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))),ϖ∈J=[0,b], | (2.1) |
Qx(ϖ)=B1u(ϖ),x(0)=x0. | (2.2) |
In the above, S:D(S)⊂Y→R(S)⊂Z is a linear operator, the control function u∈L2(J,U), a Banach space of admissible control function with U as a Banach space, B1:U→X is a linear continuous operator and ai,bj∈C(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 x∈Y, then (2.1) and (2.2) can be written as
cDα[y(ϖ)+F(ϖ,S−1y(ϖ),S−1y(b1(ϖ)),⋯,S−1y(bm(ϖ)))]=σS−1y(ϖ)+G(ϖ,S−1y(ϖ),S−1y(a1(ϖ)),⋯,S−1y(an(ϖ))),ϖ∈J=[0,b], | (2.3) |
˜Qy(ϖ)=B1u(ϖ),y(0)=y0, | (2.4) |
where ˜Q=QS−1:Z→X is a linear operator. The operator A:Y→Z given by
D(AS−1)={w∈D(σS−1):˜Qw=0}, |
AS−1w=σS−1w for w∈D(AS−1), (see [4,23]).
Definition 2.1. [4,23] The operators A:D(A)⊂Y→Z and S:D(S)⊂Y→Z satisfying the following hypotheses:
(H1)A and S are closed linear operators.
(H2)D(S)⊂D(A) and S is bijective.
(H3)S−1:Z→D(S) is continuous.
The hypothesis (H1)–(H3) and the closed graph theorem imply the boundedness of the linear operator AS−1:Z→Z and AS−1 generates an analytic compact semigroup of uniformly bounded linear operators {T(ϖ):ϖ≥0}. This means that there exists a M≥1 such that ‖T(ϖ)‖≤M. Without loss of generality, we assume that 0∈λ(AS−1). 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 ‖x‖q=‖(−A)qx‖,x∈Y.
(2) T(ϖ):Y→Yq for each (−A)qT(ϖ)x=T(ϖ)(−A)qx, for all x∈Yq and ϖ≥0.
(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<q≤1, then D(−A)q↪D(−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)=1Γα∫ϖ0f(ν)dν(ϖ−ν)1−α,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(n−α)∫ϖ0f(n)(ν)dν(ϖ−ν)α+1−n=In−αf(n)(ϖ), ϖ>0,0≤n−1<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:U→Z such that σS−1B∈L(U,Z), ˜Q(Bu)=B1u,for allu∈U. Also Bu(ϖ) is continuously differentiable and
‖(−A)βBu‖≤C‖B1u‖, |
for all u∈U, where C is a constant.
(A3) For all ϖ∈(0,b] and u∈U, T(ϖ)Bu∈D(AS−1). Moreover, there exists a positive function M0>0 such that ‖AS−1T(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(AS−1). Hence, the systems (2.3) and (2.4) can be written in terms of A and B as
cDα[z(ϖ)+F(ϖ,S−1y(ϖ),S−1y(b1(ϖ)),⋯,S−1y(bm(ϖ)))]=AS−1z(ϖ)+σS−1Bu(ϖ)−BcDαu(ϖ)+G(ϖ,S−1y(ϖ),S−1y(a1(ϖ)),⋯,S−1y(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,S−1y(0),S−1y(b1(0)),⋯,S−1y(bm(0)))]−F(ϖ,S−1y(ϖ),S−1y(b1(ϖ)),⋯,S−1y(bm(ϖ)))]+1Γα∫ϖ0S−1Ay(ν)dν(ϖ−ν)1−α−1Γα∫ϖ0S−1ABu(ν)dν(ϖ−ν)1−α+1Γα∫ϖ0S−1σBu(ν)dν(ϖ−ν)1−α+1Γα∫ϖ0G(ν,S−1y(ν),S−1y(a1(ν)),⋯,S−1y(an(ν)))dν(ϖ−ν)1−α, | (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)=S−1Sα(ϖ)Sx(0)+S−1Sα(ϖ)F(0,x(0),x(b1(0)),⋯,x(bm(0)))−S−1F(ϖ,x(ϖ),x(b1(ϖ)),⋯,x(bm(ϖ)))−∫ϖ0(ϖ−ν)α−1ATα(ϖ−ν)S−1F(ν,x(ν),x(b1(ν)),⋯,x(bm(ν)))dν+∫ϖ0S−1(ϖ−ν)α−1[Tα(ϖ−ν)σS−1B−AS−1Tα(ϖ−ν)B]u(ν)dν+∫ϖ0S−1(ϖ−ν)α−1Tα(ϖ−ν)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=α∫∞0θξα(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,x1∈Y, there exists a control u∈L2(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 x∈Y, ‖Sα(ϖ)x‖≤M‖x‖, ‖Tα(ϖ)x‖≤αM‖x‖Γ(α+1).
(ii) {Sα(ϖ),ϖ≥0} and {Tα(ϖ),ϖ≥0} are strongly continuous.
(iii) For all ϖ≥0,Sα(ϖ) and Tα(ϖ) are also compact operators.
(iv) For any x∈Y,β∈(0,1) and δ∈(0,1), we have
(−A)Tα(ϖ)x=(−A)1−βTα(ϖ)(−A)βx, |
and
‖(−A)δTα(ϖ)‖≤αCδΓ2−δϖαδΓ1+α(1−δ),ϖ∈(0,b). |
Remark 2.9. For any x∈Y,β∈(0,1) and δ=1, we have
‖ATα(ϖ)x‖=α‖∫∞0θξα(θ)AT(ϖαθ)xdθ‖=α‖x‖M0Γ(1+α). |
Further, assume the following assumptions:
(A4) The linear operator W from L2(J,U) into Y is given by
Wu=∫b0S−1(b−ν)α−1[Tα(b−ν)σS−1B−AS−1Tα(b−ν)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)β≤K1,0<β≤1,‖B‖≤K2 and ‖˜W−1‖≤K3.
(A5) F:J×Ym+1→Y 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(|ν1−ν2|+maxi=0,1,⋯,m‖xi−yi‖), |
for 0≤ν1,ν2≤b, xi,yi∈Y,i=0,1,⋯,m and
‖(−A)βF(ϖ,x0,x1,⋯,xm)‖≤M2(maxi=0,1,⋯,m‖xi‖+1), | (2.9) |
holds for (ϖ,x0,x1,⋯,xm)∈J×Ym+1.
(A6) G:J×Yn+1→Y fulfill the subsequent conditions:
(i) For every ϖ∈J, G(ϖ,⋅):Yn+1→Y is continuous and for every (x0,x1,⋯,xn)∈Yn+1, G(⋅,x0,x1,⋯,xn):J→Y is strongly measurable.
(ii) For every k∈N, there exists hk(⋅):[0,b]→R+ such that
sup‖x0‖,⋯,‖xn‖≤k‖G(ϖ,x0,x1,⋯,xn)‖≤hk(ϖ), |
S→(ϖ−ν)1−αhk(ν)∈L1([0,ϖ],R+) |
and there exists ⋀>0 such that
limk→∞inf∫ϖ0(ϖ−ν)1−αhk(ν)dνk=⋀<∞,ϖ∈[0,b]. |
(A7) We assume
L∗=‖S−1‖M1[(M+1)K1+C1−βΓ(1+β)bαββΓ(1+αβ)<1, | (2.10) |
[M‖S−1‖K1M2+‖S−1‖K1M2+‖S−1‖C1−βΓ(1+β)bαβM2βΓ(1+αβ)+‖S−1‖αMΓ(1+α)⋀](×)(1+[‖S−1‖2‖σ‖bαMΓ(1+α)+‖S−1‖bαM0Γ(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)=˜W−1[x1−S−1Sα(b)Sx0−S−1Sα(b)F(0,v(0))+S−1F(b,v(b))+∫b0(b−ν)α−1ATα(b−ν)S−1F(ν,v(ν))dν−∫b0S−1(b−ν)α−1Tα(b−ν)G(ν,w(ν))dν](ϖ). |
We now define P as follows:
(Px)(ϖ)=S−1Sα(ϖ)Sx(0)+S−1Sα(ϖ)F(0,v(0))−S−1F(ϖ,v(ϖ))−∫ϖ0(ϖ−ν)α−1ATα(ϖ−ν)S−1F(ν,v(ν))dν+∫ϖ0S−1(ϖ−ν)α−1Tα(ϖ−ν)σS−1Bu(ν)dν−∫ϖ0S−1(ϖ−ν)α−1AS−1Tα(ϖ−ν)Bu(ν)dν+∫ϖ0S−1(ϖ−ν)α−1Tα(ϖ−ν)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={x∈Y:‖x(ϖ)‖≤k,0≤ϖ≤b}. |
Then for every k, Bk is clearly a bounded closed convex set in Y. From Lemma 2.8 and Eq (2.9) yields
‖∫ϖ0(ϖ−ν)α−1ATα(ϖ−ν)S−1F(ν,v(ν))dν‖≤∫ϖ0‖(ϖ−ν)α−1S−1(−A)1−βTα(ϖ−ν)(−A)βF(ν,v(ν))‖dν≤‖S−1‖αC1−βΓ(1+β)Γ(1+αβ)∫ϖ0(ϖ−ν)αβ−1(−A)βF(ν,v(ν))dν≤C1−βΓ(1+β)‖S−1‖bαβM2Γ(1+αβ)[maxi=1,2,⋯,m‖xi‖+1]≤‖S−1‖C1−βΓ(1+β)βΓ(1+αβ)bαβ(k+1)M2, |
then it follows that (ϖ−ν)α−1ATα(ϖ−ν)S−1F(ν,v(ν)) is integrable on J, by Lemma (2.5), P is well defined on Bk. From (A6)(ii), one can get
‖∫ϖ0S−1(ϖ−ν)α−1Tα(ϖ−ν)G(ν,w(ν))dν‖≤∫ϖ0‖S−1(ϖ−ν)α−1Tα(ϖ−ν)G(ν,w(ν))‖dν≤‖S−1‖αMΓ(α+1)∫ϖ0(ϖ−ν)α−1‖G(ν,w(ν))‖dν≤‖S−1‖αMΓ(α+1)∫ϖ0(ϖ−ν)α−1hk(ν)dν. |
We conclude that for k>0 such that PBk⊆Bk. If it fails, then there exist a function xk(⋅)∈Bk but PBk⊈Bk, 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)‖≤‖S−1Sα(ϖ)Sx(0)+S−1Sα(ϖ)F(0,vk(0))−S−1F(ϖ,vk(ϖ))−∫ϖ0(ϖ−ν)α−1ATα(ϖ−ν)S−1F(ν,vk(ν))dν+∫ϖ0S−1(ϖ−ν)α−1[Tα(ϖ−ν)σS−1−AS−1Tα(ϖ−ν)]B˜W−1(×){x1−S−1Sα(b)Sx(0)−S−1Sα(b)F(0,vk(0))+S−1F(b,vk(b))+∫b0(b−τ)α−1ATα(b−τ)S−1F(τ,vk(τ))dν−∫b0S−1(b−τ)α−1Tα(b−τ)G(τ,wk(τ))dτ}(ν)dν+∫ϖ0S−1(ϖ−ν)α−1Tα(ϖ−ν)G(ν,wk(ν))dν‖≤M‖S−1‖‖S‖||x0‖+M‖S−1‖||(−A)−β(−A)βF(0,vk(0))‖+‖S−1‖||(−A)−β(−A)βF(ϖ,vk(ϖ))‖+‖S−1‖C1−βΓ(1+β)βΓ(1+αβ)bαβ(k+1)M2+∫ϖ0‖S−1‖(ϖ−ν)α−1[‖σ‖||S−1‖||Tα(ϖ−ν)‖+‖AS−1Tα(ϖ−ν)‖](×)‖B‖‖˜W−1‖{‖x1‖+M‖S−1‖‖S‖||x0‖+M‖S−1‖||(−A)−β(−A)βF(0,vk(0))‖+‖S−1‖||(−A)−β(−A)βF(b,vk(b))‖+‖S−1‖C1−βΓ(1+β)βΓ(1+αβ)bαβ(k+1)M2+∫b0‖S−1‖(b−τ)α−1‖Tα(b−τ)‖||G(τ,wk(τ))‖dτ}dν+∫ϖ0‖S−1‖(ϖ−ν)α−1‖Tα(ϖ−ν)‖||G(ν,wk(ν))‖dν≤M‖S−1‖‖S‖||x0‖+M‖S−1‖K1M2(k+1)+‖S−1‖K1M2(k+1)+‖S−1‖C1−βΓ(1+β)bαβ(k+1)βΓ(1+αβ)M2+‖S−1‖bαα[‖σ‖||S−1‖αMΓ(α+1)+αM0Γ(α+1)]K2K3(×){‖x1‖+M‖S−1‖‖S‖||x0‖+M‖S−1‖K1M2(k+1)+‖S−1‖K1M2(k+1)+‖S−1‖C1−βΓ(1+β)βΓ(1+αβ)bαβ(k+1)M2+αMΓ(α+1)‖S−1‖∫b0(b−τ)α−1hk(τ)dτ}+αMΓ(α+1)‖S−1‖∫ϖ0(ϖ−ν)α−1hk(ν)dν. |
Dividing by k on both sides of the above inequality and letting k→+∞, one can get
1≤M‖S−1‖K1M2+‖S−1‖K1M2+‖S−1‖C1−βΓ(1+β)βΓ(1+αβ)bαβM2+‖S−1‖bαα[‖σ‖||S−1‖αMΓ(α+1)+αM0Γ(α+1)]K2K3(M‖S−1‖K1M2+‖S−1‖K1M2+‖S−1‖C1−βΓ(1+β)βΓ(1+αβ)bαβM2+αMΓ(α+1)‖S−1‖⋀)+‖S−1‖αMΓ(α+1)⋀. |
Therefore,
[M‖S−1‖K1M2+‖S−1‖K1M2+‖S−1‖C1−βΓ(1+β)βΓ(1+αβ)bαβM2+‖S−1‖αMΓ(α+1)⋀](1+[‖S−1‖2‖σ‖bαMΓ(1+α)+‖S−1‖bαM0Γ(1+α)]K2K3)≥1. |
The above equation contradicts Eq (2.11). Thus, for k>0, PBk⊆Bk. 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)=S−1Sα(ϖ)F(0,v(0))−S−1F(ϖ,v(ϖ))−∫ϖ0(ϖ−ν)α−1ATα(ϖ−ν)S−1F(ν,v(ν))dν, |
and
(P2x)(ϖ)=S−1Sα(ϖ)Sx0+∫ϖ0S−1(ϖ−ν)α−1[Tα(ϖ−ν)σS−1−AS−1Tα(ϖ−ν)]Bu(ν)dν+∫ϖ0S−1(ϖ−ν)α−1Tα(ϖ−ν)G(ν,w(ν))dν, |
for 0≤ϖ≤b. We have to verify P1 is a contraction mapping if P2 is compact. For checking P1 fulfills the contraction condition, we assume x1,x2∈Bk. Then, for every ϖ∈J and by hypothesis (A5) and Eq (2.10), one can get
‖(P1x1)(ϖ)−(P1x2)(ϖ)‖≤‖S−1Sα(ϖ)[F(0,v1(0))−F(0,v2(0))‖+‖S−1[F(ϖ,v1(ϖ))−F(ϖ,v2(ϖ))]‖+‖∫ϖ0S−1(ϖ−ν)α−1ATα(ϖ−ν)[F(ν,v1(ν))−F(ν,v2(ν))]dν‖≤‖S−1‖MK1M1sup0≤ν≤b‖x1(ν)−x2(ν)‖+‖S−1‖K1M1sup0≤ν≤b‖x1(ν)−x2(ν)‖+‖S−1‖bαβC1−βΓ(1+β)βΓ(1+αβ)M1sup0≤ν≤b‖x1(ν)−x2(ν)‖. |
Hence
‖(P1x1)(ϖ)−(P1x2)(ϖ)‖≤‖S−1‖M1[(M+1)K1+C1−βΓ(1+β)βΓ(1+αβ)bαβ]sup0≤ν≤b‖x1(ν)−x2(ν)‖. |
Thus,
‖(P1x1)(ϖ)−(P1x2)(ϖ)‖≤L∗sup0≤ν≤b‖x1(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 xn→x in Bk, then for every ν∈J, 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
‖P2xn−P2x‖=sup0≤ϖ≤b‖∫ϖ0S−1(ϖ−ν)α−1(Tα(ϖ−ν)σS−1−AS−1Tα(ϖ−ν))B[wn(ν)−w(ν)]dν+∫ϖ0S−1(ϖ−ν)α−1Tα(ϖ−ν)[G(ν,wn(ν))−G(ν,w(ν))]dν‖→0, |
when n→∞, i.e., P2 is continuous. Now, we need to verify {P2x:x∈Bk} is an equicontinuous family of functions. For this, we assume ϵ>0 be small, 0<ϖ1<ϖ2, then
‖(P2x)(ϖ2)−(P2x)(ϖ1)‖≤‖S−1‖||Sα(ϖ2)−Sα(ϖ1)‖||x0‖+∫ϖ1−ϵ0‖S−1‖||((ϖ2−ν)α−1Tα(ϖ2−ν)−(ϖ1−ν)α−1Tα(ϖ1−ν))σS−1Bu(ν)‖dν+∫ϖ1ϖ1−ϵ‖S−1‖||((ϖ2−ν)α−1Tα(ϖ2−ν)−(ϖ1−ν)α−1Tα(ϖ1−ν))S−1σBu(ν)‖dν+∫ϖ2ϖ1‖S−1‖||((ϖ2−ν)α−1Tα(ϖ2−ν))S−1σBu(ν)‖dν+∫ϖ1−ϵ0‖S−1‖||AS−1((ϖ2−ν)α−1Tα(ϖ2−ν)−(ϖ1−ν)α−1Tα(ϖ1−ν))Bu(ν)‖dν+∫ϖ1ϖ1−ϵ‖S−1‖||AS−1((ϖ2−ν)α−1Tα(ϖ2−ν)−(ϖ1−ν)α−1Tα(ϖ1−ν))Bu(ν)‖dν+∫ϖ2ϖ1‖S−1‖||AS−1((ϖ2−ν)α−1Tα(ϖ2−ν))Bu(ν)‖dν+∫ϖ1−ϵ0‖S−1‖||(ϖ2−ν)α−1Tα(ϖ2−ν)−(ϖ1−ν)α−1Tα(ϖ1−ν)‖||G(ν,w(ν))‖dν+∫ϖ1ϖ1−ϵ‖S−1‖||(ϖ2−ν)α−1Tα(ϖ2−ν)−(ϖ1−ν)α−1Tα(ϖ1−ν)‖||G(ν,w(ν))‖dν+∫ϖ2ϖ1‖S−1‖||(ϖ2−ν)α−1Tα(ϖ2−ν)‖||G(ν,w(ν))‖dν. |
Observe that
‖u(ν)‖≤K3{‖x1‖+M‖S−1‖‖S‖||x0‖+M‖S−1‖K1M2(k+1)+‖S−1‖K1M2(k+1)+‖S−1‖C1−βΓ(1+β)bαβ(k+1)βΓ(1+αβ)M2+αMΓ(α+1)‖S−1‖∫b0(b−τ)α−1hk(τ)dτ}. |
We see that
‖(P2x)(ϖ2)−(P2x)(ϖ1)‖≤‖S−1‖||Sα(ϖ2)−Sα(ϖ1)‖||x0‖+∫ϖ1−ϵ0‖S−1‖||(ϖ2−ν)α−1Tα(ϖ2−ν)−(ϖ1−ν)α−1Tα(ϖ1−ν)‖||σ‖||S−1‖K2(×)K3{‖x1‖+M‖S−1‖‖S‖||x0‖+M‖S−1‖K1M2(k+1)+‖S−1‖K1M2(k+1)+‖S−1‖C1−βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)‖S−1‖∫b0(b−τ)α−1hk(τ)dτ}dν+∫ϖ1ϖ1−ϵ‖S−1‖||(ϖ2−ν)α−1Tα(ϖ2−ν)−(ϖ1−ν)α−1Tα(ϖ1−ν)‖||σ‖||S−1‖K2K3(×){‖x1‖+M‖S−1‖‖S‖||x0‖+M‖S−1‖K1M2(k+1)+‖S−1‖K1M2(k+1)+‖S−1‖C1−βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)‖S−1‖∫b0(b−τ)α−1hk(τ)dτ}dν+∫ϖ2ϖ1‖S−1‖||(ϖ2−ν)α−1Tα(ϖ2−ν)‖||σ‖||S−1‖K2K3{‖x1‖+M‖S−1‖‖S‖||x0‖+M‖S−1‖K1M2(k+1)+‖S−1‖K1M2(k+1)+‖S−1‖C1−βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)‖S−1‖∫b0(b−τ)α−1hk(τ)dτ}dν+∫ϖ1−ϵ0‖S−1‖||AS−1((ϖ2−ν)α−1Tα(ϖ2−ν)−(ϖ1−ν)α−1Tα(ϖ1−ν))K2K3(×){‖x1‖+M‖S−1‖‖S‖||x0‖+M‖S−1‖K1M2(k+1)+‖S−1‖K1M2(k+1)+‖S−1‖C1−βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)‖S−1‖∫b0(b−τ)α−1hk(τ)dτ}dν+∫ϖ1ϖ1−ϵ‖S−1‖||AS−1((ϖ2−ν)α−1Tα(ϖ2−ν)−(ϖ1−ν)α−1Tα(ϖ1−ν))K2K3(×){‖x1‖+M‖S−1‖‖S‖||x0‖+M‖S−1‖K1M2(k+1)+‖S−1‖K1M2(k+1)+‖S−1‖C1−βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)‖S−1‖∫b0(b−τ)α−1hk(τ)dτ}dν+∫ϖ2ϖ1‖S−1‖||AS−1((ϖ2−ν)α−1Tα(ϖ2−ν))K2K3(×){‖x1‖+M‖S−1‖‖S‖||x0‖+M‖S−1‖K1M2(k+1)+‖S−1‖K1M2(k+1)+‖S−1‖C1−βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)‖S−1‖∫b0(b−τ)α−1hk(τ)dτ}dν+∫ϖ1−ϵ0‖S−1‖‖(ϖ2−ν)α−1Tα(ϖ2−ν)−(ϖ1−ν)α−1Tα(ϖ1−ν)‖hk(ν)dν+∫ϖ1ϖ1−ϵ‖S−1‖||(ϖ2−ν)α−1Tα(ϖ2−ν)−(ϖ1−ν)α−1Tα(ϖ1−ν)‖hk(ν)dν+∫ϖ2ϖ1‖S−1‖‖(ϖ2−ν)α−1Tα(ϖ2−ν)‖hk(ν)dν. |
We check ‖(P2x)(ϖ2)−(P2x)(ϖ1)‖ tends to zero independently of x∈Bk when ϖ2→ϖ1, 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,x∈Bk is continuous at ϖ=0. Therefore, P2 maps Bk into a family of equicontinuous functions. We need to verify that V(ϖ)={(P2x)(ϖ):x∈Bk} is relatively compact in Y. Assume that 0<ϖ≤b be fixed, 0<ϵ<ϖ, for arbitrary δ>0, for x∈Bk, we determine
(Pϵ,δ2x)(ϖ)=∫∞δξα(θ)T(ϖαθ)S−1Sx0dθ+α∫ϖ−ϵ0∫∞δθ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)σS−1Bu(ν)dθdν−α∫ϖ−ϵ0∫∞δθ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)AS−1Bu(ν)dθdν+α∫ϖ−ϵ0∫∞δθ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)G(ν,w(ν))dθdν=T(ϵαδ)∫∞δξα(θ)T(ϖαθ−ϵαδ)S−1Sx0dθ+αT(ϵαδ)∫ϖ−ϵ0∫∞δθ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ−ϵαδ)σS−1Bu(ν)dθdν−αT(ϵαδ)∫ϖ−ϵ0∫∞δθ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ−ϵαδ)AS−1Bu(ν)dθdν+αT(ϵαδ)∫ϖ−ϵ0∫∞δθ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ−ϵαδ)G(ν,w(ν))dθdν. |
Because T(ϵαδ),ϵαδ>0 is compact, then Vϵ,δ(ϖ)={(Pϵ,δ2x)(ϖ):x∈Bk} is relatively compact in Y for every ϵ,0<ϵ<ϖ and for all δ>0. Additionally, for each x∈Bk, one can get
‖(P2x)(ϖ)−(Pϵ,δ2x)(ϖ)‖≤‖∫δ0ξα(θ)T(ϖαθ)S−1Sx0dθ‖+α‖∫ϖ0∫δ0θ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)σS−1Bu(ν)dθdν‖+α‖∫ϖ0∫∞δθ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)σS−1Bu(ν)dθdν−∫ϖ−ϵ0∫∞δθ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)σS−1Bu(ν)dθdν‖+α‖∫ϖ0∫δ0θ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)AS−1Bu(ν)dθdν‖+α‖∫ϖ0∫∞δθ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)AS−1Bu(ν)dθdν−∫ϖ−ϵ0∫∞δθ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)AS−1Bu(ν)dθdν‖+α‖∫ϖ0∫δ0θ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)G(ν,w(ν))dθdν‖+α‖∫ϖ0∫∞δθ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)G(ν,w(ν))dθdν−∫ϖ−ϵ0∫∞δθ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)G(ν,w(ν))dθdν‖≤‖∫δ0ξα(θ)T(ϖαθ)S−1Sx0dθ‖+α‖∫ϖ0∫δ0θ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)σS−1Bu(ν)dθdν‖+α‖∫ϖϖ−ϵ∫∞δθ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)σS−1Bu(ν)dθdν‖+α‖∫ϖ0∫δ0θ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)AS−1Bu(ν)dθdν‖+α‖∫ϖϖ−ϵ∫∞δθ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)AS−1Bu(ν)dθdν‖+α‖∫ϖ0∫δ0θ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)G(ν,w(ν))dθdν‖+α‖∫ϖϖ−ϵ∫∞δθ(ϖ−ν)α−1ξα(θ)S−1T((ϖ−ν)αθ)G(ν,w(ν))dθdν‖≤M‖x0‖||S−1‖‖S‖∫δ0ξα(θ)dθ+αM(∫ϖ0(ϖ−ν)α−1‖σ‖||S−1‖K2K3(×){‖x1‖+M‖S−1‖‖S‖||x0‖+M‖S−1‖K1M2(k+1)+‖S−1‖K1M2(k+1)+‖S−1‖C1−βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)‖S−1‖∫b0(b−τ)α−1hk(τ)dτ}dν)∫δ0θξα(θ)dθ+αM(∫ϖϖ−ϵ(ϖ−ν)α−1‖σ‖||S−1‖K2K3(×){‖x1‖+M‖S−1‖‖S‖||x0‖+M‖S−1‖K1M2(k+1)+‖S−1‖K1M2(k+1) |
+‖S−1‖C1−βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)‖S−1‖∫b0(b−τ)α−1hk(τ)dτ}dν)∫∞0θξα(θ)dθ+αM0(∫ϖ0(ϖ−ν)α−1K2K3(×){‖x1‖+M‖S−1‖‖S‖||x0‖+M‖S−1‖K1M2(k+1)+‖S−1‖K1M2(k+1)+‖S−1‖C1−βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)‖S−1‖∫b0(b−τ)α−1hk(τ)dτ}dν)∫δ0θξα(θ)dθ+αM0(∫ϖϖ−ϵ(ϖ−ν)α−1K2K3(×){‖x1‖+M‖S−1‖‖S‖||x0‖+M‖S−1‖K1M2(k+1)+‖S−1‖K1M2(k+1)+‖S−1‖C1−βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)‖S−1‖∫b0(b−τ)α−1hk(τ)dτ}dν)∫∞0θξα(θ)dθ+‖S−1‖αM(∫ϖ0(ϖ−ν)α−1hk(ν)dν)∫δ0θξα(θ)dθ+‖S−1‖αM(∫ϖϖ−ϵ(ϖ−ν)α−1hk(ν)dν)∫∞0θξα(θ)dθ≤M‖x0‖||S−1‖‖S‖∫δ0ξα(θ)dθ+αM(∫ϖ0(ϖ−ν)α−1‖σ‖||S−1‖K2K3(×){‖x1‖+M‖S−1‖‖S‖||x0‖+M‖S−1‖K1M2(k+1)+‖S−1‖K1M2(k+1)+‖S−1‖C1−βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)‖S−1‖∫b0(b−τ)α−1hk(τ)dτ}dν)∫δ0θξα(θ)dθ+αM(∫ϖϖ−ϵ(ϖ−ν)α−1‖σ‖||S−1‖K2K3(×){‖x1‖+M‖S−1‖‖S‖||x0‖+M‖S−1‖K1M2(k+1)+‖S−1‖K1M2(k+1)+‖S−1‖C1−βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)‖S−1‖∫b0(b−τ)α−1hk(τ)dτ}dν)+αM0(∫ϖ0(ϖ−ν)α−1K2K3(×){‖x1‖+M‖S−1‖‖S‖||x0‖+M‖S−1‖K1M2(k+1)+‖S−1‖K1M2(k+1)+‖S−1‖C1−βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)‖S−1‖∫b0(b−τ)α−1hk(τ)dτ}dν)∫δ0θξα(θ)dθ+αM0(∫ϖϖ−ϵ(ϖ−ν)α−1K2K3(×){‖x1‖+M‖S−1‖‖S‖||x0‖+M‖S−1‖K1M2(k+1)+‖S−1‖K1M2(k+1)+‖S−1‖C1−βΓ(1+β)bαβ(k+1)M2βΓ(1+αβ)+αMΓ(α+1)‖S−1‖∫b0(b−τ)α−1hk(τ)dτ}dν)+‖S−1‖αM(∫ϖ0(ϖ−ν)α−1hk(ν)dν)∫δ0θξα(θ)dθ+‖S−1‖αM(∫ϖϖ−ϵ(ϖ−ν)α−1hk(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:
c∂αϖ[(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 ν∈Ω. |
In the above, u∈L2(Σ), χ0∈L2(Δ), F,G∈L2(Q) and c∂αϖ 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=H−12(Γ),U=L2(Γ),B1=I. Now S:D(S)⊂Y→Z given by Sℏ=ℏ−Δℏ with D(S)=H2(Ω) and
D(σ)={χ∈L2(Ω):Δχ∈L2(Ω)},σχ=Δχ. |
The trace operator θ is well defined and expressed as θχ=χ|Γ and for χ∈D(σ), θχ∈H−12(Γ) [24]. Define A:D(A)⊂Y→Z in the following way: AS−1ℏ=ΔS−1ℏ with D(AS−1)=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) Aℏ=∑∞p=1p2(ℏ,ℏp)ℏp,ℏ∈D(A), and Sℏ=∑∞p=1(1+p2)(ℏ,ℏp)ℏp,ℏ∈D(S).
(ii) For every ℏ∈Y,
A−12ℏ=∞∑p=11p(ℏ,ℏp)ℏp. |
(iii) A12 is defined as follows:
A12=∞∑p=1p(ℏ,ℏp)ℏp. |
On D(A12)={ℏ(⋅)∈Y;∑∞p=1p(ℏ,ℏp)ℏp∈Y}, ℏp(y)=√2sinpν,p=1,2,3,⋯ be the orthogonal set of eigen vectors of A. Additionally, for ℏ∈Y.
S−1ℏ=∞∑p=111+p2(ℏ,ℏp)ℏp,AS−1ℏ=∞∑p=1p21+p2(ℏ,ℏp)ℏp,T(ϖ)ℏ=∞∑p=1ep21+p2(ℏ,ℏp)ℏp. |
Clearly, AS−1 generates a strongly continuous compact semigroup T(ϖ) with ‖T(ϖ)‖≤M, for all ϖ≥0. 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, ˜W−1 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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