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Solvability and optimal controls of non-instantaneous impulsive stochastic neutral integro-differential equation driven by fractional Brownian motion

  • In this manuscript, a new class of non-instantaneous impulsive stochastic neutral integrodi fferential equation driven by fractional Brownian motion (fBm, in short) with state-dependent delay and their stochastic optimal control problem is studied. We utilize the theory of the resolvent operator and a fixed point technique to present the solvability of the stochastic system. Then, the existence of optimal controls is discussed for the proposed stochastic system. Finally, an example is offered to demonstrate the obtained theoretical results.

    Citation: Rajesh Dhayal, Muslim Malik, Syed Abbas. Solvability and optimal controls of non-instantaneous impulsive stochastic neutral integro-differential equation driven by fractional Brownian motion[J]. AIMS Mathematics, 2019, 4(3): 663-683. doi: 10.3934/math.2019.3.663

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  • In this manuscript, a new class of non-instantaneous impulsive stochastic neutral integrodi fferential equation driven by fractional Brownian motion (fBm, in short) with state-dependent delay and their stochastic optimal control problem is studied. We utilize the theory of the resolvent operator and a fixed point technique to present the solvability of the stochastic system. Then, the existence of optimal controls is discussed for the proposed stochastic system. Finally, an example is offered to demonstrate the obtained theoretical results.


    Stochastic differential equations have been used with great success in many application areas including biology, epidemiology, mechanics, economics and finance. For the fundamental study of the theory of stochastic differential equations, we refer to [1,2,3,4]. Yang and Zhu [5] studied the existence, uniqueness, and stability of mild solutions for the stochastic differential equations with Poisson jumps by using fixed point techniques. The fBm with Hurst parameter H(0,1) is a self-similar centered Gaussian random process with stationary increments. It admits the long-range dependence properties when H>1/2. Many exciting applications of fBm have been established in diverse fields such as finance, economics, telecommunications, and hydrology. For more details on fBm, see [6,7,8,9] and the references cited therein. Boudaoui et al. [10] studied the existence and continuous dependence of the mild solutions for the impulsive stochastic differential equation driven by fBm.

    In recent years, the differential equation with fixed moments of impulses (instantaneous impulses) has become the natural framework for modeling of many evolving processes and phenomena studied in economics, population dynamics, and physics. For more details on differential equations with instantaneous impulses, one can see the papers [11,12,13,14] and the references cited therein. Deng et al. [15] discussed the existence and exponential stability for impulsive neutral stochastic functional differential equations driven by fBm with non-compact semigroup. Zhu [16] obtained some sufficient conditions to ensure the pth moment exponential stability of impulsive stochastic functional differential equations with Markovian switching. The action of instantaneous impulses does not describe certain dynamics of evolution processes in pharmacotherapy. For example, consider the following simplified situation concerning the hemodynamic equilibrium of a person. In the case of a decompensation (for example, high or low levels of glucose) one can prescribe some intravenous drugs (insulin). Since the introduction of the drugs into the bloodstream and the consequent absorption for the body are gradual and continuous processes, we can interpret the situation as an impulsive action that starts abruptly and remains active over a finite time interval. For these reasons, Hernández and O'Regan [17] introduced a new class of abstract differential equations with non-instantaneous impulses and they investigated the existence of mild and classical solutions. For comprehensive details on differential equation with non-instantaneous impulses, see [18,19,20]. The qualitative properties of mild solutions for differential equations with non-instantaneous impulses have been investigated in several papers [21,22,23] and the references cited therein.

    On the other hand, delay differential equation has been gaining much interest and attracting the attention of several researchers, because of its wide applications in various fields of science and engineering such as control theory, heat flow, mechanics, distributed networks, and neural networks, etc. The delay depends on the state variable, is called state-dependent delay. For more details on state-dependent delay, we refer to [24,25,26,27,28]. In the neutral differential equation, the highest order derivative of the state variable appears without delay and with delay. Ezzinbi et al. [29] discussed the existence and regularity of solutions for the neutral functional integro-differential equation with delay. Vijayakumar [30] investigated the approximate controllability for integro-differential inclusions by using the resolvent operators. The optimal control problem plays an important role in many scientific fields, such as engineering, mathematics, and biomedical. When the stochastic differential equation describes the performance index and system dynamics, an optimal control problem reduces to a stochastic optimal control problem. Wei et al. [31] obtained the existence of optimal controls for the impulsive integro-differential equation of mixed type. Jiang et al. [32] discussed the existence of optimal controls for fractional evolution inclusion with Clarke subdifferential and nonlocal conditions. In particular, in [33,34], the authors analyzed the existence of optimal controls for the fractional differential equations, whereas in [35,36] the authors investigated the same type of problem for the impulsive fractional stochastic integro-differential equations with delay.

    To the best of our knowledge, there is no paper discussing the solvability and optimal controls of a non-instantaneous impulsive stochastic system driven by fBm with state-dependent delay. In order to fill this gap, we consider the following non-instantaneous impulsive stochastic neutral integro-differential equation driven by fBm with state-dependent delay:

    {dD(t,zt)=A[D(t,zt)+t0G(ts)D(s,zs)ds]dt+C(t)v(t)dt+F2(t,zρ(t,zt))dBH(t)t(pj,tj+1],j=0,1,,M,z(t)=Ej(t,zt),t(tj,pj],j=1,2,,M,z0=ΩB, (1.1)

    where z() takes values in a real separable Hilbert space Z, A is the generator of a C0-semigroup of operators {(t):t0} on Z. BH={BH(t):t0} is a fBm with Hurst index H(1/2,1), takes values in a Hilbert space Y. The initial data Ω={Ω(t),t(,0]} is a B-valued, F0-adapted random variable, which not dependent on BH, where B abstract phase space. The history valued function zt:(,0]Z is defined as zt(θ)=z(t+θ) for all θ(,0] belongs to B. The control function v takes value from a separable reflexive Hilbert space T, and C is linear operator from T into Z. 0=t0=p0<t1<p1<<tM<pM<tM+1=b< are prefixed numbers, J1=[0,b]. Suppose that G(t),tJ1 is a linear and bounded operator. The function D:J1×BZ is defined by D(t,ψ)=ψ(0)F1(t,ψ),ψB and F1:J1×BZ, F2:J1×BL02(Y,Z), where L02(Y,Z) is space of all Q-Hilbert-Schmidt operators from Y into Z, Ej:(tj,pj]×BZ, j=1,2,,M and ρ:J1×B(,b] are suitable functions and they will be specified later.

    The manuscript is structured as follows. Section 2 introduces preliminary facts and some notations. In Section 3, we discussed the solvability of the stochastic system and Section 4 is devoted to the investigation of the existence of optimal control pairs of the Lagrange problem corresponding to the proposed stochastic system. In Section 5, an example is provided to illustrate the applications of the obtained results. The last section is devoted to our conclusions.

    In this section, we briefly review some basic definitions and notations that will be used in the subsequent sections. Let (Ω,F,{Ft}t0,P) be a filtered complete probability space, where Ft the σ-algebra is generated by {BH(s),s[0,t]}. By L(Y,Z), we denote the space of bounded linear operator from Y into Z. For convenience, the same notation . is used to denote the norms in Z, Y, L(Y,Z). The collection of all square integrable, strongly measurable, Z-valued random variables, denoted by L2(Ω,Z), which is a Banach space. L2F0(Ω,Z)={fL2(Ω,Z):fisF0measurable} is subspace of L2(Ω,Z). We denote by PC([r1,r2],Z) the space formed by the normalized piecewise continuous, Ft-adapted measurable process from [r1,r2] into Z.

    Definition 2.1. Given H(0,1), a centered Gaussian and continuous random process βH={βH(t),t0} with covariance function

    E[βH(ϱ1),βH(ϱ2)]=12(ϱ2H1+ϱ2H2|ϱ1ϱ2|2H),

    is called one dimensional fBm and H is the Hurst parameter.

    The fBm βH(t) with 1/2<H<1 has the following integral representation

    βH(t)=t0KH(t,ϱ)dw(ϱ),

    where w(ϱ) is a Wiener process or Brownian motion and the kernel KH(t,ϱ) is defined as

    KH(t,ϱ)=PHϱ1/2Htϱ(τϱ)H3/2τH1/2dτ,fort>ϱ.

    We put KH(t,ϱ)=0 if tϱ. Notice that KHt(t,ϱ)=PH(t/ϱ)H1/2(tϱ)H3/2. Here, PH=[H(2H1)/ξ(22H,H1/2)]1/2 and ξ(,) is Beta function. For ΨL2([0,b]), it is well known from [37] that the Wiener-type integral of the function Ψ w.r.t fBm βH is defined by

    b0Ψ(ϱ)dβH(ϱ)=b0KHΨ(ϱ)dw(ϱ),

    where KHΨ(ϱ)=bϱΨ(t)KHt(t,ϱ)dt.

    Let the operator QL(Y,Y) is defined by Qei=λiei, where {λi0:i=1,2,,} are real numbers with trace Tr(Q)=i=1λi< and {ei,i=1,2,,} is a complete orthonormal basis in Y. Next, we define the infinite dimensional fBm BH on Y with covariance Q as

    BH(t)=BHQ(t)=i=1λieiβHi(t),

    where βHi(t) are real, independent fBm. Now, we define the separable Hilbert space L02(Y,Z) of all Q-Hilbert-Schmidt operators from Y into Z with norm ψ2L02=i=1λiψei2< and the inner product ψ1,ψ2L02=i=1ψ1ei,ψ2ei. The Wiener integral of function Υ:J1L02(Y,Z) w.r.t fBm BH is defined by

    t0Υ(s)dBH(s)=i=1t0λiΥ(s)eidβHi(s)=i=1t0λiKH(Υei)(s)dwi(s). (2.1)

    Lemma 2.1. [6] If Υ:J1L02(Y,Z) satisfies b0Υ(s)2L02ds<, then equation (2.1) is well-defined and Z-valued random variable and we get

    Et0Υ(s)dBH(s)22Ht2H1t0Υ(s)2L02ds. (2.2)

    Now, we introduce the space PC(Z) formed by all Ft-adapted measurable, Z-valued stochastic processes {z(t):tJ1} such that z is continuous at ttj, z(tj)=z(tj) and z(t+j) exists for all j=1,2,,M, endowed with the norm zPC=(suptJ1Ez(t)2)1/2. Then (PC(Z),PC) is Banach space.

    In the following, let T is a separable reflexive Hilbert space from which the controls v take the values. Operator CL(J1,L(T,Z)), where L(J1,L(T,Z)) denote the space of operator-valued functions which are measurable in the strong operator topology and uniformly bounded on the interval J1, endowed with the norm . Let L2F(J1,T) denote the space of all measurable and Ft-adapted, T-valued stochastic processes satisfying the condition Eb0v(t)2Tdt<, and endowed with the norm vL2F=(Eb0v(t)2Tdt)1/2. Let U be a non-empty closed bounded convex subset of T. We define the admissible control set

    Uad={vL2F(J1,T)|v(t)Ua.e.tJ1}.

    Then, CvL2(J1,Z) for all vUad.

    In this paper, we assume that the phase space (B,B) is a seminormed linear space of functions mapping (,0] into Z and subsequent conditions are satisfied.

    [A1]: If z:(,e+b]Z,b>0 is such that z|[e,e+b]PC([e,e+b],Z) and zeB, then for each t[e,e+b] the subsequent conditions are satisfied:

    1. ztB.

    2. z(t)K1ztB.

    3. ztBK2(te)sup{z(s):est}+K3(te)zeB, where K1 is a positive constant, K2,K3:[0,+)[1,+), K2 is a continuous function, K3 is a locally bounded function and K1,K2,K3 are independent of z().

    [A2]: For the function z() in [A1], the function tzt is continuous from [e,e+b] into B.

    [A3]: The phase space B is complete.

    For more details on phase space, we refer to [38,39].

    Lemma 2.2. [21] Let z:(,b]Z be an Ft-adapted measurable process such that the F0-adapted process z0 = Ω(t)L2F0(Ω,B) and z|J1PC(Z), then

    zsBK3EΩB+K2supsJ1Ez(s),

    where K2=suptJ1K2(t), K3=suptJ1K3(t).

    Definition 2.2. A one parameter family {(t):t0} of bounded linear operators, is called resolvent operator for

    dzdt=A[z(t)+t0G(tκ)z(κ)dκ], (2.3)

    if

    1. (0)=I and (t)Neβt for some constants β and N1.

    2. For all zZ, (t)z is strongly continuously for tJ1.

    3. For all tJ1, (t)L(X). For all xX, ()xC1(J1,Z)C(J1,X) and

    ddt(t)x=A[(t)x+t0G(tκ)(κ)xdκ]=(t)Ax+t0(tκ)AG(κ)xdκ,tJ1.

    For more details on the resolvent operator, we refer to [40,41].

    Definition 2.3. A Zvalued stochastic process {z(t),t(,b]} is called a mild solution of the stochastic system (1.1) if z0=Ω, zρ(s,zs)B, z|[0,b]PC(Z) and

    1. z(t) is measurable and adapted to Ft, t0.

    2. z(t)Z has càdlàg paths on [0,b] almost everywhere and for every t[0,b], z(t) satisfies z(t) = Ej(t,zt) for all t(tj,pj], j=1,2,,M, and

    z(t)=(t)[Ω(0)F1(0,Ω)]+F1(t,zt)+t0(ts)C(s)v(s)ds+t0(ts)F2(s,zρ(s,zs))dBH(s)

    for all t[0,t1] and

    z(t)=(tpj)[Ej(pj,zpj)F1(pj,zpj)]+F1(t,zt)+tpj(ts)C(s)v(s)ds+tpj(ts)F2(s,zρ(s,zs))dBH(s)

    for all t(pj,tj+1],j=1,2,,M.

    In this section, we prove the existence of mild solutions for the stochastic system (1.1). Let ρ:J1×B(,b] be a continuous function. To prove our main results, we need the following hypotheses:

    [H1]: (t),t>0 is compact and there exists a constant N>0 such that (t)N for every tJ1.

    [H2]: The function tΩt is continuous from the set S(ρ)={ρ(t,ψ)0:(t,ψ)J1×B} into B and there exists a bounded and continuous function LΩ:S(ρ)(0,) to ensure that ΩtBLΩ(t)ΩB for all tS(ρ).

    [H3]: There exists a constant LF1>0 such that the function F1:J1×BZ satisfies the following conditions

    EF1(t,ψ)2LF1(ψ2B+1),ψB,tJ1,EF1(t,ψ1)F1(t,ψ2)2LF1ψ1ψ22B,ψ1,ψ2B,tJ1.

    [H4]: There exist constants LEj>0, j=1,2,,M, such that the functions Ej:(tj,pj]×BZ, j=1,2,,M, satisfies the following conditions

    EEj(t,ψ)2LEj(ψ2B+1),ψB,EEj(t,ψ1)Ej(t,ψ2)2LEjψ1ψ22B,ψ1,ψ2B.

    [H5]: The function F2:J1×BL02(Y,Z) satisfies the conditions

    (a) The function F2(t,):BL02(Y,Z) is continuous for a.e tJ1, and tF2(t,ψ) is measurable for all ψB.

    (b) There exists a continuous function η:J1[0,) and a continuous nondecreasing function Θ:[0,)(0,) to ensure that for all (t,ψ)J1×B

    EF2(t,ψ)2L02η(t)ΘF2(ψ2B),lim infwΘF2(w)w=Θ1.

    [H6]: The following inequality holds

    max1jM2[K2]2[LEj+8N2(LEj+LF1)+4LF1+8HN2b2H1Θ1b0η(s)ds]<1.

    Lemma 3.1. [28] Let z:(,b]Z such that z0=Ω and z|J1PC(Z). If [H2] be hold, then

    ztB(K3+LΩ)ΩB+K2sup{Ez(ω):ω[0,max{0,t}]},tS(ρ)J1,

    where K2=suptJ1K2(t), K3=suptJ1K3(t), and LΩ=suptS(ρ)LΩ(t).

    Theorem 3.1. If the hypotheses [H1]–[H6] are fulfilled. Then for each vUad, the stochastic system (1.1) has at least one mild solution on J1, provided that

    max1jM2[K2]2(LEj+4N2LEj+2(2N2+1)LF1)<1. (3.1)

    Proof. On the space BPC = {zPC(Z):z(0)=Ω(0)} endowed with the uniform convergence topology. For each l>0, let

    ¯Bl={zBPC:z2PCl}.

    Let the operator F:¯Bl BPC be specified by

    (Fz)(t)={R(t)[Ω(0)F1(0,Ω)]+F1(t,¯zt)+t0R(ts)C(s)v(s)ds+t0R(ts)F2(s,¯zρ(s,¯zs))dBH(s),t[0,t1],j=0,Ej(t,¯zt),t(tj,pj],j1,R(tpj)[Ej(pj,¯zpj)F1(pj,¯zpj)]+F1(t,¯zt)+tpjR(ts)C(s)v(s)ds+tpjR(ts)F2(s,¯zρ(s,¯zs))dBH(s),t(pj,tj+1],j1,

    where ¯z:(,b]Z is such that ¯z0=Ω and ¯z=z on J1. For z¯Bl, from Lemma 3, we have

    ¯zρ(s,¯zs)2B2(K3+LΩ)2Ω2B+2[K2]2l=l.

    From [H1] and Hölder's inequality, we have

    Etpj(ts)C(s)v(s)ds2E[tpj(ts)C(s)v(s)ds]2N2C2(tj+1pj)Etpjv(s)2TdsN2C2(tj+1pj)v2L2F.

    By Bochner theorem, it follows that (ts)C(s)v(s) are integrable on (pj,t),j=0,1,,M. Therefore F is well defined on ¯Bl. Now, we split F as F1+F2, where

    (F1z)(t)={(t)[Ω(0)F1(0,Ω)]+F1(t,¯zt),t[0,t1],j=0,Ej(t,¯zt),t(tj,pj],j1,(tpj)[Ej(pj,¯zpj)F1(pj,¯zpj)]+F1(t,¯zt),t(pj,tj+1],j1,

    and

    (F2z)(t)={t0(ts)C(s)v(s)ds+t0(ts)F2(s,¯zρ(s,¯zs))dBH(s),t[0,t1],j=0,0,t(tj,pj],j1,tpj(ts)C(s)v(s)ds+tpj(ts)F2(s,¯zρ(s,¯zs))dBH(s),t(pj,tj+1],j1.

    For the sake of convenience, we break the proof into a sequence of steps.

    Step 1. There exists l>0 such that F(¯Bl)¯Bl.

    If we assume that this assertion is false, then for any l>0, we can choose zl¯Bl and tJ1 such that EF(zl)(t)2>l. By [H1], [H3]–[H6] and Hölder's inequality, we have for t[0,t1],

    l<EF(zl)(t)24E(t)[Ω(0)F1(0,Ω)]2+4EF1(t,¯zlt)2+4Et0(ts)C(s)v(s)ds2+4Et0(ts)F2(s,¯zlρ(s,¯zls))dBH(s)28N2[K21Ω2B+EF1(0,Ω)2]+4EF1(t,¯zlt)2+4E[t0(ts)C(s)v(s)ds]2+8HN2t2H11t0EF2(s,¯zlρ(s,¯zls))2L02ds8N2[K21Ω2B+LF1(Ω2B+1)]+4LF1(¯zlt2B+1)+4N2C2t1v2L2F+8HN2t2H11t0η(s)ΘF2(¯zlρ(s,¯zls)2B)ds.

    For any t(tj,pj], j=1,2,,M, we have

    l<EF(zl)(t)2LEj(¯zlt2B+1).

    Similarly, for any t(pj,tj+1], j=1,2,,M, we have

    l<EF(zl)(t)24E(tpj)[Ej(pj,¯zlpj)F1(pj,¯zlpj)]2+4EF1(t,¯zlt)2+4Etpj(ts)C(s)v(s)ds2+4Etpj(ts)F2(s,¯zlρ(s,¯zls))dBH(s)28N2[EEj(pj,¯zlpj)2+EF1(pj,¯zlpj)2]+4EF1(t,¯zlt)2+4E[tpj(ts)C(s)v(s)ds]2+8HN2t2H1j+1tpjEF2(s,¯zlρ(s,¯zls))2L02ds8N2(LEj+LF1)¯zlpj2B+8N2(LEj+LF1)+4LF1(¯zlt2B+1)+4N2C2tj+1v2L2F+8HN2t2H1j+1tpjη(s)ΘF2(¯zlρ(s,¯zls)2B)ds.

    For any t[0,b], we have

    l<EF(zl)(t)2W+LEjl+8N2(LEj+LF1)l+4LF1l+8HN2b2H1ΘF2(l)t0η(s)ds,

    and hence,

    l<2(K3+LΩ)2Ω2B+2[K2]2[W+LEjl+8N2(LEj+LF1)l+4LF1l+8HN2b2H1ΘF2(l)b0η(s)ds],

    where

    W=max1jM{8N2[K21Ω2B+LF1(Ω2B+1)]+LEj+8N2(LEj+LF1)+4LF1+4N2C2bv2L2F}.

    Dividing both sides by l and taking the limit as l, we have

    1<2[K2]2[LEj+8N2(LEj+LF1)+4LF1+8HN2b2H1Θ1b0η(s)ds],

    which is contrary to our assumption [H6]. Hence, for some l>0, F(¯Bl)¯Bl.

    Step 2. F1 is a contraction map on ¯Bl.

    For any y,z¯Bl, if t[0,t1], then we have

    E(F1y)(t)(F1z)(t)2LF1¯yt¯zt2B2[K2]2LF1sup{E¯y(s)¯z(s)2:0<s<t}2[K2]2LF1sups[0,b]E¯y(s)¯z(s)2=2[K2]2LF1sups[0,b]Ey(s)z(s)2,(since¯z=zin[0,b])=2[K2]2LF1yz2PC.

    If t(tj,pj], j=1,2,,M, then we have

    E(F1y)(t)(F1z)(t)2LEj¯yt¯zt2B2[K2]2LEjsups[0,b]E¯y(s)¯z(s)2=2[K2]2LEjyz2PC.

    Similarly, if t(pj,tj+1], j=1,2,,M, then we have

    E(F1y)(t)(F1z)(t)22N2[2EEj(pj,¯ypj)Ej(pj,¯zpj)2+2EF1(pj,¯ypj)F1(pj,¯zpj)2]+2EF1(t,¯yt)F1(t,¯zt)28N2[K2]2LEjsup{E¯y(s)¯z(s)2:0<s<t}+4[K2]2LF1(2N2+1)sup{E¯y(s)¯z(s)2:0<s<t}4[K2]2[2N2LEj+(2N2+1)LF1]sups[0,b]E¯y(s)¯z(s)2=4[K2]2[2N2LEj+(2N2+1)LF1]sups[0,b]Ey(s)z(s)2=4[K2]2[2N2LEj+(2N2+1)LF1]yz2PC.

    For any t[0,b], we have

    E(F1y)(t)(F1z)(t)2LF1yz2PC.

    Taking supremum over t

    F1yF1z2PCLF1yz2PC,

    where LF1=2[K2]2(LEj+4N2LEj+2(2N2+1)LF1). By Eq. (3.1), we see that LF1<1. Hence, F1 is a contraction map on ¯Bl.

    Step 3. We show that F2 is continuous on ¯Bl.

    Let {zm}m=1¯Bl be a sequence such that zmz in ¯Bl as m. From axiom [A1], we have that (¯zm)s¯zs uniformly for s(,b] as m. By hypothese [H5] and [42, Theorem 2.2, Step-3], we have

    F2(s,¯zmρ(s,(¯zm)s))F2(s,¯zρ(s,¯zs)),

    for any s[0,t], and since

    EF2(s,¯zmρ(s,(¯zm)s))F2(s,¯zρ(s,¯zs))2L022ΘF2(l)η(s).

    For any t(pj,tj+1],j=0,1,,M, we have

    E(F2zm)(t)(F2z)(t)2=Etpj(ts)[F2(s,¯zmρ(s,¯zms))F2(s,¯zρ(s,¯zs))]dBH(s)22HN2t2H1j+1tpjEF2(s,¯zmρ(s,(¯zm)s))F2(s,¯zρ(s,¯zs))2L02ds2HN2b2H1t0EF2(s,¯zmρ(s,(¯zm)s))F2(s,¯zρ(s,¯zs))2L02ds.

    By the Lebesgue dominated convergence theorem, we have

    F2zmF2z2PC0asm.

    Thus, F2 is continuous.

    Step 4. We show that {F2z:z¯Bl} is equicontinuous.

    Since (t) is compact, which implies that the continuity of (t) in (0,b]. Let pj<ϵ<ttj+1, j=0,1,,M, and ω>0 such that (ξ1s)(ξ2s)2<ϵ for every ξ1,ξ2(pj,tj+1] with |ξ1ξ2|<ω. For each z¯Bl, 0<|κ|<ω with t,t+κ(pj,tj+1], j=0,1,,M, we have

    E(F2z)(t+κ)(F2z)(t)24Et+κt(t+κs)C(s)v(s)ds2+4Etpj[(t+κs)(ts)]C(s)v(s)ds2+4Et+κt(t+κs)F2(s,¯zρ(s,¯zs))dBH(s)2+4Etpj[(t+κs)(ts)]F2(s,¯zρ(s,¯zs))dBH(s)2=4[χ1+χ2],

    where

    χ1E[t+κt(t+κs)C(s)v(s)ds]2+E[tpj(t+κs)(ts)C(s)v(s)ds]2N2κC2Et+κtv(s)2Tds+C2tj+1Etpj(t+κs)(ts)2v(s)2TdsN2κC2Et+κtv(s)2Tds+ϵC2tj+1Etpjv(s)2Tds,χ22HN2t2H1j+1t+κtEF2(s,¯zρ(s,¯zs))2L02ds+2Ht2H1j+1tpj(t+κs)(ts)2EF2(s,¯zρ(s,¯zs))2L02ds2HN2t2H1j+1ΘF2(l)t+κtη(s)ds+2ϵHt2H1j+1ΘF2(l)tpjη(s)ds.

    We conclude that E(F2z)(t+κ)(F2z)(t)20 as κ0 and ϵ is sufficiently small. Hence, {F2z:z¯Bl} is equicontinuous. Also, clearly {F2z:z¯Bl} is uniformly bounded.

    Step 5. The set Q(t)={(F2z)(t):z¯Bl},tJ1 is relatively compact in Z.

    Clearly, Q(0)={0} is compact. Let ξ is real number and t(pj,tj+1],j=0,1,,M, be fixed with 0<ξ<t. For z¯Bl, we define

    (Fξ2z)(t)={tξ0(ts)C(s)v(s)ds+tξ0(ts)F2(s,¯zρ(s,¯zs))dBH(s),t[0,t1],j=0,0,t(tj,pj],j1,tξpj(ts)C(s)v(s)ds+tξpj(ts)F2(s,¯zρ(s,¯zs))dBH(s),t(pj,tj+1],j1.

    Since (t) is compact, the set Qξ(t)={(Fξ2z)(t):z¯Bl} is relatively compact in Z for every ξ. For t(pj,tj+1],j=0,1,,M, we have

    E(F2z)(t)(Fξ2z)(t)22Etpj(ts)C(s)v(s)dstξpj(ts)C(s)v(s)ds2+2Etpj(ts)F2(s,¯zρ(s,¯zs))dBH(s)tξpj(ts)F2(s,¯zρ(s,¯zs))dBH(s)22Ettξ(ts)C(s)v(s)ds2+2Ettξ(ts)F2(s,¯zρ(s,¯zs))dBH(s)22N2ξC2Ettξv(s)2Tds+4HN2t2H1j+1ΘF2(l)ttξη(s)ds0asξ0.

    The relatively compact set Qξ(t) and set Q(t) are arbitrarily close. Hence, Q(t)={(F2z)(t):z¯Bl} is relatively compact in Z. By using step 3–5 along with Arzela-Ascoli theorem, we obtain that the F2 is a completely continuous operator. Hence, by Krasnoselskii's theorem [43], we realize that the operator F1+F2 has a fixed point, which is a mild solution of the stochastic system (1.1).

    In this section, we prove the existence of optimal controls for the stochastic system. Let zv be the mild solution of the stochastic system (1.1) corresponding to the control vUad. We consider the Lagrange problem (LP): Find an optimal state-control pair (z,v)BPC×Uad such that

    J(z,v)J(zv,v)for allvUad,

    where

    J(zv,v)=Eb0M(t,zvt,zv(t),v(t))dt.

    For the existence of optimal controls, we shall introduce the following hypotheses

    [H7]: The function M:J1×B×Z×TR{} satisfies:

    (a) M is Borel measurable

    (b) M(t,z1,z2,) is convex function on T for each z1B, z2Z and almost all tJ1.

    (c) M(t,,,) is sequentially lower semi-continuous on B×Z×T for almost all tJ1.

    (d) There exist constants ω1,ω20, ω3>0 and Φ is non-negative function in L1(J1,R) such that

    M(t,z1,z2,v)Φ(t)+ω1z1B+ω2z2+ω3v2T.

    [H8]: The operator C is strongly continuous.

    Theorem 4.1. Assume that the presumptions [H1]–[H8] are fulfilled. Then the problem (LP) admits at least one optimal control pair on BPC×Uad.

    Proof. If inf{J(zv,v):vUad}=+, there is nothing to prove. Next, we choose inf{J(zv,v):vUad}=ϵ<+ and using the hypotheses [H7], we obtain

    J(zv,v)b0Φ(t)dt+ω1b0zvt(t)Bdt+ω2b0zv(t)dt+ω3b0v(t)2Tϵ>.

    By definition of infimum, there exists a minimizing sequence {(zk,vk)}Rad, where Rad = {(z,v):z be the mild solution of the stochastic system (1.1) corresponding to the control vUad} such that

    J(zk,vk)ϵask+.

    Since {vk} Uad, {vk} is bounded in the space L2F(J1,T), then exists a subsequence, relabeled as {vk}, and vL2F(J1,T) such that vk converges weakly to v in L2F(J1,T) as k. Since Uad is convex and closed, then by Marzur Lemma, we have vUad.

    Let zk be the sequence of mild solutions of the stochastic system (1.1) corresponding to vk and zk fulfills the consecutive integral equations

    zk(t)={(t)[Ω(0)F1(0,Ω)]+F1(t,¯zkt)+t0(ts)C(s)vk(s)ds+t0(ts)F2(s,¯zkρ(s,¯zks))dBH(s),t[0,t1],j=0,Ej(t,¯zkt),t(tj,pj],j1,(tpj)[Ej(pj,¯zkpj)F1(pj,¯zkpj)]+F1(t,¯zkt)+tpj(ts)C(s)vk(s)ds+tpj(ts)F2(s,¯zkρ(s,¯zks))dBH(s),t(pj,tj+1],j1.

    Let Fk2(s)F2(s,¯zkρ(s,¯zks)). Then, for each zk¯BlBPC, by hypotheses [H5], we obtain that Fk2:J1L02(Y,Z) is bounded operator. Hence, Fk2()L2(J1,L02(Y,Z)). Furthermore, {Fk2()} is bounded in L2(J1,L02(Y,Z)), there are subsequence, relabeled as {Fk2()} and F2()L2(J1,L02(Y,Z)) such that Fk2()wF2()inL2(J1,L02(Y,Z))ask.

    Next, we consider the following stochastic system

    {dD(t,zt)=A[D(t,zt)+t0G(ts)D(t,zs)ds]dt+C(t)v(t)dt+F2(t)dBH(t)t(pj,tj+1],j=0,1,,M,z(t)=Ej(t,zt),t(tj,pj],j=1,2,,M,z0=ΩB. (4.1)

    By Theorem 3.1, we know that the stochastic system (4.1) has a mild solution

    z(t)={(t)[Ω(0)F1(0,Ω)]+F1(t,¯zt)+t0(ts)C(s)v(s)ds+t0(ts)F2(s)dBH(s),t[0,t1],j=0,Ej(t,¯zt),t(tj,pj],j1,(tpj)[Ej(pj,¯zpj)F1(pj,¯zpj)]+F1(t,¯zt)+tpj(ts)C(s)v(s)ds+tpj(ts)F2(s)dBH(s),t(pj,tj+1],j1.

    For any t[0,t1], we have

    Ezk(t)z(t)23[Υk1(t)+Υk2(t)+Υk3(t)],

    where

    Υk1(t)=EF1(t,¯zkt)F1(t,¯zt)2LF1¯zkt¯zt2B2[K2]2LF1sup{E¯zk(s)¯z(s)2:0<s<t}2[K2]2LF1sups[0,b]E¯zk(s)¯z(s)2=2[K2]2LF1sups[0,b]Ezk(s)zk(s)2,(since¯z=zin[0,b])=2[K2]2LF1zkz2PC,Υk2(t)=Et0R(ts)C(s)[vk(s)v(s)]ds2N2t1Et0C(s)vk(s)C(s)v(s)2ds,Υk3(t)=Et0R(ts)[Fk2(s)F2(s)]dBH(s)22Ht2H11t0E(ts)[Fk2(s)F2(s)]2L02ds.

    For any t(tj,pj], j=1,2,,M, we have

    Ezk(t)z(t)22[K2]2LEjzkz2PC.

    For any t(pj,tj+1], j=1,2,,M, we have

    Ezk(t)z(t)24[Ψk1(t)+Ψk2(t)+Ψk3(t)+Ψk4(t)],

    where

    Ψk1(t)=2N2EEj(pj,¯zkpj)Ej(pj,¯zpj)24[K2]2N2LEjzkz2PC,Ψk2(t)=2N2EF1(pj,¯zkpj)F1(pj,¯zpj)2+EF1(t,¯zkt)F1(t,¯zt)2(2N2+1)LF1¯zkt¯zt2B2[K2]2(2N2+1)LF1zkz2PC,
    Ψk3(t)=EtpjR(ts)C(s)[vk(s)v(s)]ds2N2tj+1EtpjC(s)vk(s)C(s)v(s)2ds,
    Ψk4(t)=EtpjR(ts)[Fk2(s)F2(s)]dBH(s)22Ht2H1j+1tpjE(ts)[Fk2(s)F2(s)]2L02ds.

    For t[0,b], we have

    Ezk(t)z(t)2L0zkz2PC+Φk1(t)+Φk2(t),

    where

    L0=max1jM[16[K2]2N2LEj+8[K2]2(2N2+1)LF1+2[K2]2LEj]<1,Φk1(t)=4N2bEt0C(s)vk(s)C(s)v(s)2ds,Φk2(t)=8Hb2H1t0E(ts)[Fk2(s)F2(s)]2L02ds.

    Thus, we have

    zkz2PCΦk1(t)+Φk2(t)1L0.

    By [H8], we have

    CvkCv2L2(J1,Z)0ask. (4.2)

    By the Lebesgue dominated convergence theorem and Eq. (4.2), we have

    Φk1(t),Φk2(t)0ask.

    Hence,

    zkzinBPCask.

    By [H5], we obtain

    Fk2()F2(,¯zρ(,¯z))inBPCask.

    Limit is unique, so we obtain

    F2(t)=F2(t,¯zρ(t,¯zt)).

    Thus, z can be given

    z(t)={(t)[Ω(0)F1(0,Ω)]+F1(t,¯zt)+t0(ts)C(s)v(s)ds+t0(ts)F2(s,¯zρ(s,¯zs))dBH(s),t[0,t1],j=0,Ej(t,¯zt),t(tj,pj],j1,(tpj)[Ej(pj,¯zpj)F1(pj,¯zpj)]+F1(t,¯zt)+tpj(ts)C(s)v(s)ds+tpj(ts)F2(s,¯zρ(s,¯zs))dBH(s),t(pj,tj+1],j1.

    Since BPCL1(J1,Z), by using the [H7] and Balder's theorem [44], we have

    ϵJ(z,v)=Eb0M(t,zt,z,v)dtlimkEb0M(t,zkt,zk,vk)dt=ϵ,

    which shows that J attains its infimum at (z,v)BPC×Uad.

    Consider the following non-instantaneous impulsive stochastic partial neutral integro-differential control system driven by fBm with state-dependent delay:

    dD(t,μt)(ε)=2ε2[D(t,μt)(ε)+t0S(ts)D(s,μs)(ε)ds]dt+10K(ε,s)v(s,t)dsdt+tω3(t,st,ε,μ(sρ1(t)ρ2(μ(t)),ε))dsdBH(t),vUad,(t,ε)Mj=0(pj,tj+1]×[0,π],μ(t,ε)=t¯ωj(st,ε)μ(s,ε)ds,(t,ε)Mj=1(tj,pj]×[0,π]μ(t,0)=0=μ(t,π),μ(s,ε)=Ω(s,ε),(s,ε)(,0]×[0,π], (5.1)

    with cost functional as

    J(μ,v)=E10π00μ(t+s,ε)2dsdεdt+E10π0μ(t,ε)2dεdt+E10π0v(t,ε)2Tdεdt,

    where 0=t0=p0<t1<p1<<tM<pM<tM+1=b=1, K:[0,π]×[0,1] is continuous and BH is a fBm with the Hurst index 1/2<H<1. In this system

    D(t,μt)(ε)=μ(t,ε)tω1(st)μ(s,ε)ds.

    Consider the space Z=T=L2[0,π] and A:D(A)ZZ by Aθ=θ and domain of A is defined as

    D(A)={θZ:θ,θare absolutely continuous, θZ,θ(0)=θ(π)=0}. (5.2)

    Then A generates a C0-semigroup (t) which is compact, self-adjoint. And there exist normalized set θn(v)=2/πsin(nv),nN of eigenvectors of A corresponding to eigenvalues n2,nN. Since the resolvent operator (t) is compact, there exists a constant N>0 such that (t)N, then the hypotheses [H1] is fulfilled. Next, we define the admissible control set Uad={v(,ε)|[0,1]T is measurable, Ft-adapted stochastic processes, and vL2Fα,α>0}.

    Let l0, 1q<, Λ:(,l]R, be a measurable and non-negative function. We denote by PCl×Lq(Λ,Z) the set consists of all classes of functions Ω:(,0]Z such that Ω|[l,0]PC([l,0],Z), ΛΩq is Lebesgue integrable on (,l) and Ω() is Lebesgue measurable on (,l) with norm

    ΩB=sup{Ω(κ):lκ0}+(lΛ(κ)Ω(κ)qdκ)1/q.

    The space PC0×L2(Λ,Z) satisfies the axioms [A1]–[A3] with choice K1=1, K3(t)=γ(t)1/2, K2(t)=1+(0tΛ(κ)dκ)1/2, for t0. To get points of interest about the phase space, see [21,38].

    Let η(κ)(ε)=η(κ,ε), (κ,ε)(,0]×[0,π]. Set

    μ(t)(ε)=μ(t,ε),ρ(t,η)=ρ1(t)ρ2(η(0)),

    we have

    F1(t,η)(ε)=0ω1(κ)η(κ)(ε)dκ,F2(t,η)(ε)=0ω2(t,κ,ε,η(κ)(ε))dκ,C(t)v(t)(ε)=10K(ε,s)v(s,t)ds,Ej(t,η)(ε)=0¯ωj(κ,ε)η(κ)(ε)dκ,j=1,2,,M.

    Moreover, we assume that

    1. ρi:[0,)[0,),i=1,2, are continuous functions.

    2. ω1:RR is continuous function, and

    lF1=(0(ω1(s))2Λ(s)ds)1/2<.

    3. There exist continuous functions a31,a32:RR such that continuous function ω3:R4R satisfies the conditions

    |ω3(t,s,ε,y)|a31(t)a32(s)|y|,(t,s,ε,y)R4,withlF2=(0(a32(s))2Λ(s)ds)1/2<.

    4. There exist continuous functions cj:RR such that continuous functions ¯ωj:R2R,j=1,2,,M satisfies the conditions

    |¯ωj(s,ε)|cj(s),(s,ε)R2,withlEj=(0(cj(s))2Λ(s)ds)1/2<.

    From the above facts, we obtain

    EF1(t,η)2=E[(π0(0ω1(κ)η(κ)(ε)dκ)2dε)1/2]2E[(0(ω1(κ))2Λ(κ)dκ)1/2(0Λ(κ)η(κ)2dκ)1/2]2[lF1(η(0)+(0Λ(κ)η(κ)2dκ)1/2)]2=LF1η2B,

    where LF1=[lF1]2.

    EF1(t,η1)F1(t,η2)2=E[(π0(0ω1(κ)[η1(κ)(ε)η2(κ)(ε)]dκ)2dε)1/2]2E[(0(ω1(κ))2Λ(κ)dκ)1/2(0Λ(κ)η1(κ)η2(κ)2dκ)1/2]2[lF1(η1(0)η2(0)+(0Λ(κ)η1(κ)η2(κ)2dκ)1/2)]2=LF1η1η22B,

    where LF1=[lF1]2. Similarly, we have EF2(t,η)2LF2η2B, EEj(t,η1)Ej(t,η2)2LEjη1η22B, and EEj(t,η)2LEjη2B, where LEj=[lEj]2,LF2=[a31lF2]2. Further, we can impose some suitable conditions on the above-defined functions to verify the hypotheses of the Theorems 3.1 and 4.1. Therefore, the problem (LP) corresponding to the stochastic system (5.1) has at least one optimal control pair.

    In this manuscript, we studied the stochastic optimal control problem for a class of non-instantaneous impulsive stochastic neutral integro-differential equation driven by fBm. We define a concept of the piecewise continuous mild solutions for the proposed system, which is used to construct a suitable operator and apply fixed point technique to derive the existence result. Also, we prove the existence of optimal controls for the proposed system, which is used to derive optimization conditions. Finally, the obtained results have been verified through an example. There are two direct issues which require further study. First, we will investigate the optimal control problems for the non-instantaneous impulsive stochastic delay differential equations driven by Lévy processes [45]. Second, we will be devoted to studying the approximate controllability for the Markov and semi-Markov switched stochastic system [46,47].

    We are very thankful to the anonymous reviewers and editor for their constructive comments and suggestions which help us to improve the manuscript.

    All authors declare no conflicts of interest in this paper.



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