Research article

Study on a semilinear fractional stochastic system with multiple delays in control

  • Received: 19 February 2022 Revised: 04 April 2022 Accepted: 12 April 2022 Published: 25 April 2022
  • MSC : 34K35, 34K50, 93B05, 93E20

  • This paper studies a semilinear fractional stochastic differential equation with multiple constant point delays in control. We transform the controllability problem into a fixed point problem. We obtain sufficient condition for the controllability by using Schauder's fixed point theorem. In addition, we discuss the optimal controllability of the problem. Some examples are given to illustrate the main result.

    Citation: Abdur Raheem, Maryam G. Alshehri, Asma Afreen, Areefa Khatoon, Musaad S. Aldhabani. Study on a semilinear fractional stochastic system with multiple delays in control[J]. AIMS Mathematics, 2022, 7(7): 12374-12389. doi: 10.3934/math.2022687

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  • This paper studies a semilinear fractional stochastic differential equation with multiple constant point delays in control. We transform the controllability problem into a fixed point problem. We obtain sufficient condition for the controllability by using Schauder's fixed point theorem. In addition, we discuss the optimal controllability of the problem. Some examples are given to illustrate the main result.



    Consider the stochastic fractional differential equation with several delays in control:

    {CDαtz(t)=Az(t)+rq=0Equ(tηq)+ϱ1(t,z(t),rq=0u(tηq))+ϱ2(t,z(t),rq=0u(tηq))dυ(t)dt,t[0,],z(0)=z0,z(0)=z1,u(t)=0,t[ηr,0], (1.1)

    where 1<α<2 and CDαt is the standard Caputo fractional derivative of order α. Let Z and W be separable Hilbert spaces such that the state function z(t)Z. The operator A generates a strongly continuous α-order fractional cosine family {Cα(t):t0} in Z. Let υ be a W-valued Weiner process with a finite trace nuclear covariance operator Q0 on a complete probability space (Ω,Υ,P), where ΥtΥ, t[0,] is a normal filtration. Υt is a right continuous increasing family and Υ0 contains all P-null sets. Also, let L02=L2(Q1/2W,Z), the space of all Hilbert-Schmidt operators from Q1/2W to Z be a separable Hilbert space with the norm ψ2Q=tr[ψQψ]. Let the control function u takes value in a separable and reflexive Hilbert space U and EqL(U,Z),q=0,1,2,,r are linear continuous operators and 0=η0<η1<η2<<ηq<<ηr1<ηr are delay points. For convenience, let u()Uad=LpΥ([0,],U), where Uad denotes the set of admissible control functions which is closed and convex. ϱq,q=1,2 are nonlinear functions that satisfy some suitable conditions which will be specified later. z0 and z1 denote Υ0-measurable Z-valued random variables.

    Let C([0,],Lp(Υ,Z)) be the Banach space of continuous maps defined on [0,] into Lp(Υ,Z) such that

    supt[0,]Ez(t)pZ<,

    where Lp(Υ,Z) denotes the Banach space of all Z valued, p-integrable and Υ-measurable random variables and E is the expectation given by E(z)=Ωz(υ)dP. Take C2=Cp([0,],Z), then C2 is a closed subspace of C([0,],Lp(Υ,Z)) endowed with the norm

    zC2=(supt[0,]Ez(t)pZ)1p.

    Classical differential equations cannot adequately describe more and more phenomena as science and technology advance. Various physical processes, for example, have memory and heritability properties that the classical local differential operators cannot adequately represent. Many well-known mathematicians such as Euler, Liouville, Riemann, Caputo and Letnikov developed a new excellent tool to describe these nonlocal processes (fractional differential equations described by nonlocal operators) [13,19]. In recent years, it has turned out that many phenomena in viscoelastic polymers, fluid mechanics, foams and animal tissues can be successfully modeled by fractional order derivatives.

    The development of Fractional calculus theory is due to the significant contributions of many mathematicians such as Euler, Liouville, Riemann and Letnikov. The fractional theory deals with arbitrary order derivatives or integrals. Fractional calculus is an influential tool that plays an essential role in studying non-integer parametric models. Also, it emerges a significant role to specify bio-system, neuroscience, drug diffusion in the human body, fractional biological neurons, frequency-modulated systems, chemical technology and many real-life phenomena. Fractional integrals and derivatives also appear in control dynamical systems. Fractional differential equations describe many natural processes and phenomena studied in biotechnology, electric circuits, engineering science, optimal control, porous media, economics, etc. A comprehensive study of fractional calculus is essential and is now well-established. For the basic theory of fractional calculus and applications in control theory, refer to [2,12,33].

    Noise and stochastic distress are so common in natural and man-made systems that they cannot be avoided. Furthermore, some randomness may appear. As a result, stochastic models are being considered for improved performance and are becoming more important tools for formulating and analyzing phenomena. In 1940, Kiyosi Ito, a Japanese mathematician, pioneered the mathematical theory of stochastic differential equations.

    Many real dynamical systems have a fundamental feature of uncertainty. The theory of stochastic dynamical systems is now a well-established area of study that is still in active development and has many unresolved issues. Statistical physics, economic problems, decision problems, epidemiology, insurance mathematics, risk theory, reliability theory and other stochastic equation-based methods are important fields of applications. For more information on the fundamental theory of stochastic differential equations, see [20]. The control theory is used to study a wide range of stochastic systems. These papers [6,24,25,31] show the fascinating property of such dynamical systems.

    Many mathematicians, physicists and engineers have been drawn to control problems and significant contributions to theory and applications have been made. R. E. Kalman began systematically developing controllability theory in 1963. The fundamental concepts of controllability are described in Barnett (1975), Curtain and Zwart (1995) [26,28]. The scientific community has grown increasingly interested in studying control problems described as abstract differential equations or inclusions in recent decades. The concept of controllability has been central to modern control theory throughout history. It plays an essential role in investigating and designing dynamical control systems and has applications in engineering and operations research. Stochastic systems can be used to model physical problems where some randomness appears. Many researchers have focused their efforts on determining the controllability of stochastic fractional semilinear systems. Most authors have looked into the controllability of autonomous systems [5,8,17]. Some authors, however, have investigated non-autonomous systems [31]. For more work, see [9,18,24,30,34].

    The goal of controllability theory is to be able to control a specific system to the desired state by giving appropriate input functions in a finite time interval. Many authors demonstrated the control system with several delays [6,14,15,17]. Optimal control theory extends the calculus of variations in which an optimized objective function is obtained. We minimize the cost functional due to optimization. It is important in a variety of scientific fields, including engineering, mathematics and biology. The papers [21,25,29] contain some works on controllability.

    Fractional-order stochastic differential equations with multiple control delays have played a significant role in real-life problems. Furthermore, many practical problems have either constant point or time variable delay terms in their control. Differential equations with multiple delays have many applications in control, including population dynamics, electro-mechanical, control theory, biology, epidemiology, etc. Many researchers are now focusing on this theory and its applications. The controllability concept has numerous applications in control theory, electric bulk power systems, industrial and chemical process control, aerospace engineering and, more recently, quantum systems theory. For more information, refer to [4,10,32].

    In 2006, P. Balasubramaniam and S. K. Ntouyas [23] provided the controllability result for partial stochastic functional differential inclusions with infinite delay. In 2017, R. Haloi [27] gave sufficient conditions for controllability of non-autonomous differential equations with a nonlocal finite delay with deviating arguments. In 2022, A. Afreen et al. [1] studied a semilinear stochastic system with constant delays in control.

    More specifically, in 2012, K. Balachandran et al. [17] considered the following nonlinear fractional dynamical system with multiple delays in control

    {CDqtx(t)=Ax(t)+Mi=0Biu(hi(t))+f(t,x(t),u(t)),t[0,T]:=J,x(0)=x0,

    where 0<q<1,xRn,uRp.

    In 2019, A. Haq and N. Sukavanam [3] obtained sufficient conditions for the controllability of the following semilinear delay system

    {ϑ(t)=Aϑ(t)+B1v(t)+B2v(tb)+F(t,ϑa(t),v(t)+v(tb)),t(0,β],ϑ(0)=ϑ1,g(ϑ)=φ,v(t)=0,t[b,0].

    In 2015, A. Shukla et al. [7] studied the approximate controllability of the following semilinear fractional control system of order α(1,2]

    {CDαty(t)=Ay(t)+Bv(t)+f(t,yt,v),0tT,y0(θ)=ϕ(θ),θ[h,0],y(0)=y0.

    In [6,14,15], the authors have studied the controllability of a semilinear system with multiple delays in control. However, in 2017, A. Shukla et al. [9] examined fractional-order α(1,2] stochastic system without control delay. Best of our knowledge, there are no papers concerned with the problem of nonlinear fractional stochastic systems with multiple delays in control in abstract spaces. To fill the gap, we have constructed the system (1.1), which is inspired by the works of [6,7,9,14,15]. Our aim is to examine the controllability of the considered system. To establish the results, first, we transform the controllability problem into a fixed-point problem.

    The remaining part of the paper is designed as follows: Section 2 contains some basic definitions, lemmas and assumptions. In Section 3, the controllability problem is transformed into the existence of a fixed-point problem. Sections 4 and 5 contain the main results of the controllability. In Section 6, several examples are provided to show the effectuality of the result. In the end, a conclusion is added for further work.

    Definition 1. [13] The Caputo fractional derivative of order α for a function gCn([0,],R) is defined by

    CDαtg(t)=1Γ(nα)t0(ts)nα1g(n)(s)ds,n1<α<n,nN.

    Consider the following linear fractional order system

    CDαtz(t)=Az(t),z(0)=ξ,z(0)=0, (2.1)

    where α(1,2),A:D(A)ZZ is closed and densely defined operator in a Hilbert space Z.

    Definition 2. [9] Let α(1,2). A family {Cα}α0L(Z) (Banach space of all bounded linear operators on Z) is called a solution operator (or strongly continuous α-order fractional cosine family) for (2.1) and A is called the infinitesimal generator of Cα(t), if the following conditions are satisfied

    (1) Cα(t) is strongly continuous for t0 and Cα(0)=I;

    (2) Cα(t)D(A)D(A) and ACα(t)ξ=Cα(t)Aξ for all ξD(A),t0;

    (3) Cα(t)ξ is a solution of z(t)=ξ+1Γ(α)t0(ts)α1Az(s)ds for all ξD(A).

    Definition 3. [9] The fractional sine family Sα:R+L(Z) associated with Cα is defined by

    Sα(t)=t0Cα(s)ds,t0.

    Definition 4. [9] The fractional Riemann-Liouville family Pα:R+L(Z) associated with Cα is defined by

    Pα(t)=Iα1tCα(t)=1Γ(α1)t0(ts)α2Cα(s)ds,t0.

    Definition 5. (Mild solution) A stochastic process zC2 is said to be a mild solution of (1.1) if it satisfies

    z(t)=Cα(t)z0+Sα(t)z1+t0Pα(ts)rq=0Equ(sηq)ds+t0Pα(ts)ϱ1(s,z(s),rq=0u(sηq))ds+t0Pα(ts)ϱ2(s,z(s),rq=0u(sηq))dυ(s). (2.2)

    Definition 6. The control system (1.1) is said to be controllable if the initial states of the system are changed to some other desired states by a controlled input in a finite duration of time. If the system is controllable for all z0 at t=0 and for all z()=z at t=, it will be called completely controllable on [0,].

    Lemma 1. [9] For any zLp(Υ,Z), there exists φLpΥ([0,],L02) such that

    z=Ez+0φ(s)dυ(s).

    Lemma 2. [31] Let V:[0,]×ΩL02 be strongly measurable mapping such that 0EV(s)pL02ds <. Then

    Et0V(s)dv(s)pLVt0EV(s)pds,

    for every t[0,] and p2, where LV is the constant depending on p and .

    Schauder's fixed-point theorem. Let (X,) be a Banach space over K(K=R or C) and SX is a non-empty closed, bounded and convex set. Any compact operator A:SS has atleast one fixed point.

    The following assumptions hold throughout the paper.

    (C1) There exist constants μ11,μ2=μ1,μ3=μ1α1Γ(α),μ4>0 such that Cα(t)μ1,Sα(t)μ2,Pα(t)μ3,μ4=max{Eq:q=0,1,2,,r}.

    (C2) The nonlinear function ϱ1:[0,]×Z×UadZ is continuous and there are real constants α1,β1 such that

    ϱ1(t,z(t),rq=0u(tηq))ϱ1(t,˜z(t),rq=0˜u(tηq))pZα1z˜zpC2+β1u˜upUad,

    where u˜upUad=rq=0(u˜u)(tηq)p.

    (C3) The nonlinear function ϱ2:[0,]×Z×UadL02 is continuous and there are real constants α2,β2 such that

    ϱ2(t,z(t),rq=0u(tηq))ϱ2(t,˜z(t),rq=0˜u(tηq))pL02α2z˜zpC2+β2u˜upUad,

    where u˜upUad=rq=0(u˜u)(tηq)p.

    Our aim is to find a suitable control u which steers the stochastic solution of the dynamical system (1.1) from z(0)=z0 to z=Ez+0φ(s)dυ(s). Now for each (y,w)M=C([0,],Lp(Υ,Z))×C([0,],Uad), consider the fractional linear system

    {CDαtz(t)=Az(t)+rq=0Equ(tηq)+ϱ1(t,y(t),rq=0w(tηq))+ϱ2(t,y(t),rq=0w(tηq))dυ(t)dt,t[0,],z(0)=z0,z(0)=z1,u(t)=0,t[ηr,0], (3.1)

    where 1<α<2. M=C([0,],Lp(Υ,Z))×C([0,],Uad) is the Banach space with the norm (y,w)p=yp+wp, where

    yp=supt[0,]Ey(t)pZ.

    The solution of (3.1) is given by

    z(t)=Cα(t)z0+Sα(t)z1+t0Pα(ts)rq=0Equ(sηq)ds+t0Pα(ts)ϱ1(s,y(s),rq=0w(sηq))ds+t0Pα(ts)ϱ2(s,y(s),rq=0w(sηq))dυ(s). (3.2)

    Using u(t)=0,t[ηr,0], we get

    z(t)=Cα(t)z0+Sα(t)z1+rq=0tηq0Pα(tsηq)Equ(s)ds+t0Pα(ts)ϱ1(s,y(s),rq=0w(sηq))ds+t0Pα(ts)ϱ2(s,y(s),rq=0w(sηq))dυ(s). (3.3)

    Putting t= in (3.3), we get

    z()=Cα()z0+Sα()z1+rq=0ηq0Pα(sηq)Equ(s)ds+0Pα(s)ϱ1(s,y(s),rq=0w(sηq))ds+0Pα(s)ϱ2(s,y(s),rq=0w(sηq))dυ(s). (3.4)

    Now, let us introduce the following notation

    ϕ(z0,z();y,w)=EzCα()z0Sα()z1+0φ(s)dυ(s)0Pα(s)ϱ1(s,y(s),rq=0w(sηq))ds0Pα(s)ϱ2(s,y(s),rq=0w(sηq))dυ(s). (3.5)

    Define the controllability Grammian operator

    ζ(0,ηq;y,w){}=rq=0ηq0Pα(sηq)Eq{Pα(sηq)Eq}E{|Υs}ds, (3.6)

    where q=0,1,2,,r and denotes the adjoint. System (3.1) is completely controllable if and only if the controllablity Grammian operator is nonsingular; or equivalently (see Theorem 1, [22])

    ζ(0,ηq;y,w)bI, (3.7)

    where b>0 and I stands for the identity operator.

    If the system (3.1) satisfies the above condition, then one of the control that steers the state (3.3) to the desired state z is given by

    u(t)(t,0,z0,ηq,z;y,w)=EqPα(tηq)ζ1ϕ(z0,z();y,w). (3.8)

    Substituting (3.8) into (3.4) with (3.5) and (3.6), it is easy to verify that for each fixed (y,w)M, the control u(t) steers the initial state z0 to the desired state z=Ez+0φ(s)dυ(s).

    If arbitrarily chosen vectors y,w agree with z,u that result from (3.3) and (3.8), respectively, then these vectors are also solutions of the semilinear system (1.1). Hence, the controllability problem for system (1.1) becomes an existence of a fixed point problem for (3.3) and (3.8).

    Theorem 1. Assume that for (z,˜u)M,

    lim(z,˜u)pϱ1(t,z,˜u)pZ+ϱ2(t,z,˜u)pL02(z,˜u)p=0,

    uniformly on [0,] and (C1) holds. Further, if there exists a closed bounded convex subset H of M such that the operator κ defined by

    κ(y,˜w)=(z,˜u),for any(y,˜w)H, (4.1)

    where ˜u=rq=0u(tηq),˜w=rq=0w(tηq), has a fixed point in H, then the semilinear fractional system (1.1) is completely controllable if it satisfies (3.7).

    Proof. Define the operator κ:HMH by

    κ(y,˜w)=(z,˜u),for any(y,˜w)H, (4.2)

    where

    u(t)=EqPα(tηq)ζ1ϕ(z0,z();y,w)=EqPα(tηq)ζ1×[EzCα()z0Sα()z1+0φ(s)dυ(s)0Pα(s)ϱ1(s,y(s),rq=0w(sηq))ds0Pα(s)ϱ2(s,y(s),rq=0w(sηq))dυ(s)],

    and

    z(t)=Cα(t)z0+Sα(t)z1+rq=0tηq0Pα(tsηq)Eq×EqPα(sηq)ζ1ϕ(z0,z();y,w)ds+t0Pα(ts)ϱ1(s,y(s),rq=0w(sηq))ds+t0Pα(ts)ϱ2(s,y(s),rq=0w(sηq))dυ(s).

    For simplicity, take

    ϱ1p=sups[0,]Eϱ1(s,y(s),rq=0w(sηq))p,ϱ2p=sups[0,]Eϱ2(s,y(s),rq=0w(sηq))p,

    λ1=0Eφ(s)pds,Λ=6p1μp4μp3ζ1p,1p+1σ=1,δ1=Λ1+p/σμp3,δ2=ΛLϱ2μp3,

    δ3=5p11+p/σμp3{(r+1)μp4δ1+1}, δ4=5p11+p/σμp3{(r+1)μp4δ2+Lϱ2},

    N1=Λ{EEzp+μp1Ez0p+μp2Ez1p+Lφλ1} , N2=5p1{μp1Ez0p+μp2Ez1p+(r+1)1+p/σμp3μp4N1},

    N=max{N1,N2},δ=max{δ1,δ2,δ3,δ4}.

    Using Lemma 2 and Holder's inequality with the assumption (C1), we have

    Eu(t)p6p1EqPα(tηq)ζ1p[EEzp+ECα()z0p+ESα()z1p+Lφ0Eφ(s)pds+p/σ0EPα(s)ϱ1(s,y(s),rq=0w(sηq))pds+Lϱ20EPα(s)ϱ2(s,y(s),rq=0w(sηq))pds]6p1μp4μp3ζ1p[EEzp+μp1Ez0p+μp2Ez1p+Lφλ1+1+p/σμp3ϱ1p+Lϱ2μp3ϱ2p]=N1+δ1ϱ1p+δ2ϱ2pN+δ(ϱ1p+ϱ2p),

    E˜u(t)p(r+1)[N+δ(ϱ1p+ϱ2p)]

    and

    Ez(t)p5p1[ECα()z0p+ESα()z1p+p/σrq=0ηq0EPα(sηq)Equ(s)pds+p/σ0EPα(s)ϱ1(s,y(s),rq=0w(sηq))pds+Lϱ20EPα(s)ϱ2(s,y(s),rq=0w(sηq))pds]5p1[μp1Ez0p+μp2Ez1p+(r+1)1+p/σμp3μp4{N1+δ1ϱ1p+δ2ϱ2p}+1+p/σμp3ϱ1p+Lϱ2μp3ϱ2p]=N2+δ3ϱ1p+δ4ϱ2pN+δ(ϱ1p+ϱ2p).

    Since the function ϱ1 and ϱ2 satisfy Proposition 1 of [16]. Therefore, for each pair of constants N and δ, there exists ε>0 such that, if Ey(t)pε2andE˜w(t)pε2, i.e., (y,˜w)pε, then N+δ(ϱ1p+ϱ2p)ε. Therefore, E˜u(t)p(r+1)εandEz(t)pε. Thus, we have proved that, if H(ε)={(y,˜w)H:ypε2and˜wpε2}, where ε=max{(r+2)ε,ε} then κ maps H(ε) into iteslf. Since ϱ1,ϱ2 are continuous, therefore κ is continuous. The complete continuity of κ is followed by Arzela-Ascoli theorem. As H(ε) is closed, bounded and convex set, therefore by Schauder's fixed point theorem, κ has a fixed point (y,˜w)H(ε), i.e., κ(y,˜w)=(y,˜w)(z,˜u). Hence, we have

    z(t)=Cα(t)z0+Sα(t)z1+rq=0tηq0Pα(tsηq)Equ(s)ds+t0Pα(ts)ϱ1(s,y(s),rq=0w(sηq))ds+t0Pα(ts)ϱ2(s,y(s),rq=0w(sηq))dυ(s).

    It is easy to prove that the control u(t) steers the system (1.1) from z0 to z. Hence, the system (1.1) is completely controllable.

    We consider the Lagrange problem to find an optimal state-control pair (z0,u0)C2×Uad satisfying [25]

    I(z0,u0)I(z,u),(z,u)C2×Uad,

    where z denotes the mild solution of the stochastic system (1.1) corresponding to the control uUad and

    I(z,u)=E{0˜G(t,z(t),rq=0u(tηq))dt}. (5.1)

    To discuss the Lagrange problem, we assume the following conditions

    (C4) The Borel measurable function ˜G:[0,]×Z×UadR{} satisfies

    (a) For almost all t[0,],˜G(t,z,) is convex on Uad for each zZ.

    (b) For almost all t[0,],˜G(t,,) is sequentially lower semicontinuous on Z×Uad.

    (c) There exist constants e10,e2>0 and Φ is a non-negative function in L1([0,],R) such that

    ˜G(t,z(t),rq=0u(tηq))Φ(t)+e1zZ+e2upUad,

    where upUad=rq=0u(tηq)p.

    Balder's Theorem 2.1. [11]: The following three conditions

    (a) f(t,,) is sequentially l.s.c. on X×Vμ-a.e.,

    (b) f(t,x,) is convex on V for every xXμ-a.e.,

    (c) there exist M>0 and ψL1R such that f(t,x,v)ψ(t)M(x+|v|) for all xX,vVμ-a.e.,

    are sufficient for sequential strong-weak lower semicontinuity of If on L1X×L1V. Moreover, they are also necessary, provided that If(ˉx,ˉv)<+ for some ˉxL1X,ˉvL1V.

    Theorem 2. Let assumptions (C1)–(C4) hold. Further, if all the hypotheses of Theorem 1 are satisfied, then there exists an optimal pair of (1.1) if 3p1μp3(p/σα1+α2Lϱ2)<1.

    Proof. It is enough to show that there exists (z0,u0)C2×Uad which minimize I(z,u).

    If inf{I(z,u):(z,u)Z×Uad}=, then result holds trivially.

    If inf{I(z,u):(z,u)Z×Uad}=ϵ0<, then there exists a minimizing sequence {(zn,un)} such that I(zn,un)ϵ0 as n. Since Uad is closed and convex, therefore, sequence {un} has a weakly convergent subsequence umu0Uad by Marzur Lemma.

    Using Theorem 1, for each umUad, there exists a mild solution zm of (1.1),

    zm(t)=Cα(t)z0+Sα(t)z1+t0Pα(ts)rq=0Equm(sηq)ds+t0Pα(ts)ϱ1(s,zm(s),rq=0um(sηq))ds+t0Pα(ts)ϱ2(s,zm(s),rq=0um(sηq))dυ(s).

    Similarly, corresponding to u0, we have

    z0(t)=Cα(t)z0+Sα(t)z1+t0Pα(ts)rq=0Equ0(sηq)ds+t0Pα(ts)ϱ1(s,z0(s),rq=0u0(sηq))ds+t0Pα(ts)ϱ2(s,z0(s),rq=0u0(sηq))dυ(s).

    We have,

    Ezm(t)z0(t)p

    3p1Et0Pα(ts)rq=0{Equm(s)Equ0(s)}dsp+3p1Et0Pα(ts){ϱ1(s,zm(s),rq=0um(sηq))ϱ1(s,z0(s),rq=0u0(sηq))}dsp+3p1Et0Pα(ts){ϱ2(s,zm(s),rq=0um(sηq))ϱ2(s,z0(s),rq=0u0(sηq))}dυ(s)p3p1p/σμp3μp4(r+1)t0umu0pds+3p1p/σμp3t0{α1zmz0p+β1umu0p}ds+3p1μp3Lϱ2t0{α2zmz0p+β2umu0p}ds3p1μp3(p/σμp4(r+1)+p/σβ1+β2Lϱ2)t0umu0pds+3p1μp3(p/σα1+α2Lϱ2)t0zmz0pds.

    Since 3p1μp3(p/σα1+α2Lϱ2)<1 and umu0p0, we conclude that zmz0.

    Applying Balder's theorem (see Theorem 2.1, [11]), we obtain

    ϵ0=limmE{0˜G(t,zm(t),rq=0um(tηq))dt}E{0˜G(t,z0(t),rq=0u0(tηq))dt}=I(z0,u0)ϵ0.

    This shows that I(z0,u0)=ϵ0.

    Example 6.1. Consider the following fractional system with single point delay in control

    {CD1.7tz(t,x)=zxx(t,x)+E0u(t,x)+5u(t2π,x)+t3sin(3πt)(z(t,x)+u(t,x)+u(t2π,x))+tcos(t)(3zt(x)x+u(t,x)+u(t2π,x))dυ(t)dt,x[0,π],t[0,7],z(0,x)=z0(x),z(t,x)t|t=0=z1(x),u(t)=0,t[2π,0],z(t,0)=z(t,π)=0,t[0,7]. (6.1)

    Here, η0=0,η1=2π.

    Let Z=L2[0,π] and the operator A:ZZ is defined as Az=z with

    D(A)={zZ:z,zare absolutely continuous,zZandz(0)=z(π)=0}.

    The operator A has discrete spectrum with normalized eigenvectors eq(x)=2πsin(qx) corresponding to the eigenvalues λq=q2,qN. The set {eq:qN} forms an orthogonal basis for Z. Thus, we have

    Az=qNq2z,eqeq,zD(A).

    A generates strongly continuous cosine and sine family given by

    C(t)z=qNcos(qt)z,eqeq,

    and

    S(t)z=qNsin(qt)qz,eqeq,tR,

    respectively. For α(1,2) [12]

    Cα(t)=0tα/2ψα/2(stα/2)C(s)ds,

    where

    ψμ(x)=n=0(x)nn!Γ(μn+1μ),0<μ<1,t>0.

    Define

    U={u:u=q=2uqeq(x)|q=2u2q<},

    with the norm u=(q=2u2q)1/2.

    Define the operator E0:UZ by E0u=(Eu)(t), where EL(U,Z) such that

    Eu(t)=2u2(t)e1(x)+q=2uq(t)eq(x).

    If we define z(t) and u(t) as

    z(t)()=z(t,),u(t)()=u(t,).

    Then

    ϱ1(t,z(t),1q=0u(tηq))(x)=t3sin(3πt)(z(t,x)+u(t,x)+u(t2π,x)),

    and

    ϱ2(t,z(t),1q=0u(tηq))(x)=tcos(t)(3zt(x)x+u(t,x)+u(t2π,x)).

    Now the system (5.1) can be written as in the abstract form (1.1). Thus, (5.1) has a solution. Clearly, all the requirements of Theorem 1 are satisfied, therefore, the system (5.1) is completely controllable on [0,7].

    Example 6.2. Consider the following system

    {CD1.85tz(t,x)=zxx(t,x)+E0u(t,x)+4q=1u(t3q,x)+51+sintz(t,x)+2πu(t,x)+e2u(t3,x)+u(t6,x)+17eu(t9,x)+u(t12,x)+(πe5tz(t,x)+31+e2t4q=0u(t3q,x))dυ(t)dt,x[0,π],t[0,14],z(0,x)=z0(x),z(t,x)t|t=0=z1(x),u(t)=0,t[12,0],z(t,0)=z(t,π)=0,t[0,14]. (6.2)

    Collecting the above definitions and following Example 6.1, we can easily conclude the result.

    Example 6.3. Consider the following system having multiple delays

    {CD1.5tz(t,x)=zxx(t,x)+79nq=0u(t2q,x)+e3tz(t,x)+8e4tnq=0u(t2q,x)+(5z(t,x)+21+πnq=0u(t2q,x))dυ(t)dt,x[0,π],t[0,3n],z(0,x)=z0(x),z(t,x)t|t=0=z1(x),u(t)=0,t[2n,0],z(t,0)=z(t,π)=0,t[0,3n]. (6.3)

    Following Example 6.1, we can conclude that the system (6.3) is completely controllable on [0,3n].

    In the present paper, we have established sufficient conditions for the controllability of a semilinear fractional stochastic system with multiple delays in control. The controllability problem has been transformed into a fixed point problem. The existence of a subset on which the operator is invariant is shown to be a sufficient condition for controllability using Schauder's fixed point theorem. It is also shown that the problem admits at least one optimal pair of state-control under some natural assumptions. Several examples are provided to demonstrate the efficacy of the results. In the future, the above work could be extended to a multi-term time-fractional impulsive system using the same technique or the Picard iterative technique.

    The authors declare no conflicts of interest.



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