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An investigation on boundary controllability for Sobolev-type neutral evolution equations of fractional order in Banach space

  • The main focus of this paper is on the boundary controllability of fractional order Sobolev-type neutral evolution equations in Banach space. We show our key results using facts from fractional calculus, semigroup theory, and the fixed point method. Finally, we give an example to illustrate the theory we have established.

    Citation: Yong-Ki Ma, Kamalendra Kumar, Rohit Patel, Anurag Shukla, Kottakkaran Sooppy Nisar, Velusamy Vijayakumar. An investigation on boundary controllability for Sobolev-type neutral evolution equations of fractional order in Banach space[J]. AIMS Mathematics, 2022, 7(7): 11687-11707. doi: 10.3934/math.2022651

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  • The main focus of this paper is on the boundary controllability of fractional order Sobolev-type neutral evolution equations in Banach space. We show our key results using facts from fractional calculus, semigroup theory, and the fixed point method. Finally, we give an example to illustrate the theory we have established.



    In recent decades, fractional calculus has played a significant role in mathematics. Some physical problems cannot be addressed using integer-order differential equations, while fractional-order differential equations can. Fractional differential equations have received a lot of attention and are utilized widely in engineering, physics, chemistry, biology, and a variety of other subjects. Fractional calculus notions have lately been effectively applied to a wide range of domains, and scientists are increasingly realizing that the fractional system may well correspond to many occurrences in regular sciences and engineering. Rheology, liquid stream, scattering, microscopic structures, viscoelasticity, and optics are just a few of the significant fractional calculus issues that are now being studied. Although diagnostic structures are often difficult to come by, the efficacy of mathematical evaluation methodologies for fractional systems in these disciplines has impressed some academics. Readers can check [1,2,3,6,7,14,15,16,17,18,22,25,26,27,28,29,30,31,33,35,37,38,39,40,41,44,52,54,55,56,57,58,59].

    The use of controllability notation in the research and design of control systems is beneficial. Fractional derivatives of various significations can be used to address these types of difficulties. It may be used in a range of sectors, including economics, chemical outgrowth control, biology, power systems, space technology, engineering, electronics, physics, robotics, transportation, chemistry, and so on. The topic of controllability is particularly important in control theory. If the control system is controllable, it can manage a variety of issues such as stability, pole assignment, and optimum control. Boundary controllability plays an important role in the analysis and design of control systems. The researchers in the recent years derived results on controllability for a variety of systems like neutral systems, integrodifferential equations, impulsive systems, fixed delay systems, and time-varying delay systems, etc. Solving these types of seeds has become a significant work for young scholars, one can refer to [1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,20,21,23,27,28,29,31,32,33,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53].

    Fattorini proved the controllability condition on the first and second-order boundary control systems by replacing boundary controls with distributed controls [13]. By assuming exact controllability of the linear system and approximate controllability of linearization, the authors [21] studied global controllability for the abstract semilinear system. [2] obtained results for approximate boundary controllability of stochastic control systems of fractional order with Poisson jump and fractional Brownian motion are cited by the authors. Zhou et al. [59] derived various conditions for the existence of mild solutions with the help of fixed point theorems and fractional power of operators for neutral fractional-order evolution equations having nonlocal conditions.

    Also, authors in [22] established results for the neutral integrodifferential fractional-order system having nonlocal conditions and finite delays in abstract space with the help of the measure of noncompactness. In [4] authors established some sufficient conditions for boundary controllability of integrodifferential system of Sobolev-type with the help of Banach contraction principle and theory of strongly continuous operators. With the help of Schauder's fixed point theorem, Ahmed [3] established sufficient conditions for boundary controllability of integrodifferential fractional-order non-linear system in abstract space. Inspired by the above and recent work, to the best of our knowledge there is no article dealing with boundary controllability for Sobolev-type neutral evolution equations of fractional order using this technique. We obtained sufficient conditions for boundary controllability. The results are advanced and weighed as an improvement to the control theory for fractional-order control systems.

    The paper is structured in the following manner: In segment 2, we propose a few elementary definitions. In segment 3, we obtained results for boundary controllability. In segment 4, we discussed an example to understand theoretical results.

    Assume that Y and Z be two real Banach spaces with and ||. Assume that σ be a closed linear and densely defined operator with domain D(σ)Y and R(σ)Z. Consider Q be a linear operator with D(Q)Y and R(Q)X, a Banach space together X.

    Assume that the boundary control of neutral evolution equations of Sobolev-type with fractional order of the form

    cDα[Sx(ϖ)+F(ϖ,x(ϖ),x(b1(ϖ)),,x(bm(ϖ)))]=σx(ϖ)+G(ϖ,x(ϖ),x(a1(ϖ)),,x(an(ϖ))),ϖJ=[0,b], (2.1)
    Qx(ϖ)=B1u(ϖ),x(0)=x0. (2.2)

    In the above, S:D(S)YR(S)Z is a linear operator, the control function uL2(J,U), a Banach space of admissible control function with U as a Banach space, B1:UX is a linear continuous operator and ai,bjC(J,J),i=1,2,,n, j=1,2,,m where C(J,J) is a set of all continuous function defined from J to J. G and F are the appropriate functions to be specified later and cDα,0<α<1 is in the Caputo sense. Let y(ϖ)=Sx(ϖ) for xY, then (2.1) and (2.2) can be written as

    cDα[y(ϖ)+F(ϖ,S1y(ϖ),S1y(b1(ϖ)),,S1y(bm(ϖ)))]=σS1y(ϖ)+G(ϖ,S1y(ϖ),S1y(a1(ϖ)),,S1y(an(ϖ))),ϖJ=[0,b], (2.3)
    ˜Qy(ϖ)=B1u(ϖ),y(0)=y0, (2.4)

    where ˜Q=QS1:ZX is a linear operator. The operator A:YZ given by

    D(AS1)={wD(σS1):˜Qw=0},

    AS1w=σS1w for wD(AS1), (see [4,23]).

    Definition 2.1. [4,23] The operators A:D(A)YZ and S:D(S)YZ satisfying the following hypotheses:

    (H1)A and S are closed linear operators.

    (H2)D(S)D(A) and S is bijective.

    (H3)S1:ZD(S) is continuous.

    The hypothesis (H1)–(H3) and the closed graph theorem imply the boundedness of the linear operator AS1:ZZ and AS1 generates an analytic compact semigroup of uniformly bounded linear operators {T(ϖ):ϖ0}. This means that there exists a M1 such that T(ϖ)M. Without loss of generality, we assume that 0λ(AS1). This allow us to define the fractional power (A)q, for 0<q<1 as a closed linear operator on its domain D((A)q) with inverse (A)q.

    Theorem 2.2. [34]

    (1) Yq=D((A)q) is a Banach space with the norm xq=(A)qx,xY.

    (2) T(ϖ):YYq for each (A)qT(ϖ)x=T(ϖ)(A)qx, for all xYq and ϖ0.

    (3) For all ϖ>0,(A)qT(ϖ) is bounded on Y and there exists a positive constant Cq such that

    (A)qT(ϖ)Cqϖq.

    (4) If 0<β<q1, then D(A)qD(A)β and the embedding is compact whenever the resolvent operator of A is compact.

    Let us recall the following known definitions.

    Definition 2.3. [35] The fractional integral of order α>0 with the lower limit zero for a function f can be defined as

    Iαf(ϖ)=1Γαϖ0f(ν)dν(ϖν)1α,ϖ>0,α>0,

    provided the right-hand side is pointwise defined on [0,), where Γ is the Gamma function.

    Definition 2.4. [35] The Caputo derivative of order α with the lower limit zero for a function f can be written as:

    cDαf(ϖ)=1Γ(nα)ϖ0f(n)(ν)dν(ϖν)α+1n=Inαf(n)(ϖ), ϖ>0,0n1<α<n.

    If f is an abstract function with the values in Y, then the integrals in the above definition are taken in Bochner's sense.

    Lemma 2.5. A measurable function :[0,b]Y is Bochner integrable if || is Lebesgue integrable.

    We now present the following results on the controllability.

    (A1) D(σ)D(Q) and the restriction of Q to D(σ) is continuous relative to graph norm of D(σ).

    (A2) There exists a linear continuous operator S:UZ such that σS1BL(U,Z), ˜Q(Bu)=B1u,for alluU. Also Bu(ϖ) is continuously differentiable and

    (A)βBuCB1u,

    for all uU, where C is a constant.

    (A3) For all ϖ(0,b] and uU, T(ϖ)BuD(AS1). Moreover, there exists a positive function M0>0 such that AS1T(ϖ)M0 (see [3,18]).

    Let y(ϖ) be the solution of the systems (2.3) and (2.4). Then we define a function z(ϖ)=y(ϖ)Bu(ϖ). From the assumptions it follows that z(ϖ)D(AS1). Hence, the systems (2.3) and (2.4) can be written in terms of A and B as

    cDα[z(ϖ)+F(ϖ,S1y(ϖ),S1y(b1(ϖ)),,S1y(bm(ϖ)))]=AS1z(ϖ)+σS1Bu(ϖ)BcDαu(ϖ)+G(ϖ,S1y(ϖ),S1y(a1(ϖ)),,S1y(an(ϖ))), (2.5)
    z(0)=y(0)Bu(0). (2.6)

    For more details, see [1,19]. From the systems (2.5) and (2.6), we present the integral form of the systems (2.3) and (2.4) in the following way:

    y(ϖ)=y(0)+F(0,S1y(0),S1y(b1(0)),,S1y(bm(0)))]F(ϖ,S1y(ϖ),S1y(b1(ϖ)),,S1y(bm(ϖ)))]+1Γαϖ0S1Ay(ν)dν(ϖν)1α1Γαϖ0S1ABu(ν)dν(ϖν)1α+1Γαϖ0S1σBu(ν)dν(ϖν)1α+1Γαϖ0G(ν,S1y(ν),S1y(a1(ν)),,S1y(an(ν)))dν(ϖν)1α, (2.7)

    (see [4,14,22,59]) and hence, the mild solution of the systems (2.1) and (2.2) is presented in the following way:

    x(ϖ)=S1Sα(ϖ)Sx(0)+S1Sα(ϖ)F(0,x(0),x(b1(0)),,x(bm(0)))S1F(ϖ,x(ϖ),x(b1(ϖ)),,x(bm(ϖ)))ϖ0(ϖν)α1ATα(ϖν)S1F(ν,x(ν),x(b1(ν)),,x(bm(ν)))dν+ϖ0S1(ϖν)α1[Tα(ϖν)σS1BAS1Tα(ϖν)B]u(ν)dν+ϖ0S1(ϖν)α1Tα(ϖν)G(ν,x(ν),x(a1(ν)),,x(an(ν)))dν, (2.8)

    where ξα(θ) is a probability density function defined on (0,) and

    Sα(ϖ)=0ξα(θ)T(ϖαθ)xdθ,

    and

    Tα(ϖ)x=α0θξα(θ)T(ϖαθ)xdθ.

    Remark 2.6. [59] ξα(θ)0, θ(0,), 0ξα(θ)dθ=1 and 0θξα(θ)dθ=1Γ(1+α).

    Definition 2.7. [4,14] The systems (2.1) and (2.2) are said to be controllable on the interval J if for every x0,x1Y, there exists a control uL2(J,U) such that the solution x() of the systems (2.1) and (2.2) satisfies x(b)=x1.

    Lemma 2.8. [22] The operators Sα(ϖ) and Tα(ϖ) have the following properties:

    (i) For any fixed xY, Sα(ϖ)xMx, Tα(ϖ)xαMxΓ(α+1).

    (ii) {Sα(ϖ),ϖ0} and {Tα(ϖ),ϖ0} are strongly continuous.

    (iii) For all ϖ0,Sα(ϖ) and Tα(ϖ) are also compact operators.

    (iv) For any xY,β(0,1) and δ(0,1), we have

    (A)Tα(ϖ)x=(A)1βTα(ϖ)(A)βx,

    and

    (A)δTα(ϖ)αCδΓ2δϖαδΓ1+α(1δ),ϖ(0,b).

    Remark 2.9. For any xY,β(0,1) and δ=1, we have

    ATα(ϖ)x=α0θξα(θ)AT(ϖαθ)xdθ=αxM0Γ(1+α).

    Further, assume the following assumptions:

    (A4) The linear operator W from L2(J,U) into Y is given by

    Wu=b0S1(bν)α1[Tα(bν)σS1BAS1Tα(bν)B]u(ν)dν,

    induces an invertible operator ˜W defined on L2(J,U)/KerW, and there exists K1,K2 and K3>0 such that (A)βK1,0<β1,BK2 and ˜W1K3.

    (A5) F:J×Ym+1Y is continuous and there exists β(0,1) and M1,M2>0 such that (A)βF fulfills the subsequent condition:

    (A)βF(ν1,x0,x1,,xm)(A)βF(ν2,y0,y1,,ym)M1(|ν1ν2|+maxi=0,1,,mxiyi),

    for 0ν1,ν2b, xi,yiY,i=0,1,,m and

    (A)βF(ϖ,x0,x1,,xm)M2(maxi=0,1,,mxi+1), (2.9)

    holds for (ϖ,x0,x1,,xm)J×Ym+1.

    (A6) G:J×Yn+1Y fulfill the subsequent conditions:

    (i) For every ϖJ, G(ϖ,):Yn+1Y is continuous and for every (x0,x1,,xn)Yn+1, G(,x0,x1,,xn):JY is strongly measurable.

    (ii) For every kN, there exists hk():[0,b]R+ such that

    supx0,,xnkG(ϖ,x0,x1,,xn)hk(ϖ),
    S(ϖν)1αhk(ν)L1([0,ϖ],R+)

    and there exists >0 such that

    limkinfϖ0(ϖν)1αhk(ν)dνk=<,ϖ[0,b].

    (A7) We assume

    L=S1M1[(M+1)K1+C1βΓ(1+β)bαββΓ(1+αβ)<1, (2.10)
    [MS1K1M2+S1K1M2+S1C1βΓ(1+β)bαβM2βΓ(1+αβ)+S1αMΓ(1+α)](×)(1+[S12σbαMΓ(1+α)+S1bαM0Γ(1+α)]K2K3)<1. (2.11)

    Theorem 2.10. [36,Sadovskii fixed point theorem]Let ϕ be a condensing operator on a Banach space Y, that is ϕ is continuous and takes bounded sets into bounded sets, and μ(ϕ(B))μ(B) for every bounded set B of Y with μ(B)>0. If ϕ(γ)γ for a convex, closed and bounded set γ of Y, then ϕ has a fixed point in Y. (Here μ() denotes Kuratowski's measure of non compactness).

    Theorem 3.1. If (A1)(A7) are fulfilled, then the systems (2.1) and (2.2) are controllable on J.

    Proof. For our convenience, we use the following

    (ϖ,x(ϖ),x(b1(ϖ)),,x(bm(ϖ))=(ϖ,v(ϖ)),

    and

    (ϖ,x(ϖ),x(a1(ϖ)),,x(an(ϖ))=(ϖ,w(ϖ)).

    Using the assumption (A5), for x(), we define

    u(ϖ)=˜W1[x1S1Sα(b)Sx0S1Sα(b)F(0,v(0))+S1F(b,v(b))+b0(bν)α1ATα(bν)S1F(ν,v(ν))dνb0S1(bν)α1Tα(bν)G(ν,w(ν))dν](ϖ).

    We now define P as follows:

    (Px)(ϖ)=S1Sα(ϖ)Sx(0)+S1Sα(ϖ)F(0,v(0))S1F(ϖ,v(ϖ))ϖ0(ϖν)α1ATα(ϖν)S1F(ν,v(ν))dν+ϖ0S1(ϖν)α1Tα(ϖν)σS1Bu(ν)dνϖ0S1(ϖν)α1AS1Tα(ϖν)Bu(ν)dν+ϖ0S1(ϖν)α1Tα(ϖν)G(ν,w(ν))dν,

    has a fixed point and this fixed point is then a solution of (2.1) and (2.2). So, we have to prove that P has a fixed point. For every k>0, we set

    Bk={xY:x(ϖ)k,0ϖb}.

    Then for every k, Bk is clearly a bounded closed convex set in Y. From Lemma 2.8 and Eq (2.9) yields

    ϖ0(ϖν)α1ATα(ϖν)S1F(ν,v(ν))dνϖ0(ϖν)α1S1(A)1βTα(ϖν)(A)βF(ν,v(ν))dνS1αC1βΓ(1+β)Γ(1+αβ)ϖ0(ϖν)αβ1(A)βF(ν,v(ν))dνC1βΓ(1+β)S1bαβM2Γ(1+αβ)[maxi=1,2,,mxi+1]S1C1βΓ(1+β)βΓ(1+αβ)bαβ(k+1)M2,

    then it follows that (ϖν)α1ATα(ϖν)S1F(ν,v(ν)) is integrable on J, by Lemma (2.5), P is well defined on Bk. From (A6)(ii), one can get

    ϖ0S1(ϖν)α1Tα(ϖν)G(ν,w(ν))dνϖ0S1(ϖν)α1Tα(ϖν)G(ν,w(ν))dνS1αMΓ(α+1)ϖ0(ϖν)α1G(ν,w(ν))dνS1αMΓ(α+1)ϖ0(ϖν)α1hk(ν)dν.

    We conclude that for k>0 such that PBkBk. If it fails, then there exist a function xk()Bk but PBkBk, and Pxk(ϖ)>k, for some ϖ(k)J, where ϖ(k) denotes that ϖ is independent of k. Then, one can get

    k(Pxk)(ϖ)S1Sα(ϖ)Sx(0)+S1Sα(ϖ)F(0,vk(0))S1F(ϖ,vk(ϖ))ϖ0(ϖν)α1ATα(ϖν)S1F(ν,vk(ν))dν+ϖ0S1(ϖν)α1[Tα(ϖν)σS1AS1Tα(ϖν)]B˜W1(×){x1S1Sα(b)Sx(0)S1Sα(b)F(0,vk(0))+S1F(b,vk(b))+b0(bτ)α1ATα(bτ)S1F(τ,vk(τ))dνb0S1(bτ)α1Tα(bτ)G(τ,wk(τ))dτ}(ν)dν+ϖ0S1(ϖν)α1Tα(ϖν)G(ν,wk(ν))dνMS1S||x0+MS1||(A)β(A)βF(0,vk(0))+S1||(A)β(A)βF(ϖ,vk(ϖ))+S1C1βΓ(1+β)βΓ(1+αβ)bαβ(k+1)M2+ϖ0S1(ϖν)α1[σ||S1||Tα(ϖν)+AS1Tα(ϖν)](×)B˜W1{x1+MS1S||x0+MS1||(A)β(A)βF(0,vk(0))+S1||(A)β(A)βF(b,vk(b))+S1C1βΓ(1+β)βΓ(1+αβ)bαβ(k+1)M2+b0S1(bτ)α1Tα(bτ)||G(τ,wk(τ))dτ}dν+ϖ0S1(ϖν)α1Tα(ϖν)||G(ν,wk(ν))dνMS1S||x0+MS1K1M2(k+1)+S1K1M2(k+1)+S1C1βΓ(1+β)bαβ(k+1)βΓ(1+αβ)M2+S1bαα[σ||S1αMΓ(α+1)+αM0Γ(α+1)]K2K3(×){x1+MS1S||x0+MS1K1M2(k+1)+S1K1M2(k+1)+S1C1βΓ(1+β)βΓ(1+αβ)bαβ(k+1)M2+αMΓ(α+1)S1b0(bτ)α1hk(τ)dτ}+αMΓ(α+1)S1ϖ0(ϖν)α1hk(ν)dν.

    Dividing by k on both sides of the above inequality and letting k+, one can get

    1MS1K1M2+S1K1M2+S1C1βΓ(1+β)βΓ(1+αβ)bαβM2+S1bαα[σ||S1αMΓ(α+1)+αM0Γ(α+1)]K2K3(MS1K1M2+S1K1M2+S1C1βΓ(1+β)βΓ(1+αβ)bαβM2+αMΓ(α+1)S1)+S1αMΓ(α+1).

    Therefore,

    [MS1K1M2+S1K1M2+S1C1βΓ(1+β)βΓ(1+αβ)bαβM2+S1αMΓ(α+1)](1+[S12σbαMΓ(1+α)+S1bαM0Γ(1+α)]K2K3)1.

    The above equation contradicts Eq (2.11). Thus, for k>0, PBkBk. Now, we need to verify P has a fixed point on Bk, which implies (2.1) and (2.2) have a mild solution. We decompose P as P=P1+P2, where P1 and P2 are determined on Bk by

    (P1x)(ϖ)=S1Sα(ϖ)F(0,v(0))S1F(ϖ,v(ϖ))ϖ0(ϖν)α1ATα(ϖν)S1F(ν,v(ν))dν,

    and

    (P2x)(ϖ)=S1Sα(ϖ)Sx0+ϖ0S1(ϖν)α1[Tα(ϖν)σS1AS1Tα(ϖν)]Bu(ν)dν+ϖ0S1(ϖν)α1Tα(ϖν)G(ν,w(ν))dν,

    for 0ϖb. We have to verify P1 is a contraction mapping if P2 is compact. For checking P1 fulfills the contraction condition, we assume x1,x2Bk. Then, for every ϖJ and by hypothesis (A5) and Eq (2.10), one can get

    (P1x1)(ϖ)(P1x2)(ϖ)S1Sα(ϖ)[F(0,v1(0))F(0,v2(0))+S1[F(ϖ,v1(ϖ))F(ϖ,v2(ϖ))]+ϖ0S1(ϖν)α1ATα(ϖν)[F(ν,v1(ν))F(ν,v2(ν))]dνS1MK1M1sup0νbx1(ν)x2(ν)+S1K1M1sup0νbx1(ν)x2(ν)+S1bαβC1βΓ(1+β)βΓ(1+αβ)M1sup0νbx1(ν)x2(ν).

    Hence

    (P1x1)(ϖ)(P1x2)(ϖ)S1M1[(M+1)K1+C1βΓ(1+β)βΓ(1+αβ)bαβ]sup0νbx1(ν)x2(ν).

    Thus,

    (P1x1)(ϖ)(P1x2)(ϖ)Lsup0νbx1(ν)x2(ν),

    and by assumption 0<L<1, we see that P1 is a contraction. To prove that P2 is compact, firstly we prove that P2 is continuous on Bk. Assume {xn}Bk with xnx in Bk, then for every νJ, wn(ν)w(ν) and by (A6)(i), one can get G(ν,wn(ν))G(ν,w(ν)), when n. By the dominated convergence theorem, one can get

    P2xnP2x=sup0ϖbϖ0S1(ϖν)α1(Tα(ϖν)σS1AS1Tα(ϖν))B[wn(ν)w(ν)]dν+ϖ0S1(ϖν)α1Tα(ϖν)[G(ν,wn(ν))G(ν,w(ν))]dν0,

    when n, i.e., P2 is continuous. Now, we need to verify {P2x:xBk} is an equicontinuous family of functions. For this, we assume ϵ>0 be small, 0<ϖ1<ϖ2, then

    (P2x)(ϖ2)(P2x)(ϖ1)S1||Sα(ϖ2)Sα(ϖ1)||x0+ϖ1ϵ0S1||((ϖ2ν)α1Tα(ϖ2ν)(ϖ1ν)α1Tα(ϖ1ν))σS1Bu(ν)dν+ϖ1ϖ1ϵS1||((ϖ2ν)α1Tα(ϖ2ν)(ϖ1ν)α1Tα(ϖ1ν))S1σBu(ν)dν+ϖ2ϖ1S1||((ϖ2ν)α1Tα(ϖ2ν))S1σBu(ν)dν+ϖ1ϵ0S1||AS1((ϖ2ν)α1Tα(ϖ2ν)(ϖ1ν)α1Tα(ϖ1ν))Bu(ν)dν+ϖ1ϖ1ϵS1||AS1((ϖ2ν)α1Tα(ϖ2ν)(ϖ1ν)α1Tα(ϖ1ν))Bu(ν)dν+ϖ2ϖ1S1||AS1((ϖ2ν)α1Tα(ϖ2ν))Bu(ν)dν+ϖ1ϵ0S1||(ϖ2ν)α1Tα(ϖ2ν)(ϖ1ν)α1Tα(ϖ1ν)||G(ν,w(ν))dν+ϖ1ϖ1ϵS1||(ϖ2ν)α1Tα(ϖ2ν)(ϖ1ν)α1Tα(ϖ1ν)||G(ν,w(ν))dν+ϖ2ϖ1S1||(ϖ2ν)α1Tα(ϖ2ν)||G(ν,w(ν))dν.

    Observe that

    u(ν)K3{x1+MS1S||x0+MS1K1M2(k+1)+S1K1M2(k+1)+S1C1βΓ(1+β)bαβ(k+1)βΓ(1+αβ)M2+αMΓ(α+1)S1b0(bτ)α1hk(τ)dτ}.

    We see that

    (P2x)(ϖ2)(P2x)(ϖ1)S1||Sα(ϖ2)Sα(ϖ1)||x0+ϖ1ϵ0S1||(ϖ2ν)α1Tα(ϖ2ν)(ϖ1ν)α1Tα(ϖ1ν)||σ||S1K2(×)K3{x1+MS1S||x0+MS1K1M2(k+1)+S1K1M2(k+1)+S1C1βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)S1b0(bτ)α1hk(τ)dτ}dν+ϖ1ϖ1ϵS1||(ϖ2ν)α1Tα(ϖ2ν)(ϖ1ν)α1Tα(ϖ1ν)||σ||S1K2K3(×){x1+MS1S||x0+MS1K1M2(k+1)+S1K1M2(k+1)+S1C1βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)S1b0(bτ)α1hk(τ)dτ}dν+ϖ2ϖ1S1||(ϖ2ν)α1Tα(ϖ2ν)||σ||S1K2K3{x1+MS1S||x0+MS1K1M2(k+1)+S1K1M2(k+1)+S1C1βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)S1b0(bτ)α1hk(τ)dτ}dν+ϖ1ϵ0S1||AS1((ϖ2ν)α1Tα(ϖ2ν)(ϖ1ν)α1Tα(ϖ1ν))K2K3(×){x1+MS1S||x0+MS1K1M2(k+1)+S1K1M2(k+1)+S1C1βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)S1b0(bτ)α1hk(τ)dτ}dν+ϖ1ϖ1ϵS1||AS1((ϖ2ν)α1Tα(ϖ2ν)(ϖ1ν)α1Tα(ϖ1ν))K2K3(×){x1+MS1S||x0+MS1K1M2(k+1)+S1K1M2(k+1)+S1C1βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)S1b0(bτ)α1hk(τ)dτ}dν+ϖ2ϖ1S1||AS1((ϖ2ν)α1Tα(ϖ2ν))K2K3(×){x1+MS1S||x0+MS1K1M2(k+1)+S1K1M2(k+1)+S1C1βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)S1b0(bτ)α1hk(τ)dτ}dν+ϖ1ϵ0S1(ϖ2ν)α1Tα(ϖ2ν)(ϖ1ν)α1Tα(ϖ1ν)hk(ν)dν+ϖ1ϖ1ϵS1||(ϖ2ν)α1Tα(ϖ2ν)(ϖ1ν)α1Tα(ϖ1ν)hk(ν)dν+ϖ2ϖ1S1(ϖ2ν)α1Tα(ϖ2ν)hk(ν)dν.

    We check (P2x)(ϖ2)(P2x)(ϖ1) tends to zero independently of xBk when ϖ2ϖ1, with ϵ sufficiently small because of the compactness of Sα(ϖ), for ϖ>0 (see [34]) implies the continuity of Sα(ϖ) for ϖ>0 in ϖ in the uniform operator topology. We can verify that P2x,xBk is continuous at ϖ=0. Therefore, P2 maps Bk into a family of equicontinuous functions. We need to verify that V(ϖ)={(P2x)(ϖ):xBk} is relatively compact in Y. Assume that 0<ϖb be fixed, 0<ϵ<ϖ, for arbitrary δ>0, for xBk, we determine

    (Pϵ,δ2x)(ϖ)=δξα(θ)T(ϖαθ)S1Sx0dθ+αϖϵ0δθ(ϖν)α1ξα(θ)S1T((ϖν)αθ)σS1Bu(ν)dθdναϖϵ0δθ(ϖν)α1ξα(θ)S1T((ϖν)αθ)AS1Bu(ν)dθdν+αϖϵ0δθ(ϖν)α1ξα(θ)S1T((ϖν)αθ)G(ν,w(ν))dθdν=T(ϵαδ)δξα(θ)T(ϖαθϵαδ)S1Sx0dθ+αT(ϵαδ)ϖϵ0δθ(ϖν)α1ξα(θ)S1T((ϖν)αθϵαδ)σS1Bu(ν)dθdναT(ϵαδ)ϖϵ0δθ(ϖν)α1ξα(θ)S1T((ϖν)αθϵαδ)AS1Bu(ν)dθdν+αT(ϵαδ)ϖϵ0δθ(ϖν)α1ξα(θ)S1T((ϖν)αθϵαδ)G(ν,w(ν))dθdν.

    Because T(ϵαδ),ϵαδ>0 is compact, then Vϵ,δ(ϖ)={(Pϵ,δ2x)(ϖ):xBk} is relatively compact in Y for every ϵ,0<ϵ<ϖ and for all δ>0. Additionally, for each xBk, one can get

    (P2x)(ϖ)(Pϵ,δ2x)(ϖ)δ0ξα(θ)T(ϖαθ)S1Sx0dθ+αϖ0δ0θ(ϖν)α1ξα(θ)S1T((ϖν)αθ)σS1Bu(ν)dθdν+αϖ0δθ(ϖν)α1ξα(θ)S1T((ϖν)αθ)σS1Bu(ν)dθdνϖϵ0δθ(ϖν)α1ξα(θ)S1T((ϖν)αθ)σS1Bu(ν)dθdν+αϖ0δ0θ(ϖν)α1ξα(θ)S1T((ϖν)αθ)AS1Bu(ν)dθdν+αϖ0δθ(ϖν)α1ξα(θ)S1T((ϖν)αθ)AS1Bu(ν)dθdνϖϵ0δθ(ϖν)α1ξα(θ)S1T((ϖν)αθ)AS1Bu(ν)dθdν+αϖ0δ0θ(ϖν)α1ξα(θ)S1T((ϖν)αθ)G(ν,w(ν))dθdν+αϖ0δθ(ϖν)α1ξα(θ)S1T((ϖν)αθ)G(ν,w(ν))dθdνϖϵ0δθ(ϖν)α1ξα(θ)S1T((ϖν)αθ)G(ν,w(ν))dθdνδ0ξα(θ)T(ϖαθ)S1Sx0dθ+αϖ0δ0θ(ϖν)α1ξα(θ)S1T((ϖν)αθ)σS1Bu(ν)dθdν+αϖϖϵδθ(ϖν)α1ξα(θ)S1T((ϖν)αθ)σS1Bu(ν)dθdν+αϖ0δ0θ(ϖν)α1ξα(θ)S1T((ϖν)αθ)AS1Bu(ν)dθdν+αϖϖϵδθ(ϖν)α1ξα(θ)S1T((ϖν)αθ)AS1Bu(ν)dθdν+αϖ0δ0θ(ϖν)α1ξα(θ)S1T((ϖν)αθ)G(ν,w(ν))dθdν+αϖϖϵδθ(ϖν)α1ξα(θ)S1T((ϖν)αθ)G(ν,w(ν))dθdνMx0||S1Sδ0ξα(θ)dθ+αM(ϖ0(ϖν)α1σ||S1K2K3(×){x1+MS1S||x0+MS1K1M2(k+1)+S1K1M2(k+1)+S1C1βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)S1b0(bτ)α1hk(τ)dτ}dν)δ0θξα(θ)dθ+αM(ϖϖϵ(ϖν)α1σ||S1K2K3(×){x1+MS1S||x0+MS1K1M2(k+1)+S1K1M2(k+1)
    +S1C1βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)S1b0(bτ)α1hk(τ)dτ}dν)0θξα(θ)dθ+αM0(ϖ0(ϖν)α1K2K3(×){x1+MS1S||x0+MS1K1M2(k+1)+S1K1M2(k+1)+S1C1βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)S1b0(bτ)α1hk(τ)dτ}dν)δ0θξα(θ)dθ+αM0(ϖϖϵ(ϖν)α1K2K3(×){x1+MS1S||x0+MS1K1M2(k+1)+S1K1M2(k+1)+S1C1βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)S1b0(bτ)α1hk(τ)dτ}dν)0θξα(θ)dθ+S1αM(ϖ0(ϖν)α1hk(ν)dν)δ0θξα(θ)dθ+S1αM(ϖϖϵ(ϖν)α1hk(ν)dν)0θξα(θ)dθMx0||S1Sδ0ξα(θ)dθ+αM(ϖ0(ϖν)α1σ||S1K2K3(×){x1+MS1S||x0+MS1K1M2(k+1)+S1K1M2(k+1)+S1C1βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)S1b0(bτ)α1hk(τ)dτ}dν)δ0θξα(θ)dθ+αM(ϖϖϵ(ϖν)α1σ||S1K2K3(×){x1+MS1S||x0+MS1K1M2(k+1)+S1K1M2(k+1)+S1C1βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)S1b0(bτ)α1hk(τ)dτ}dν)+αM0(ϖ0(ϖν)α1K2K3(×){x1+MS1S||x0+MS1K1M2(k+1)+S1K1M2(k+1)+S1C1βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)S1b0(bτ)α1hk(τ)dτ}dν)δ0θξα(θ)dθ+αM0(ϖϖϵ(ϖν)α1K2K3(×){x1+MS1S||x0+MS1K1M2(k+1)+S1K1M2(k+1)+S1C1βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)S1b0(bτ)α1hk(τ)dτ}dν)+S1αM(ϖ0(ϖν)α1hk(ν)dν)δ0θξα(θ)dθ+S1αM(ϖϖϵ(ϖν)α1hk(ν)dν).

    Hence, there are relative compact sets arbitrary close to V(ϖ),ϖ>0. Therefore, V(ϖ),ϖ>0 is also relatively compact in Y. Consequently, with the help of Arzela-Ascoli theorem it can be say that P2 is compact. The above evidence demonstrates that P=P1+P2 is a condensing mapping on Bk, and by the Theorem 2.10, x() exists for P on Bk and the systems (2.1) and (2.2) have a mild solution.

    Remark 3.2. Many authors have recently investigated the boundary controllability of fractional evolution differential systems utilizing fractional theories, mild solutions, Caputo fractional derivatives, and fixed-point techniques. Very particularly, in [1,2,3,4,5], the authors discussed the existence and boundary controllability outcomes for integer and fractional order systems with and without delay by referring to multivalued functions, various fixed point theorems, fractional calculus, and nonlocal conditions. One can extend our current study to the integro-differential systems, Volterra-Fredholm integro-differential systems with integer and fractional order settings by using well-known fixed point theorems.

    Let us assume that Ω be a bounded, open subset of Rn. Consider Γ be a sufficiently smooth boundary of Ω. Assume that the following fractional differential system:

    cαϖ[(χ(ϖ,ν)Δχ(ϖ,ν))+F(ϖ,χ(ϖ,ν),χ(b1(ϖ),ν),,χ(bm(ϖ),ν))]=Δχ(ϖ,ν)+G(ϖ,χ(ϖ,ν),χ(a1(ϖ),ν),,χ(an(ϖ),ν))inQ=(0,b)×Ω,χ(ϖ,0)=u(ϖ,0), on Σ=(0,b)×Γ,ϖ[0,b],χ(ϖ,ν)=0,χ(0,ν)=χ0(ν),for νΩ.

    In the above, uL2(Σ), χ0L2(Δ), F,GL2(Q) and cαϖ is a Caputo fractional partial derivative of order 0<α<1. We can formulate the above problem as the boundary control problem (2.1) and (2.2) by suitably taking the space Y=Z=L2(Ω),X=H12(Γ),U=L2(Γ),B1=I. Now S:D(S)YZ given by S=Δ with D(S)=H2(Ω) and

    D(σ)={χL2(Ω):ΔχL2(Ω)},σχ=Δχ.

    The trace operator θ is well defined and expressed as θχ=χ|Γ and for χD(σ), θχH12(Γ) [24]. Define A:D(A)YZ in the following way: AS1=ΔS1 with D(AS1)=H10(Ω)H2(Ω). Here Hk(Ω),Hν(Ω) are the usual Sobolev space on Ω,Γ. Then, we introduce A and S in the following way:

    (i) A=p=1p2(,p)p,D(A), and S=p=1(1+p2)(,p)p,D(S).

    (ii) For every Y,

    A12=p=11p(,p)p.

    (iii) A12 is defined as follows:

    A12=p=1p(,p)p.

    On D(A12)={()Y;p=1p(,p)pY}, p(y)=2sinpν,p=1,2,3, be the orthogonal set of eigen vectors of A. Additionally, for Y.

    S1=p=111+p2(,p)p,AS1=p=1p21+p2(,p)p,T(ϖ)=p=1ep21+p2(,p)p.

    Clearly, AS1 generates a strongly continuous compact semigroup T(ϖ) with T(ϖ)M, for all ϖ0. To verify (A2) and (A3), we introduce B:L2(Γ)L2(Γ) by Bu=vu, vu is the unique solution to Δvu=0 in Ω, vu=u in Γ. We now define F and G in the following way:

    F(ϖ,x(ϖ),x(b1(ϖ)),,x(bm(ϖ)))=F(ϖ,χ(ϖ,ν),χ(b1(ϖ),ν),,χ(bm(ϖ),ν)),
    G(ϖ,x(ϖ),x(a1(ϖ)),,x(an(ϖ)))=G(ϖ,χ(ϖ,ν),χ(a1(ϖ),ν),,χ(an(ϖ),ν)).

    We conclude now F, G fulfill the hypotheses (A5) and (A6). Additionally, ˜W1 also exists. Assume b and the remaining constants fulfill the hypotheses (A5)(A7). Therefore, all the requirements of the Theorem (3.1) are fulfilled and (2.1) and (2.2) are controllable.

    In this article, we mainly focused on the boundary controllability of fractional order Sobolev-type neutral evolution equations in Banach space. We show our key results using facts from fractional calculus, semigroup theory, and the fixed point method. Finally, we give an example to illustrate the theory we have established. In the future, we will focus on the boundary controllability of Hilfer fractional-order neutral evolution equations and integrodifferential equations in Banach space by using the fixed point theorem approach.

    This research was supported by the National Research Foundation of Korea (NRF) grant funded by the Korea government (MSIT) (No. 2021R1F1A1048937) to the first author.

    This work does not have any conflict of interest.



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