dependent nonlocal conditions. Often, proposed nonlocal conditions generalize several types of nonlocal conditions studied in the literature. For the importance of nonlocal conditions in different fields we refer to [11,12] and the references therein. In [22], Hernandez and O'Regan introduced a new type of nonlocal conditions, which they called state-dependent nonlocal conditions. Recently, in [21], Hernandez studied the existence of mild and strict solutions for a class of abstract differential equations with state-dependent delay.

    The problem of existence of solutions of the Cauchy problem for fractional integro-differential equations has been studied in numerous works; we refer the reader to books by Abbas and Benchohra [1], Kilbas et al. [23], Lakshmikantham et al. [25], and to papers by Anguraj et al. [5], Balachandran et al. [7] and Benchohra and Litimein [9]. Cuevas et al. [13,14,15] studied S-asymptotically ω-periodic solutions. Recently, Wang and Chen [34] considered a class of retarded integro-differential equations with nonlocal initial conditions where existence of solutions are given over the half-line [0,). Using the nonlinear alternative of Leray–Schauder type Agarwal et al. [2] studied the existence of mild solutions to a class of fractional order integro-differential equations with state-dependent delay.

    In this paper we use a recent generalization of the classical Darbo fixed point theorem for Fréchet spaces associated with the concept of measures of noncompactness. It is well known that the measure of noncompactness provides an excellent tool for establishing the existence of solutions of nonlinear differential equations. More details are found in Abbas and Benchohra [1], Akhmerov et al. [3], [4], Banas and Goebel [8], Guo et al. [20], Olszowy [28,29,30], Olszowy and Wȩdrychowicz [31], and the references therein.

    We derive some sufficient conditions for the existence of solutions of fractional integro-differential equations with state dependent nonlocal conditions in Fréchet spaces. The concept of measure of noncompactness in Fréchet spaces is applied to achieve our results.

    The work is organized as follows. In Section 2, some preliminary facts are introduced which will be used throughout the following sections. The main results are presented in Section 3, where we prove existence of mild solutions for problems (1.1)(1.2). The last section is devoted to an illustrative example.

    Let I:=[0,T] where T>0. A measurable function y:IE is Bochner integrable if and only if y is Lebesgue integrable.

    By B(E) we denote the Banach space of bounded linear operators from E into E, with norm

    NB(E)=supy=1N(y).

    Let L1(I,E) denote the Banach space of measurable functions y:IE which are Bochner integrable normed by

    yL1=T0y(t) dt.

    Let C(I,E) be the Banach space of continuous functions from I into E with the norm

    y=sup {y(t) : tI}.

    The Laplace transformation of a function fL1(R+,E) is defined by

    L(f)(λ):=ˆf(λ):=0eλtf(t)dt,Re(λ)>ω,

    if the integral is absolutely convergent for Re(λ)>ω. In order to define the mild solution of the problems (1.1)(1.2) we recall the following definition.

    Definition 2.1. Let A be a closed and linear operator with a dense domain D(A) defined on a Banach space E. We call A the generator of a solution operator if there exists ω>0 and a strongly continuous function S:R+B(E) such that

    {λα:Re(λ)>ω}ρ(A),

    and

    λα1(λαA)1x=0eλtS(t)xdt, Reλ>ω,xE.

    In this case, S(t) is called the solution operator generated by A.

    The following result is a direct consequence of [26, Proposition 3.1 and Lemma 2.2].

    Proposition 2.2. Let {S(t)}t0B(E) be the solution operator with generator A. Then the following conditions are satisfied:

    a) S(t) is strongly continuous for t0 and S(0)=I.

    b) S(t)D(A)D(A) and AS(t)x=S(t)Ax for all xD(A), t0.

    c) For every xD(A) and t0,

    S(t)x=x+t0(ts)α1Γ(α)AS(s)xds.

    d) Let xD(A). Then t0(ts)α1Γ(α)S(s)xdsD(A) and

    S(t)x=x+At0(ts)α1Γ(α)S(s)xds.

    Remark 2.3. The concept of a solution operator, as defined above, is closely related to the concept of a resolvent family (see Prüss [33]). Because of the uniqueness of the Laplace transform, in the border case α=1, the family S(t) corresponds to a C0 semigroup (see [18]), whereas in the case α=2, a solution operator corresponds to the concept of a cosine family (see [6]).

    More information on the C0semigroups and sine families can be found in [18,19,32].

    Definition 2.4. A solution operator {S(t)}t>0 is called uniformly continuous if

    limtsS(t)S(s)B(E)=0.

    Let C(R+) be the Fréchet space of all continuous functions ν from R+ into E, equipped with the family seminorms

    νn=supt[0,n]ν(t);nN,

    and the distance

    d(u,v)=n=12nuvn1+uvn;u,vC(R+).

    We recall the following definition of the notion of a sequence of measures of noncompactness [16,17].

    Definition 2.5. Let MX be the family of all nonempty and bounded subsets of a Fréchet space X. A family of functions {μn}nN where μn:MX[0,) is said to be a family of measures of noncompactness in the real Fréchet space X if it satisfies the following conditions for all B,B1,B2MX:

    (a) {μn}nN is full; that is, μn(B)=0 for nN if and only if B is precompact,

    (b) μn(B1)μn(B2) for B1B2 and nN,

    (c) μn(ConvB)=μn(B) for nN,

    (d) If {Bi}i=1 is a sequence of closed sets from MX such that Bi+1Bi,i=1,, and if limiμn(Bi)=0, for each nN, then the intersection set B:=i=1Bi is nonempty

    Some properties:

    (e) We say the family of measures of noncompactness {μn}nN is homogenous if μn(λB)=|λ|μn(B); for λR and nN.

    (f) If the family {μn}nN satisfies the condition μn(B1+B2)μn(B1)+μn(B2), for nN, it is called subadditive.

    (g) The family {μ}nN is sublinear if both conditions (e) and (f) hold.

    (h) We say that the family of measures {μn}nN has the maximum property if

    μn(B1B2)=max{μn(B1),μn(B2)}.

    (i) The family of measures of noncompactness {μn}nN is said to be regular if and only if the conditions (a), (g) and (h) hold; (full sublinear and has the maximum property).

    Example 2.6. Let X=C(R+). For BMX,xB,nN and ε>0, let us denote by ωn(x,ε), for nN, the modulus of continuity of the function x on the interval [0,n]; that is

    ωn(x,ε)=sup{x(t)x(s)t,s[0,n],|ts|ε}.

    Further, let us put

    ωn(B,ε)=sup{ωn(x,ε):xB},
    ωn0(B)=limε0+ωn(B,ε),
    ˉαn(B)=supt[0,n]α(B(t)):=supt[0,n]α({x(t):xB}),

    and

    βn(B)=ωn0(B)+ˉαn(B).

    The family of mappings {βn}nN where βn:MX[0,), satisfies the conditions (a)(d) from Definition 2.5.

    Definition 2.7. A nonempty subset BX is said to be bounded if for nN, there exists Mn>0 such that

    ynMn,   for  each   yB.

    Lemma 2.8. [10] If Y is a bounded subset of a Banach space X, then for each ε>0 there is a sequence {yk}k=1Y such that

    μ(Y)2μ({yk}k=1)+ε,

    where μ is a Kuratowskii measure of noncompactness on X.

    Lemma 2.9. [27] If {uk}k=1L1(R+,E) is uniformly integrable, then μ({uk()}k=1) is measurable and

    μ({t0uk(s)ds}k=1)2t0μ({uk(s)}k=1)ds, t0,

    where μ is a Kuratowskii measure of noncompactness on E.

    Definition 2.10. Let Ω be a nonempty subset of a Fréchet space X, and let A:ΩX be a continuous operator which transforms bounded subsets into bounded ones. One says A satisfies the Darbo condition with constants {kn}nN with respect to a family of measures of noncompactness {μn}nN, if

    μn(A(B))knμn(B)

    for each bounded set BΩ and nN. If kn<1, nN then A is called a contraction with respect to {μn}nN.

    In the sequel we will make use of the following generalization of the classical Darbo fixed point theorem for Fréchet spaces.

    Theorem 2.11. [16,17] Let Ω be a nonempty, bounded, closed, and convex subset of a Fréchet space X and let V:ΩΩ be a continuous mapping. Suppose that V is a contraction with respect to a family of measures of noncompactness {μn}nN. Then V has at least one fixed point in the set Ω.

    In this section, we present the main results for the global existence of solutions for our problem. Let us start by defining what we mean by mild solution of the problems (1.1)(1.2).

    Definition 3.1. A function yC([r,+),E) is said to be a mild solution of (1.1)(1.2) if y0=G(σ(y),y) for all t[r,0], and y satisfies the integral equation,

    y(t)=S(t)G(σ(y),y)(0)+t0S(ts) f(s,yρ(s,ys)) ds    for each tR+. (3.1)

    Let us introduce the following hypotheses:

    (H1) There exists a constant M>1 such that

    S(t)B(E)M for every tR+.

    (H2) The function tf(t,y) is measurable on R+ for each yC, and the function yf(t,y) is continuous on C for a.e. tR+.

    (H3) There exists a function pL1loc(R+,R+) and a continuous nondecreasing function ψ:R+[0,) such that

    f(t,y)p(t) ψ(y) for a.e. tR+ and each yC.

    (H4) For each bounded set BC and for each t[0,n], nN, we have

    μ(f(t,B))p(t)supθ[r,0]μ(B(θ)),

    where μ is a measure of noncompactness on the Banach space E.

    (H5) For each nN, there exists Ln>0 such that

    G(σ(y),y)Ln(1+yn)  for each yC([r,),E).

    (H6) For each nN, there exists Kn>0 such that

    μ(G(σ(y)),B)Knsupθ[r,n]μ(B(θ)),

    for any bounded BC([r,),E).

    (H7) For each nN, there exists Rn>0 such that

    MLn(1+Rn)+Mψ(Rn)pnRn,

    where for nN,

    pn:=n0p(s)ds.

    Define on C([r,),E) the family of measures of noncompactness by

    μn(D)=ωn0(D)+supt[r,n]μ(D(t)),

    and D(t)={v(t)E;vD}, t[r,n].

    Remark 3.2. Notice that if the set D is equicontinuous, then ωn0(D)=0.

    Theorem 3.3. Assume (H1)(H7) are satisfied, and for each nN,

    2MKn+4Mpn<1.

    Then the problems (1.1)(1.2) has at least one mild solution.

    Proof. Consider the operator N:C([r,+),E)C([r,+),E) defined by

    (Ny)(t)={G(σ(y),y), if t[r,0]S(t)G(σ(y),y)(0)+t0S(ts) f(s,yρ(s,ys)) ds,if tR+. (3.2)

    Clearly, the fixed points of the operator N are solutions of the problems (1.1)(1.2). We define the ball

    BRn=B(0,Rn)={yC([r,+),E):ynRn}.

    For any nN, and each yBRn and t[0,n], by (H1)(H3),(H5) and (H7), we have

    (Ny)(t)S(t)B(E)G(σ(y),y)(0)+t0S(ts)B(E)f(s,yρ(s,ys)) dsMLn(1+yn)+Mt0p(s)ψ(yn)dsMLn(1+Rn)+Mψ(Rn)t0p(s) dsMLn(1+Rn)+Mψ(Rn)pnRn.

    Thus

    N(y)nRn.

    This proves that N transforms the ball BRn into itself.

    We shall show that the operator N:BRnBRn satisfies all the assumptions of Theorem 2.11.

    Step 1: N:BRnBRn is continuous.

    Let {yk}kN be a sequence such that yky in BRn. Then for each t[0,n], we have

    N(yk)(t)N(y)(t)=S(t)[G(σ(yk),yk)(0)G(σ(y),y)(0)]+t0 S(ts) [f(s,ykρ(s,yks))f(s,yρ(s,ys))] dsMG(σ(yk),yk)(0)G(σ(y),y)(0)+Mt0 f(s,ykρ(s,yks))f(s,yρ(s,ys)) ds.

    Since yky as k, the Lebesgue dominated convergence theorem implies that

    N(yk)N(y)n0 as k+.

    Thus N is continuous.

    Step 2: N(BRn) is bounded.

    Since N(BRn)BRn and BRn is bounded, then N(BRn) is bounded.

    Step 3: For each equicontinuous subset D of BRn,μn(N(D))lnμn(D).

    From Lemmas 2.8 and 2.9, for any equicontinuous set DBRn and any ϵ>0, there exists a sequence {yk}k=1D, such that for all t[0,n], we have

    μ((ND)(t))=μ({S(t)G(σ(y),y)(0)+t0S(ts)f(s,yρ(s,ys))ds; yD})μ({S(t)G(σ(y),y)(0),yD})+μ({t0S(ts)f(s,yρ(s,ys))ds; yD})2μ({S(t)G(σ(yk),yk)(0)}k=1)+2μ({t0S(ts)f(s,ykρ(s,yks))ds}k=1)+ϵ2μ(S(t)B(E){G(σ(yk),yk)(0)}k=1)+4t0μ(S(ts)B(E){f(s,ykρ(s,yks))}k=1)ds+ϵ2MKnsupθ[r,n]μ({yk(θ)}k=1)+4Mt0μ({f(s,ykρ(s,yks))}k=1)ds+ϵ2MKnsupθ[r,n]μ({yk(θ)}k=1)+4Mt0p(s)μ({ykρ(s,yks)}k=1)ds+ϵ2MKnμn(D)+4Mpnμn(D)+ϵ=(2MKn+4Mpn)μn(D)+ϵ.

    Since ϵ>0 is arbitrary, then

    μ((ND)(t))(2MKn+4Mpn)μn(D).

    Thus

    μn(N(D))(2MKn+4Mpn)μn(D).

    As a consequence of Steps 1 to 3, together with Theorem 2.11, we can conclude that N has at least one fixed point in BRn which is a mild solution of problems (1.1)(1.2).

    We consider the following fractional integro-differential equation with state dependent delay

    {ut(t,ξ)1Γ(μ1)t0(ts)μ2Lξu(s,ξ)ds=Q(t)|u(tη(u(t,ξ)),ξ)|, t[0,+), ξ[0,π],u0(θ,ξ)=α(uσ(u)(θ,ξ)),θ[r,0], ξ[0,π], (4.1)

    where 1<μ<2, ηC(R,[0,r]), αC(R,R), σC((C[r,+),E),[0,+)), Q is a continuous function from [0,+) to R and Lξ stands for the operator with respect to the spatial variable ξ which is given by

    Lξ=2ξ2.

    Consider E=L2([0,π],R) and the operator A:=Lξ:D(A)EE with domain

    D(A):={ uE :uE, u(0)=u(π)=0 }.

    Clearly A is densely defined in E and is sectorial. Hence A is a generator of a solution operator on E.

    Set

    y(t)(ξ)=u(t,ξ),  t[0,+), ξ[0,π].
    G(t,v)=α(vt(θ)),  t[0,+), θ[r,0].
    f(t,ϕ)(ξ)=Q(t)|u(ξ)|,  for t[0,+),  ξ[0,π],  ϕE.

    Thus, under the above definitions the problem (4.1) can be represented by the problems (1.1)(1.2). Furthermore, we can check that the assumptions of Theorem 3.3 hold. Consequently, Theorem 3.3 implies that the problem (4.1) has at least one mild solution on [r,+).

    The authors are grateful to the referees for the careful reading of the paper and for their helpful remarks.

    The authors declare no conflict of interest.



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