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Research article

A study on controllability for Hilfer fractional differential equations with impulsive delay conditions

  • Received: 25 September 2022 Revised: 09 November 2022 Accepted: 13 November 2022 Published: 02 December 2022
  • MSC : 93B05, 34K30, 34K40, 47H08, 47H10

  • This article focuses on the controllability of a Hilfer fractional impulsive differential equation with indefinite delay. We analyze our major outcomes using fractional calculus, the measure of non-compactness and a fixed-point approach. Finally, an example is provided to show the theory.

    Citation: Kulandhaivel Karthikeyan, Palanisamy Raja Sekar, Panjaiyan Karthikeyan, Anoop Kumar, Thongchai Botmart, Wajaree Weera. A study on controllability for Hilfer fractional differential equations with impulsive delay conditions[J]. AIMS Mathematics, 2023, 8(2): 4202-4219. doi: 10.3934/math.2023209

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  • This article focuses on the controllability of a Hilfer fractional impulsive differential equation with indefinite delay. We analyze our major outcomes using fractional calculus, the measure of non-compactness and a fixed-point approach. Finally, an example is provided to show the theory.



    Fractional calculus and its potential applications have grown in importance because fractional calculus has evolved into a powerful tool with more accurate and successful results in modeling various complex phenomena in a wide range of seemingly diverse and widespread fields of science and engineering. This technology could be used in physics, signal processing, wave propagation, robotics, and other fields [1,2,3,4,5,6,7,8] and there are research papers on the theory of fractional differential equations [9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38].

    The evolution of a physical system in time is described by an initial and boundary value problem, i.e., a differential equation (ordinary or partial) and an initial or boundary condition. In many cases, it is better to have more information on the conditions. The local condition is replaced then by a non-local condition, which gives a better effect than the local initial or boundary condition, since the measurement given by a non-local condition is usually more precise than the only one measurement given by a local condition. The study of initial value problems with non-local conditions is of significance, since they have applications in problems in physics and other areas of applied mathematics.

    Hilfer [24] developed a new sort of fractional derivative that combines Riemann-Liouville (R-L) and Caputo fractional derivative (FDs). Impulsive differential equaitions plays an important role in the real life applications. Many authors have examined the applications of this, see[19,20,22,23]. Inspired by this work, several scholars have recently expressed a strong interest in this area, and readers can consult past investigations [25,29]. Various authors studied the outcomes of controllability results for linear and nonlinear integer-order differential equations in [10,11,14,15,16,17,21,26,29,30,31,32,33,34].

    Nonetheless, to the best of our knowledge, the topic of controllability addressed in this article has not been studied, which provides an impetus for our research. The Hilfer fractional implusive differential equation (H-FIDEs) have the following form:

    Dζ,η0+u(t)=Au(t)+F(t,ut)+Bv(t),tY=(0,p],ttk, (1.1)
    Δu|t=tk=Ik(u(tk)),k=1,2,,m, (1.2)
    I(1ζ)(1η)0+u(t)=ϕ(t)+g(yt1,yt2,yt3,,ytm)Pg, (1.3)

    where Dζ,η0+ denotes the Hilfer FD of order ζ and type η. Also, 0ζ1;12<η<1 and (U,) is a Banach space and A denotes the infinitesimal generator of a strongly continuous functions of bounded linear operators {T(t)}t0 on U. A suitable function F:Y×PgU is connected with the phase space uθ(t) with the mapping ut:(,0]U,uθ(t)=u(t+θ),θ0. Here, v() is provided in L2(Y,V), a Banach space of admissible control functions; 0<t1<t2<t3<,<tmp,g:PgPg denotes continuous functions.

    The article is organized as follows: Section 2 introduces a few key notions and definitions related to our research that will be used throughout the discussion of this article. Section 3 is flipped to discuss the controllability results of the H-FIDEs. Finally, Section 4 provides an example to illustrate the theory.

    Now we recall some definitions, concepts, and lemmas chosen to achieve the desired outcomes. Let PC(Y,U) be the Banach space of all continuous function spaces from YU. Assume that γ=ζ+ηζη, In our case, (1γ)=(1ζ)(1η). Now, define C1γ(Y,U)={u:t1γz(t)PC(Y,U)}, along γ defined by uγ=sup{t1γu(t),tY,γ=(ζ+ηζη)}. Clearly, C1γ(Y,U) is a Banach space. We introduce F with norm, FLμ(Y,R+), whenever FLμ(Y,R+) for some μ with 1μ.

    We will now discuss some significant fractional calculus results (see Hilfer [24]).

    Definition 2.1. Let F:[p,+)R and the integral

    Iηp+F(t)=1Γ(η)tpF(θ)(tθ)η1dθ,t>p,η>0

    be called the left-sided R-L fractional integral of order η having a lower limit p of a continuous function, where Γ() denotes the gamma function provided that the right-hand side exists.

    Definition 2.2. Let F:[p,+)R and the integral

    (RL)Dηp+F(t)=1Γ(kη)(ddt)ktpF(t)(tθ)kη1dt,t>p,k1<η<k

    be called the left-sided (R-L) fractional derivative of order η[k1,k), where kR.

    Definition 2.3. Let F:[p,+)R and the integral

    Dζ,ηp+F(t)=(Iζ(1η)p+D(I(1ζ)(1η)p+F))(t)

    be called the left-sided Hilfer-fractional derivative of order 0ζ1 and 0<η<1 function of F(t).

    Definition 2.4. Let F:[p,+)R and the integral

    CDμp+F(t)=1Γ(kη)dkdtktpF(k)(t)(tθ)kη1dt,t>p,k1<η<k

    be called the left-sided Caputo's derivative type of order η(k1,k), where kR.

    Remark 2.5. (i) The Hilfer FD coincides with the standard (R-L) FD; if ζ=0,0<η<1 and p=0, then

    D0,η0+F(t)=ddtI1η0+F(t)=(RL)Dη0+F(t);

    (ii) The Hilfer FD coincides with the standard Caputo derivative; if ζ=1,0<η<1 and p=0, then

    D1,η0+F(t)=I1η0+ddtF(t)=CDη0+F(t).

    Let us characterize the abstract phase space Pg and refer to [35] for more details. Consider that g:(,0](0,+) is continuous along j=0g(λ)dλ<+. For each k>0,

    P={ψ :[i,0]U such that ψ(λ) is bounded and measurable},

    along

    ψ[i,0]=supδ[i,0]ψ(δ)

    for all ψP.

    Now, we define

    Pg={ψ:(,0]U such that for any i>0,ψ|[i,0]P and 0g(δ)ψ[δ,0]dδ<+},

    provided that Pg is endowed along

    ψPg=0g(δ)ψ[δ,0]dδ

    for all ψPg; therefore, (Pg.Pg) is a Banach space.

    Now, we discuss

    Pg={u:(,p)U such that u|YC(Y,U),u0=ψPg,k=0,1,,n},

    where uk is a limitation of u to Y=(λk,λk+1] for k=0,1,,n.

    Set p as semi-norm in Pg defined by

    up=ϕPg+supu(χ):χ[0,p]},uPg.

    Lemma 2.6. Assuming uPg; then, for λY,uPg. Moreover,

    j|u(λ)|uλPgϕPg+jsupδ[0,λ]u(δ),

    where

    j=0g(λ)dλ<+.

    Lemma 2.7. A continuous function u:(,p]U is said to be an integral solution of H-FIDEs (1.1)–(1.3) if

    (i) u:[0,p]U is continuous;

    (ii) Ibo+u(t)D(A) for t[0,p]; and

    (iii) For [0,p], the system u(t) satisfies

    u(t)=ϕ0Γ(ζ(1η)+η)t(ζ1)(1η)+g(yt1,yt2,yt3,,ytm)+1Γ(η)t0(tϱ)(η1)F(ϱ,uϱ)dϱ+1Γ(η)t0(tϱ)(η1)Bv(ϱ)dϱ,+0<ti<tSζ,η(tti)Ii(u(ti))

    for tY.

    Remark 2.8. We introduce the mild solution of the H-FIDEs by introducing the Wright function to M(ψ). (1.1)–(1.3) as follows:

    M(ψ)=k=1(ψ)k1(k1)!Γ(1kη),0<η<1,ψC

    and it satisfies

    0ψϱM(ψ)dψ=Γ(1+ϱ)Γ(1+ηϱ)

    for ψ0.

    Lemma 2.9. If the H-FIDEs (1.1)(1.3) are satisfied, then F:Y×PhU; we get

    u(t)=Sζ,η(t)[ϕ0+g(yt1,yt2,yt3,,ytm)]+t0Pη(t)F(t,uϱ)dϱ+t0Pη(t)Bv(ϱ)dϱ+0<ti<tSζ,η(tti)Ii(u(ti)),

    where tY,

    Qη(t)=0ηψM(ψ)S(tηψ)dψ

    and

    Pη(t)=tη1Qη(t);Sζ,η(t)=Iζ(1η)0+(t)tη1Qη(t).

    Definition 2.10. A continuous function u:(,p]U is defined as a mild solution of H-FIDEs (1.1)–(1.3) if u0=ϕ(0)Pg on (,0] that satisfies

    u(t)=Sζ,η(t)[ϕ(0)+g(yt1,yt2,yt3,,ytm)]+t0(tϱ)η1Qη(tϱ)F(ϱ,uϱ)dϱ+t0(tϱ)η1Qη(tϱ)Bv(ϱ)d(ϱ)+0<ti<tSζ,η((tti))Ii(u(ti)), (2.1)

    where tY,

    Sζ,η(t)=0χη(ψ)M(tηψ)dψ,Qη=η0ψχη(ψ)M(tηψ)dψ

    are the characteristic solution operators and for ψ(0,),

    χη(ψ)=1ηψ11ηwη(ψ1η)0,¯wη(ψ)=1πk=1(1)n1ψnη1Γ(nη+1)nsin(nπη).

    Here, χη is a probalility denisty function(pdf) defined on (0,), that is, χη(ψ)0,ψ(0,) and 0χη(ψ)dψ=1.

    Remark 2.11. For v[0,1], we have

    0ψvχη(ψ)dψ=0ψηv¯ψη(ψ)dψ=Γ(1+v)Γ(1+ηv).

    Lemma 2.12. The functions Sζ,η and Qη satisfy the following:

    (i) Any fixed t0,Sζ,η and Qη are linear and bounded that is, for any uU,

    Sζ,η(t)uMtγ1Γ(ζ(1η)+η)uandQη(t)uMΓ(η)u,

    where Sζ,η(t)=Iζ(1η)0+Pη(t) and Pη(t)=tη1Qη(t);

    (ii) {Sζ,η(t)}t0 and {Qη(t)}t0 are strongly continuous functions.

    Lemma 2.13. The H-FIDEs (1.1)–(1.3) are said to be controllable on Y for every ϕPg,u1U; there exists vL2(Y,V) such that the mild solution u(t) of (1.1)–(1.3) satisfies u(p)=u1.

    Lemma 2.14. {Qη(t)}t0 and {Sζ,η(t)}t0 are strongly continuous, that is, for any uU, 0<t<tp,

    (t)η1Qη(t)u(t)η1Qη(tu0

    and Sζ,η(t)uSζ,η(t)u0 as tt.

    We now present the basic result on measures of non-compactness (MNCs).

    Definition 2.15. ([26]). Assume F+ is the positive cone of ordered Banach space (F,). The value of F+ is said to be an MNC on U of D defined on the set of all bounded subsets of U iff D(¯coα)=D(α) for all bounded subsets αU, where ¯coϕ is a closed convex hull of α. The measure of non-compactness ϕ is said to be the following:

    (i) Monotone iff, for all bounded subsets α, α1,α2 of U we have (α1ϕ2)(D(α1)D(α2));

    (ii) Non-singular iff D({c}α)=D(α) for every cU,αU;

    (iii) Regular iff D(α)=0 iff α is relatively compact in U.

    The MNC of the Hausdorff R is defined on each bounded subset α of U by

    R(α)=inf{D>0:α can be covered by a finite number of balls of radii smaller than D}

    for all bounded subsets α,α1,α2 of U;

    (iv) R(α1+α2)R(α1)+R(α2), where α1+α2={x1+x2:x1α1,x2α2};

    (v) R(α1+α2)max{R(α1),R(α2};

    (vi) R(ρα)|ρ|R(α) for any ρR;

    (vii) Let Z be a Banach space. If Q is Lipschitz continuous with the mapping Q:E(Q)UZ with i>0, then RZ(Qα)iR(α) for any bounded subset αE(Q).

    Lemma 2.16. If HC(Y,U) is bounded and eqicontinuous, then tR(H(t)) is continuous for any tY,

    R(H)=suptY{R(H(t)),tY},

    where H(t)={u(t):uH}U.

    Theorem 2.17. {vm}m=1 is a sequence of Bochner integrable functions from YU with the estimation vm(t)ϵ(t) for almost all tY and every m1, where ϵL(N,R); then, α(t)=R({vm(t):m1})L1(N,R) and satisfies R({t0vm(ϱ)dϱ:m1})2t0ϕ(ϱ)dϱ.

    Lemma 2.18. Suppose F is a closed convex subset of U and tF, X:EY is continuous which fulfills Monch's cndition, i.e., PF is countable, P¯co(0)G(P))¯P is compact. Then, X has a fixed point in F.

    This section is mainly focusing on the mild solutions of H-FIDEs (1.1)–(1.3). Consider the following assumptions for the discussion of H-FIDEs (1.1)–(1.3):

    (H0) For all bounded subsets FU and uF,

    T(t2ηϱ)uT(t1ηϱ)u0,ast2t1

    for each fixed ϱ(0,).

    (H1) F:[0,p]×PhU fulfiles the following:

    (i) Let F(,ϕ) be a measurable function ϕPg and F(t,) be continuous for tY and for uPg,G(,):[0,T]U is strongly measurable.

    (ii) q1(0,η),η(0,1) and l1L1q1(U,R+) and α:R+R+G(t,ϕ)l1(t)ψ(t1γϕPg, for all (t,ϕ)Y×Pg where Φ satisfies liminfmΦ(m)m=0.

    (iii) q2(0,η) and l2L1q1(Y,R+) such that for any bounded subset G1Pg,

    R(F(t,G1))l2(t)[sup<α0R(G1(ρ))]

    for a.e. tY, where G1(ρ)={D(ρ)E1} and R is the Hausdroff measure of non-compactness.

    (iv) Let Ii:FF denote continuous functions and there exists a constant N>0 such that, for all tY, we have Ii(u1)Ii(u2)Nu1u2.

    (H2) The operator W:L2(Y,V)U which is bounded and defined by

    Wv=p0(pϱ)η1Qη(tϱ)Bv(ϱ)dϱ,

    satisfies the following:

    (i) The bounded linear operator W having an inverseW1 takes value in L2(Y,V)/KerW; there exist Nb>0and Nw>0, such that BNb and W1Nw.

    (ii) For q3(0,η) and for every bounded subset FU, l2L1q3(J,R+) such that R((W1)(t))l3(t)R(F). Here, liL1q3(J,R+)andqi(0,η),i=1,2,3.

    (H3) The function g:PnP is continuous; there exists Li(g)>0 such that

    g(v1,v2,,vn)g(w1,w2,,wn)mi=1Li(g)viwiPg,

    for all vi,wiPg and consider Ng=sup{g(v1,v2,,vm):viPg}.

    Let us introduce

    N1=k1l1L1q1(Y,R+),N2=k2l2L1q2(Y,R+),N3=k3l1L1q3(Y,R+),ki=[(1qiηqi)pηqi1qi]1qi,i=1,2,3,K=η11q,
    N=p(1+K)(1q)(1+K)(1q),q,qi(0,η).

    Theorem 3.1. Suppose (H0)(H2) are satisfied; then, the H-FIDEs (1.1)(1.3) are controllable on [0,p] if

    C2NN2p1γΓ(η)[1+2NNbN3Γ(η)]<1forsome12<η<1. (3.1)

    Proof. By using (H2), we define the control vu(t) by

    vu(t)=W1

    ×[u1Sζ,η[ϕ(0)+g(yt1,yt2,yt3,,ytm)p0(pϱ)η1Qη(pϱ)F(ϱ,uϱ)dϱ+0<ti<tSζ,η(tti)Ii(u(ti))](t).

    Let α:PgPg be defined by

    αu(t)={ϕ(t),t(,0]Sζ,η(t)[ϕ(0)+g(yt1,yt2,yt3,,ytm)]+t0(tϱ)η1Qη(tϱ)F(ϱ,uϱ)dϱ+t0(tϱ)η1Qη(tϱ)Bvu(ϱ)dϱ+0<ti<tSζ,η(tti)Ii(u(ti)),tY. (3.2)

    For ϕPg, we define ϕ by

    ˆϕ(t)={ϕ(t),t(,0]Sζ,η(t)ϕ(0),tY;

    then ϕPg. Let u(t)=t1γ[w(t)+ˆϕ(t)], <tp. It can be easily shown that u from (2.1) iff w satisfied w0=0 and

    W(t)=t0(tϱ)η1Qη(tϱ)F(ϱ,ϱ1γ[wϱ+ˆϕϱ])dϱ+t0(tϱ)η1Qη(tϱ)Bvw(ϱ)dϱ+0<ti<tSζ,η(tti)Ii(u(ti)),

    where

    vw(t)=W1[u1Sζ,η(p)[ϕ(0)+g(yt1,yt2,yt3,,ytm)]p0(pϱ)η1Qη(pϱ)×F(ϱ,ϱ1γ[Wϱ+ˆϕϱ])dϱ+0<ti<tSζ,η(tti)Ii(u(ti))](t).

    Let Pg={wPg:w0=0Pg}. For any wPg,

    wp=w0Pg+sup{w(ϱ)}:0ϱp}=sup{w(ϱ):0ϱp}.

    Hence, (Pg,.p) is a Banach space. Now, q>0; choose Gq={wPg:wpq}; then, GqPg is uniformly bounded, and for wGq, in view of Lemma 2.6,

    wt+ˆϕtPgwtPg+ˆϕtPgj(q+M|ϕ|Γ(ζ(1η)+η))+ϕPg=q. (3.3)

    Let us introduce an operator ˜Φ:PgPg, defined by

    ˜Φw(t)={0,t(,0],t0(tϱ)η1Qη(tϱ)F(ϱ,ϱ1γ[wϱ+ˆϕϱ])dϱ+t0(tϱ)ϱ1Qη(tϱ)Bvw(ϱ)dϱ+0<ti<tSζ,η(tti)Ii(u(ti)),tY. (3.4)

    Next, to prove that ˜Φ has a fixed point, our proof contains the subsequent four steps.

    Step 1. Let us prove that there exists a q>0 such that ˜Φ(Gq)Gq. If not, then wqGq. But ˜Φ(wq)Gq that is (˜Φwq)(t)>q for all tY.

    Choose q>0, and let {Gq=uC:uγq}. Obviously, Gq is a closed, bounded and convex set of C. Therefore,

    ˜Φ(uq)γsup{t1γ˜Φ(uq)(t),tY:˜Φ(uq)(t)>q}.

    By using Hölder's-inequality, Lemma 2.12, (H1) and (H2), we get

    q<suptFt1γ˜Φ(ωq)(t)p1γt0(tϱ)η1Qη(tϱ)F(ϱ,ϱ1γ[wϱq+ˆϕϱ])dϱ+p1γt0(tϱ)η1Qη(tϱ)Bvωq(ϱ)dϱ+p1γ0<tk<tSζ,η(t)Ii(u(ti))Np1γΓ(η)t0(tϱ)η1F(ϱ,ϱ1γ[ωϱq+˜ϕϱ])dϱ+Np1γΓ(η)t0(tϱ)η1Bvωq(ϱ)dϱ+Ntβ1p1γΓ(ζ(1η)+η)0<ti<tIi(u(ti))Np1γΓ(η)t0(tϱ)η1l1Φ(q)dϱ+Np1γΓ(η)t0(tϱ)η1BW1(×)[u(p)Sζ,η(t)[ϕ(0)+g(yt1,yt2,yt3,,ytm)]p0(pϱ)η1Qη(pϱ)F(ϱ,ϱ1γ[Wqϱ+ˆϕϱ])dϱ](ϱ)dϱ+NNtβ1p1γΓ(ζ(1η)+η)uNp1γΓ(η)t0(tϱ)η1l1ψ(q)dϱ+NNbNω[p1γΓ(η)t0(tϱ)η1u1+Npγ1Γ(ζ(1η)+η)ϕ(0)+NΓ(η)d0(dϱ)η1l1Φ(q)dϱ]dϱ+NNtβ1p1γΓ(ζ(1η)+η)uNN1p1γΓ(η)Φ(q)+NNbMωΓ(η)N[p1ηu1+NΓ(ζ(1η)+η)ϕ)(0)+NN1p1γΓ(η)Φ(q)]+NNtβ1p1γΓ(ζ(1η)+η)utY. (3.5)

    Divide (3.5) by q, and letting q, we have

    1NN1p1γΓ(η)Φ(q)(1+NNbNωΓ(η)N),tY. (3.6)

    and then by (H1)(ii), (3.6) is a contradiction. Hence, ˜Φ(Gq)Gq

    Step 2. ˜Φ is continuous on Gq. For any ωm,ωGq(Y), m=0,1,2, with limmωm=ω, then we have limmωm=ω(t) and

    limmt1γωm(t)=t1γω(t).

    Let u(t)=t1γ[ω(t)+ˆϕ(t)]; then, {ωm+ˆϕ}Gq with ωm+ˆϕω+ˆϕ in Gq as m. Then, we have

    F(t,um(t))=F(t,t1γ[wm(t)+ˆϕ(t)])F(t,t1γ[w(t)+ˆϕ(t)])=F(t,u(t)),as,m,

    where F(t,t1γ[ωm(t)+ˆϕ(t)])=Gm(ϱ) and F(t,t1γ[ω(t)+ˆϕ(t)])=G(ϱ). Then, by using the hypotheses (H1) and Lebesgue's dominated convergence theorem, we have

    t0(tϱ)η1Gm(ϱ)G(ϱ)dϱ0 as m,tY. (3.7)

    Now, by (H1),

    ˜Φωm˜ΦwCp1γt0(tϱ)η1Qη(tϱ)[F(ϱ,ϱ1γ[ωmϱ+ˆϕϱ])F(ϱ,ϱ1γ[ωϱ+ˆϕϱ])]dϱ+p1γBt0(tϱ)η1Qη(tϱ)B[vωm(ϱ)vω(ϱ)]dϱ+p1γSζ,η(t)0<ti<tIi(um(ti))Ii(u(ti))Np1γΓ(η)t0(tϱ)η1[F(ϱ,ϱ1γ[ωmϱ+˜ϕϱ])]F(ϱ,ϱ1γ[wϱ+˜ϕ)]dϱ+NNbp1γΓηt0(tϱ)η1[vωm(ϱ)vω(ϱ)]dϱ+NNtβ1p1γΓ(ζ(1η)+η)um(ti)u(ti)Np1γΓ(η)t0(tϱ)η1[Gm(ϱ)G(ϱ)]dϱ+N2NbNωp1ηΓ(η)2t0(tϱ)η1(×)(p0(pϱ)η1)|Gm(ϱ)G(ϱ)]dϱ)dϱ+NNtβ1p1γΓ(ζ(1η)+η)um(ϱ)u(ϱ). (3.8)

    Observing (3.7) and (3.8), we have ˜Φωn˜ΦωC0, m, Therefore, ˜ΦΦ(Gq) is continuous on Gq.

    Step 3. ˜Φ(Gq) is equi-continuous on Y. for all α˜Φ(Gq) such that α(t2)α(t1)0 as t2t1.

    α(t)=Sζ,η(t)[ϕ0+g(yt1,yt2,yt3,,ytm)]+t0(tϱ)μ1Qη(tϱ)G(ϱ)dϱ+t0(tϱ)μ1Qη(tϱ)Bvω(ϱ)dϱ+0<tk<tSζ,η(ttk)Ii(u(ti)).

    Let 0<ϵ<t and 0<t1<t2<p. Then, ˜Φ(Gq) is equicontinuous on Y.

    α(t2)α(t1)=t1γ2t20(t2ϱ)η1Qη(t2ϱ)[G(ϱ)+Bvω(ϱ)]dϱt1γ1t10(t1ϱ)η1Qη(t1ϱ)[G(ϱ)+Bvω(ϱ)]dϱ+0<ti<t2t1Sζ,η(t2)Sζ,η(t1)Iiu(ti)t1γ2t2t1(t2ϱ)η1Qη(t2ϱ)[G(ϱ)+Bvω(ϱ)]dϱ+t1t1ϵt1γ2(t2ϱ)η1[Qη×(t2ϱ)Qη(t1ϱ)][G(ϱ)+Bvω(ϱ)]dϱ+t1t1ϵ[t1γ2(t2ϱ)η1t1γ1(t1ϱ)η1]×Qη(t1ϱ)[G(ϱ)+Bvω(ϱ)]dϱ+t1ϵ0t1γ2(t2ϱ)η1[Qη(t2ϱ)Qη(t1ϱ)]×[G(ϱ)+Bvω(ϱ)]dϱ+t1ϵ0[t1γ2(t2ϱ)η1t1γ1×(t1ϱ)η1)[Qη(t1ϱ)[G(ϱ)+Bvω(ϱ)]dϱ++NNΓ(ζ(1η)+η)(tγ12tγ11)u.

    α(t2)α(t1) becomes zero as t2t10 by using absolute continuity of the Lebesgue dominance theorem. Hence, ˜Φ(Gq) is equicontinuous on Y.

    Step 4. Let us verify Mönch's condition.

    Let ω0(t)+ˆϕ(t)=t1γSζ,η(t)ˆϕ0 for all tY and wn+1+ˆϕ(t)=˜Φ[wn+^ϕ(t)],n=0,1,2,3, and ˜Φ be relatively compact.

    Assume HPq is countable and Hconv{0}˜ψ(H). Our aim here is to show that R(H)=0, where R is the Hausdroff measure of non compactness. Suppose H={ωn+{ϕ}n=1}. Now we have to show that ˜Φ(H)(t) is relatively compact in Y, for all tY. From Theorem 2.17

    R(H(t))=R({(wn+ϕ)(t)}n=0)=R({(w0+ϕ)(t)}{(wn+ϕ)(t)}n=1)=R({wn(t)+ϕ(t)}n=1),

    and

    R({˜ψwn(t)}n=1)=R({t1γt0(tϱ)η1×Qη(tϱ)[Gn(ϱ)+Bvun(ϱ)]dϱ}n=1)=I1+I2,

    where

    I1=2Nd1γΓ(η)t0(tϱ)η1R({Gn(ϱ)}n=1)dϱ2Np1γΓ(η)t0(tϱ)η1R({F(ϱ,ϱ1γ[wnϱ+ˆϕϱ])}n=1dϱ2Np1γΓ(η)t0(tϱ)η1l2(ϱ)sup<θ0R({F(ϱ1γ[ωn(ϱ+φ)+ˆϕ(ϱ+φ)])}n))dϱ2Np1γΓ(η)t0(tϱ)η1l2(ϱ)sup0ψϱR(H(ψ))dϱ,
    I2=2NNbp1γΓ(η)t0(tϱ)η1R({vun(ϱ)}n=1)dϱ2NNbp1γΓ(η)t0(tϱ)η1[2NΓ(η)×p0(pϱ)η1R({F(ϱ,ϱ1γ))[ωnϱ+{(ˆϕ)}n=1}dϱ]dϱ4N2Nbp1γΓ(η)t0(tϱ)η1l3(ϱ)×t0(tϱ)η1l2(ϱ)sup0<ψϱR(H(ψ))dϱ]dϱ,
    I1+I2=[2NN2p1γΓ(η)+4N2NbN2N3p1γΓ(η)2]sup0<θϱR(H(ψ))2NN2p1γΓ(η)[1+2NN3Nbp1γΓ(η)]×sup0<ψϱR(H(ψ)).

    From Lemma 2.16, R(˜Φ(H))CR(H), where C is defined in 3.1. Then, from Mönch's condition,

    R(H)(conv{0}(˜Φ)))=R(˜Φ)CR(H),

    R(H)=0 and then H is relatively compact. From Lemma 2.18, ˜Φ has a fixed point ω in Gq. Therefore, u=ω+ˆϕ is a mild solution of the H-FIDEs (1.1–1.3) satisfying u(p)=u1. Hence, the systems (1.1–1.3) is controllable on Y, and the proof is completed.

    Now, analyze the following problem:

    Dζ,230+u(t,μ)=2μ2u(t,μ)+Wϑ(t,μ)+ϑ(t,tϑ1(σt)u(σ,μ)dσ), (4.1)
    Δu|t=ti=Ii(u(ti)),i=1,2,n, (4.2)
    I(1ζ)13[u(t,μ)]|μ=0=u0(μ),μ[0,π], (4.3)
    u(t,0)=u(t,π)=0,t0, (4.4)
    u(0,μ)=ϕ(t,μ),0μπ. (4.5)

    From previous equations, Dζ,230+ denotes the Hilfer FD of order η=23, and type ζ,I(1ζ)13 is the (R-L) integral of order (1ζ)13, ϕPh and ϑ:J×[0,1] is continuous. To change this frame-work into the abstract structure (1.1) and (1.2), let U=L2[0,π] be endowed with the norm L2 and A:D(A)UU be given by AE=E along with

    D(A)={E,EY:E,Eare absolutely continous,EY,+E(0)=E(π)=0}. (4.6)

    Here, A is an infinitesimal generator of a semigroup {T(t),t0} in where Y and it is given by T(t)ω(σ)=w(t+σ); for ωU, T(t) is not compact on U and R(T(t)H)R(H), where R is the Hausdorff MNC, and there exists N1 such that suptYT(t)N. Furthermore, tω(t23+σ)u is equicontinuous for t0 and μ(0,). Let F:[0,π]×UU by

    F(t,π)(μ)=ϑ(t,tϑ1(σt)u(σ,μ)dσ),

    and

    Dζ,230+u(t)(μ)=23μ23u(t,μ),u(t)(μ)=u(t,μ).

    Let B:VV be defined by (Bv)(t)(μ)=Wϑ(t,μ),0<μ<1. By assuming the suitable choices of A, B and F, the H-FIDEs (4.1)–(4.4) can be rewritten as

    Dζ,η0+u(t)=Au(t)+F(t,ut)+Bv(t),tR=(0,p], (4.7)
    Δu|t=ti=Ii(u(ti)),i=1,2,n, (4.8)
    I(1ζ)(1η)0+u(t)|t=0=ϕ(t),t(,0]. (4.9)

    For μ(0,π), W is given by

    Wv(μ)=10(1t)13Qη(1t)Fϑ(t,μ)dt,

    where

    Q23=230μχ23(μ)W(t23+μ)dμ,

    and

    χ23(μ)=32μ132ˉw23(μ32),
    ¯w23(μ)=1πn=1(1)n1t23n1Γ(23n+1)n!sin(2nπ3).

    In the above, χ23 is defined on (0,), that is,

    χ23(μ)0,μ(0,)and0χ23(μ)dμ=1.

    We take ϑ(t,tϑ1(σt)u(σ,μ)dσ)=C0sin(y(σ)), where C0 is a constant. Then, F and W satisfy the hypotheses (H1)(H3). This completes the example.

    In our study, we used non-compactness measures to investigate the controllability of Hilfer fractional impulsive differential systems with infinite delay. We started with the Hilfer fractional impulsive differential systems with controllability and applied Mönch's fixed point theorem for indefinite delay; then, extended our results to the concept of non-local conditions. Finally, an example case was provided to demonstrate the significance of our major findings. In the future, we will use the MNC to investigate the existence and controllability of Sobolov-type Hilfer fractional implusive differential systems with indefinite delay. In addition to this, we can extend our results with integro or implicit terms and we can use integral boundary conditions which has real life applications. Also we can provide some numerical approximations for this considered system.

    This research received funding support from the NSRF via the Program Management Unit for Human Resources & Institutional Development, Research and Innovation (grant number B05F650018).

    The authors declare no conflicts of interest.



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