The paper investigated the exact controllability of delayed fractional evolution systems of order α∈(1,2) in abstract spaces. At first, the exact controllability result is obtained when the nonlinear term f is locally Lipschitz continuous. Then, the certain compactness conditions and the measure of noncompactness conditions were applied to demonstrate the exact controllability of the concerned problem. The discussion was based on the fixed point theorems and the cosine family theory.
Citation: Lijuan Qin. On the controllability results of semilinear delayed evolution systems involving fractional derivatives in Banach spaces[J]. AIMS Mathematics, 2024, 9(7): 17971-17983. doi: 10.3934/math.2024875
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The paper investigated the exact controllability of delayed fractional evolution systems of order α∈(1,2) in abstract spaces. At first, the exact controllability result is obtained when the nonlinear term f is locally Lipschitz continuous. Then, the certain compactness conditions and the measure of noncompactness conditions were applied to demonstrate the exact controllability of the concerned problem. The discussion was based on the fixed point theorems and the cosine family theory.
It is well known that the semilinear evolution equations have a considerable practical background in physics, biology, engineering, and other fields (see [1,2] and the reference therein). For fractional evolution equations, the existence as well as the controllability have become a hot topic in recent years (see, for example, [3,4,5,6]). In [3], Li et al. considered the existence and uniqueness of weak solutions and strong solutions of an inhomogeneous Cauchy problem of Riemann-Liouville fractional evolution equations of order α∈(1,2) using an α-order fractional resolvent. In [4], by introducing an operator Sα in term of the generalized Mittag-Leffler function and the curve integral, Li et al. investigated the existence and uniqueness of (mild) solutions for a class of Caputo fractional Cauchy problem by means of the Banach fixed point theorem and the Schauder fixed point theorem. In [5], by using the Krasnoselskii fixed point theorem and the solution operator method, the existence of mild solutions to a class of fractional semilinear integro-differential equations of order 1<α<2 was demonstrated. In [6], Yang proved the existence and approximate controllability of the Sobolev-type fractional evolution equations of order α∈(1,2) using the Sadovskii fixed point theorem and the resolvent operator theory.
In this article, we demonstrate the exact controllability of the delayed fractional control system in the Banach space E
{C∂αty(t)=Ay(t)+f(t,yt)+Bv(t), t∈U:=[0,c], α∈(1,2),y(t)=ϕ(t), ∀t∈[−r,0],y′(0)=y1, | (1.1) |
where C∂αt represents the fractional partial derivative operator on t of order α in the Caputo sense, A:D(A)⊆E→E is a densely-defined and closed linear operator in E, D(A) is the domain of A equipped with the norm ‖x‖D(A)=‖x‖+‖Ax‖ for x∈D(A), f is a given function which represents the nonlinear term, v∈L2(U,H), H is another Banach space, y1∈E and ϕ:[−r,0]→E is continuous, B:H→E is a linear operator. For any t∈U, yt(θ)=y(t+θ) for any θ∈[−r,0]. r and c are given positive constants.
The observation of the electromagnetic, acoustic, and mechanical influence shows that there exist some transfer processes in a medium, which are not described by a usual diffusion equation. Fractional Cauchy problems are useful in physics to model such anomalous diffusion, see [3] and the references therein. Hence, it is significant to study the control system (1.1).
In 2021, the Laplace transform method and the cosine family theory were applied by Zhou et al. in [7] to present the suitable definition of mild solutions of the linear inhomogeneous Cauchy problem
{C∂αty(t)=Ay(t)+h(t), t∈[0,c], α∈(1,2),y(0)=y0, y′(0)=y1, |
where y0∈E and h is a given linear function. Then the controllability was considered for the corresponding semilinear fractional evolution system
{C∂αty(t)=Ay(t)+f(t,y(t))+Bv(t), t∈(0,c],α∈(1,2),y(0)=y0, y′(0)=y1, |
where f(t,y) is global Lipschitz continuous or satisfies a certain compactness condition. Obviously, the global Lipschitz continuity contains local Lipschitz continuity and first-order linear growth condition. The reverse is not true.
In 2023, Yang in [8] demonstrated the approximate controllability of the fractional control system
{L∂αty(t)=Ay(t)+F(t,˜yt)+Bv(t), t∈(0,c], α∈(1,2),˜y(0)=ϕ(t), t∈[−r,0],(H2−α∗y)′(0)=y1, |
where L∂αt is the fractional derivative operator on t of order α in the Riemann-Liouville sense, ˜y(t)=t2−αy(t) for t∈U with ˜y(0)=limt→0+˜y(t) and ˜yt(θ)=˜y(t+θ) for t∈U and θ∈[−r,0], Hς(t)=tς−1Γ(ς) for t,ς>0, Γ(⋅) is the standard Gamma function. The symbol ∗ represents the convolution. When the sine family T(t), corresponding to the cosine family {G(t):t≥0} generated by A, is a compact operator for t>0, the approximate controllability results were obtained.
The main features of this paper are summarized below:
(1) The exact controllability of the control system (1.1) is demonstrated in Theorem 3.1 when f is local Lipschitz continuous. Compactness conditions of the nonlinear term f or the cosine family {G(t):t≥0} or the sine family {T(t):t≥0} are essential assumptions in existing articles, but we removed it in Theorem 3.1.
(2) When f satisfies the certain compactness conditions or the measure of noncompactness conditions, the exact controllability of (1.1) is also obtained (see Theorems 3.2–3.4). These results are nature extensions of [7,8].
Let C([−r,c],E) be the Banach space of E-valued continuous functions on [−r,c] with the norm ‖y‖C([−r,c],E)=supt∈[−r,c]‖y(t)‖. B(H,E) represents the Banach space of linear bounded operators from H to E with the norm ‖⋅‖B. B(E):=B(E,E). We always suppose that B∈B(H,E), that is, ∃M1>0 such that ‖B‖B≤M1.
Definition 2.1. [9] A family {G(t):t∈R}⊂B(E) is called the strongly continuous cosine family if it satisfies
(i) G(0)=I;
(ii) for any t,s∈R, G(t+s)+G(t−s)=2G(t)G(s);
(iii) for each x∈E, t↦G(t)x is continuous on R.
Set
T(t)y:=∫t0G(θ)ydθ, ∀t∈R,y∈E. |
Then {T(t):t∈R} is called the sine family corresponding to {G(t):t∈R}. Let
D(A)={y∈E:G(t)y∈C2(R,E)}, |
Ay=d2dt2G(t)y|t=0, ∀y∈D(A). |
Then A generates a cosine family {G(t):t∈R}. Therefore, we make the following assumption on A.
(P1) A:D(A)⊆E→E generates a strongly continuous cosine family {G(t):t≥0} and
‖G(t)‖B≤M, ∀t≥0, |
where M≥1 is a constant.
Let β=α2. Then β∈(12,1). We recall the function
Mϱ(θ)=∞∑m=0(−θ)mm!Γ(1−ϱ(m+1)), θ∈C, ϱ∈(0,1), |
where C is the imaginary line.
By [7], the following definition and lemmas are achieved.
Definition 2.2. [7] For each v∈L2(U,H), y∈C([−r,c],E) is called the mild solution of (1.1) if y(t)=ϕ(t) for t∈[−r,0], y′(0)=y1 and
y(t)=Ψβ(t)+∫t0Pβ(t−s)[f(s,ys)+Bv(s)]ds, t∈U, |
where
Ψβ(t)=Cβ(t)ϕ(0)+Kβ(t)y1,Cβ(t)=∫∞0Mβ(θ)G(tβθ)dθ,Kβ(t)=∫t0Cβ(θ)dθ,Pβ(t)=∫∞0βθtβ−1Mβ(θ)T(tβθ)dθ. |
Lemma 2.1. [7] Let (P1) hold. Then for any t≥0 and y∈E, we have
‖Cβ(t)y‖≤M‖y‖, |
‖Kβ(t)y‖≤M‖y‖t, |
‖Pβ(t)y‖≤M‖y‖Γ(2β)t2β−1. |
Lemma 2.2. [7] If (P1) is fulfilled, then
(i) {Cβ(t):t≥0} is strongly continuous;
(ii) {Kβ(t):t≥0} and {Pβ(t):t≥0} are uniformly continuous;
(iii) Pβ(t) is a compact operator for t>0 if T(t),t>0, is compact.
By Lemma 2.9 of [8], we can achieve the following lemma.
Lemma 2.3. [8] If (P1) holds and T(t) is compact for t>0, the operator Φ:L2(U,E)→C(U,E), defined by
(Φϖ)(t)=∫t0Pβ(t−s)ϖ(s)ds, ∀ϖ∈L2(U,E), |
is compact.
For the nonlinear term f, we make the assumptions below.
(P2) f:U×C([−r,0],E)→E is continuous and for each R>0, there is K(R)>0 satisfying
‖f(t,ψ1)−f(t,ψ2)‖≤K(R)‖ψ1−ψ2‖C([−r,0],E) |
for any t∈U and ψj∈C([−r,0],E) with ‖ψj‖C([−r,0],E)≤R,j=1,2.
(P3) There is φ∈L2(U,R+) satisfying
‖f(t,ψ)‖≤φ(t), ∀t∈U, ψ∈C([−r,0],E). |
Lemma 2.4. Let assumptions (P1) and (P3) hold. For each v∈L2(U,H), if y∈C([−r,c],E) is the mild solution of (1.1) associated with v, there is R>0 satisfying
‖y‖C([−r,c],E)≤R. |
Proof. By Definition 2.2, we have y(t)=ϕ(t) for t∈[−r,0]. Then ‖y‖C([−r,0],E)≤‖ϕ‖C([−r,0],E).
If t∈[0,c], by (P1) and (P3), we have
‖y(t)‖≤M‖ϕ(0)‖+Mc‖y1‖+MΓ(2β)∫t0(t−θ)2β−1‖f(θ,yθ)‖dθ+MΓ(2β)∫t0(t−θ)2β−1‖Bv(θ)‖dθ≤M‖ϕ(0)‖+Mc‖y1‖+MΓ(2β)∫t0(t−θ)2β−1φ(θ)dθ+MM1Γ(2β)∫t0(t−θ)2β−1‖v(θ)‖dθ≤M‖ϕ(0)‖+Mc‖y1‖+MσΓ(2β)‖φ‖L2+MM1σΓ(2β)‖v‖L2:=R∗, |
where σ=c2β−12√4β−1. Choosing R:=R∗+‖ϕ‖C([−r,0],E), we get
‖y‖C([−r,c],E)≤R. |
This completes the proof.
Definition 2.3. For each ˉy∈E, if there is v∈L2(U,H) such that the control system (1.1) has a mild solution y∈C([−r,c],E) corresponding to v satisfying y(c)=ˉy, then the control system (1.1) is called exactly controllable on [−r,c].
Define an operator W by
Wv=∫b0Pβ(b−s)Bv(s)ds. |
Obviously, W:L2(U,H)→E is a linear operator.
(P4) (i)W−1 exists and takes values in L2(U,H)∖KerW.
(ii) There is M2>0 such that
‖W−1‖≤M2. |
According to (P4) and the definition of W, we choose a control vy∈L2(U,H) by
vy(t)=W−1[ˉy−Φβ(c)−∫c0Pβ(c−θ)f(θ,yθ)dθ](t), t∈U. | (2.1) |
If y∈C([−r,c],E) is a mild solution of (1.1) associated with vy, by (2.1) and Definition 2.2, we have
y(c)=Ψβ(c)+∫c0Pβ(c−θ)[f(θ,yθ)+Bv(θ)]dθ=Ψβ(c)+∫c0Pβ(c−θ)f(θ,yθ)dθ+∫c0Pβ(c−θ)BW−1[ˉy−Φβ(c)−∫c0Pβ(c−s)f(s,ys)ds](θ)dθ=ˉy. |
This fact implies that (1.1) is exactly controllable according to Definition 2.3.
Lemma 2.5. Let (P1),(P3) and (P4) hold. For any y∈C([−r,c],E), there is K1>0 satisfying
‖vy‖L2≤K1. |
Proof. For any y∈C([−r,c],E), by (P1),(P3) and (P4), we have
‖vy‖L2=(∫b0‖vy(t)‖2dt)12≤M2c12[‖ˉy‖+M‖ϕ(0)‖+Mc‖y1‖+MΓ(2β)∫c0(c−θ)2β−1‖f(θ,yθ)‖dθ]≤M2c12[‖ˉy‖+M‖ϕ(0)‖+Mc‖y1‖+MΓ(2β)∫c0(c−θ)2β−1φ(θ)dθ]≤M2c12[‖ˉy‖+M‖ϕ(0)‖+Mc‖y1‖+MσΓ(2β)‖φ‖L2]:=K1. |
This completes the proof.
For any R>0, put BC(R):={y∈C([−r,c],E):‖y‖C([−r,c],E)≤R}.
Lemma 2.6. Let (P1),(P2) and (P4) hold. For any y1,y2∈BC(R), there is K2>0 satisfying
‖vy1(t)−vy2(t)‖≤K2‖y1−y2‖C([−r,c],E), ∀t∈U. |
Proof. For any y1,y2∈BC(R), by (P1),(P2) and (P4), we have
‖vy1(t)−vy2(t)‖≤MM2Γ(2β)∫c0(c−θ)2β−1‖f(θ,y1θ)−f(θ,y2θ)‖dθ≤MM2K(R)Γ(2β)∫c0(c−θ)2β−1‖y1θ−y2θ‖dθ≤MM2K(R)c2βΓ(2β+1)‖y1−y2‖C([−r,c],E). |
By choosing K2=MM2K(R)c2βΓ(2β+1), we obtain the desired conclusion.
Theorem 3.1. Let (P1)−(P4) be fulfilled. Then the control system (1.1) is exactly controllable on [−r,c] provided that
MK(R)c2βΓ(2β+1)(1+MM1M2c2βΓ(2β+1))<1. | (3.1) |
Proof. Defined Q:C([−r,c],E)→C([−r,c],E) by
(Qy)(t)={Ψβ(t)+∫t0Pβ(t−s)[f(s,ys)+Bvy(s)]ds, t∈U,ϕ(t), t∈[−r,0]. | (3.2) |
By Definition 2.2 we know that the mild solution of (1.1) is equivalent to the fixed point of Q.
Let R≥M‖ϕ(0)‖+Mc‖y1‖+MσΓ(2β)‖φ‖L2+MM1σΓ(2β)K1+‖ϕ‖C([−r,0],E). We first prove that Q(BC(R))⊆BC(R). For any y∈BC(R), it is easy to see
‖Qy‖C([−r,0],E)≤‖ϕ‖C([−r,0],E). | (3.3) |
For t∈[0,c], by (P1),(P3) and Lemma 2.5, we have
‖(Qy)(t)‖≤‖Ψβ(t)‖+MΓ(2β)∫t0(t−θ)2β−1‖f(θ,yθ)‖dθ+MΓ(2β)∫t0(t−θ)2β−1‖Bvy(θ)‖dθ≤M‖ϕ(0)‖+Mc‖y1‖+MΓ(2β)∫t0(t−θ)2β−1φ(θ)dθ+MM1Γ(2β)∫t0(t−θ)2β−1‖vy(θ)‖dθ≤M‖ϕ(0)‖+Mc‖y1‖+MσΓ(2β)‖φ‖L2+MM1σΓ(2β)K1. |
This fact, together with (3.3), yields that
‖Qy‖C([−r,c],E)≤R. |
Thus, Q maps BC(R)) into itself.
Then, we claim that Q:BC(R))→BC(R)) is a contraction mapping. For any y1,y2∈BC(R)), if t∈[−r,0], (Qy1)(t)=(Qy2)(t)=ϕ(t). If t∈[0,c], by (P1),(P2) and Lemma 2.6, we achieve that
‖(Qy1)(t)−(Qy2)(t)‖≤MΓ(2β)∫t0(t−θ)2β−1‖f(θ,y1θ)−f(θ,y2θ)‖dθ+MM1Γ(2β)∫t0(t−θ)2β−1‖vy1(θ)−vy2(θ)‖dθ≤MK(R)Γ(2β)∫t0(t−θ)2β−1‖y1θ−y2θ‖C([−r,0],E)dθ+MM1Γ(2β)∫t0(t−θ)2β−1‖vy1(θ)−vy2(θ)‖dθ≤Mc2βΓ(2β+1)(K(R)+M1K2)‖y1−y2‖C([−r,c],E). |
According to (3.1) we deduce that Q:BC(R))→BC(R)) is a contraction mapping.
As such, Q has a unique fixed point y∈BC(R))⊂C([−r,c],E), which is the mild solution of (1.1).
Remark 3.1. Since the global Lipschitz continuity contains local Lipschitz continuity (but the reverse is not true), Theorem 3.1 is an improvement of Theorem 4.1 of [7].
Theorem 3.2. Let (P1),(P3) and (P4) hold. If f:U×C([−r,0],E)→E is continuous, and the condition (P5) is satisfied, where
(P5) For any t∈U and R>0, the set
{Pβ(t−s)f(s,x):s∈[0,t],‖x‖C([−r,0],E)≤R} |
is relatively compact in E, then the system (1.1) is exactly controllable on [−r,c].
Proof. Put the operator Q:C([−r,c],E)→C([−r,c],E) as in (3.2). It follows from the proof of Theorem 3.1 that Q(BC(R))⊆BC(R) for some R>0 and Q:BC(R)→BC(R) is continuous.
Next, we will show that Q is a compact operator, that is, Q(BC(R)) is relatively compact. By the Ascoli-Arzela theorem, it suffices to prove that Q(BC(R)) is equicontinuous and {(Qy)(t):y∈BC(R)} is relatively compact for t∈[−r,c]. By employing Lemma 2.2(i)(ii), the equicontinuity of Q(BC(R)) can be verified using the proof of Theorem 4.2 of [7]. Since (Qy)(t)≡ϕ(t) for t∈[−r,0], it remains to prove that {(Qy)(t):y∈BC(R)} is relatively compact for t∈U. By Lemma 2.5 and (P5), we obtain that
Ξ(t):={Pβ(t−s)[f(s,ys)+Bvy(s)]:s∈[0,t],y∈BC(R)} | (3.4) |
is relatively compact in E for t∈U. Hence, we can infer from (3.4) that
∫t0Pβ(t−s)[f(s,ys)+Bvy(s)ds∈t ¯convΞ(t), ∀t∈U, |
where ¯convΞ(t) represents the convex closure of Ξ(t). Therefore, Q(BC(R)) is relatively compact and Q:BC(R)→BC(R) is completely continuous. According to Schauder's fixed point theorem, there is a function y∈Q(BC(R)) satisfying y=Qy and y(c)=ˉy. Thus the system (1.1) is exactly controllable on [−r,c].
Obviously, if f is uniformly bounded, the assumption (P3) holds automatically. In this case, if we suppose that T(t) is compact for t>0, then the assumption (P5) is fulfilled. Hence, according to Theorem 3.2, the corollary is acquired below.
Corollary 3.11. Let (P1) and (P4) hold. In addition, f:U×C([−r,0],E)→E is continuous and uniformly bounded, T(t) is compact for t>0. Then the system (1.1) is exactly controllable on [−r,c].
Remark 3.2. Obviously, if f is completely continuous, the assumption (P5) hold automatically.
Furthermore, if we achieve the compactness of T(t) for t>0, by Lemma 2.2(iii) and Lemma 2.3, the assumption (P3) yields that
{∫t0Pβ(t−s)[f(s,ys)+Bvy(s)ds:s∈[0,t],y∈BC(R)} |
is relatively compact for t∈U. By the proof of Theorem 3.2, we can acquire the relative compactness of {(Qy)(t):y∈BC(R)} for t∈[−r,c]. Hence, the uniform boundedness of f in Corollary 3.11 can be removed.
Theorem 3.3. Let (P1),(P3) and (P4) hold. In addition, f:U×C([−r,0],E)→E is continuous and T(t) is compact for t>0. Then the system (1.1) is exactly controllable on [−r,c].
From Corollary 3.1 and Theorem 3.3, we can see that the assumption (P5) and the compactness of T(t) for t>0 are too strong. It is of interesting to weaken or remove such assumptions. Next, we will apply the measure of noncompactness method to discuss the exact controllability of (1.1).
Let E be a Banach space and D⊂E a bounded subset of E. We define
χ(D):=inf{ϵ>0:D has finite ϵ-net in E} |
the Hausdorff measure of noncompactness in E. If D⊂C(U,E) is bounded, D(t):={y(t):y∈D}⊂E is bounded for each t∈U and χ(D(t))≤χ(D).
Lemma 3.1. [10] If D⊂E is bounded, then there exists a countable subset D0⊂D such that
χ(D)≤2χ(D0). |
Lemma 3.2. [11] If D⊂C(U,E) is bounded and equicontinuous, then χ(D(t)) is continuous for t∈U and
χ(D)=supt∈U‖χ(D(t))‖. |
Lemma 3.3. [12] Let D:={yn}⊂C(U,E) be countable. If there is ω∈L1(U) such that, for each n≥1, yn(t)≤ω(t) a.e., then χ(D(t)) is Lebesgue integrable on U and
χ({∫Uyn(t)dt})≤2∫Uχ(D(t))dt. |
Furthermore, we make the assumptions below.
(P6) f:U×C([−r,0],E)→E is continuous and there is a function η∈L2(U,R+) such that for each bounded subset D1⊂C([−r,0],E), we have
χ(f(t,D1))≤η(t)sup−r≤s≤0χ(D1(s)), ∀t∈U. |
(P7) There is a constant L>0 such that
χ(W−1(D2)(t))≤Lχ(D2), ∀t∈U |
for each bounded subset D2⊂E.
Theorem 3.4. Let (P1),(P3),(P4),(P6) and (P7) be fulfilled and
MσΓ(2β)(1+2MLM1c2βΓ(2β+1))‖η‖Ł2<14. | (3.5) |
Then, the system (1.1) is exactly controllable on [−r,c].
Proof. From the Theorem 3.2 and its proof, we obtain that Q:BC(R)→BC(R), defined as in (3.2), is continuous and equicontinuous. Next, we will verify that Q:BC(R)→BC(R) is a condensing mapping using (P6) and (P7).
Since for any θ∈U, we have
sup−r≤τ≤0χ({yθ(τ):y∈BC(R)})≤sup0≤τ≤0χ({y(τ):y∈BC(R)})≤χ(BC(R)), | (3.6) |
according to (P6),(P7), (3.6) and (2.1), we can deduce that
χ({Bvy(s):y∈BC(R)})≤2MM1LσΓ(2β)‖η‖L2χ({BC(R)}). | (3.7) |
Since Q(BC(R)) is bounded and equicontinuous, according to Lemma 3.1 and Lemma 3.2, there is a countable subset {yn:n≥1}⊂BC(R) such that
χ(Q(BC(R)))≤ 2χ({(Qyn):n≥1})= 2supt∈[−r,c]χ({(Qyn)(t):n≥1}). | (3.8) |
Obviously, for t∈[−r,0], (Qyn)(t)≡ϕ(t) for n≥1, so
χ({(Qyn)(t):n≥1})=0. |
For t∈U, by (3.6), (3.7) and Lemma 3.3, we can infer that
χ({(Qyn)(t):n≥1})≤ 2MΓ(2β)∫t0(t−s)2β−1χ({f(s,yns)+Bvyn(s):n≥1})ds≤ 2MΓ(2β)∫t0(t−s)2β−1η(s)sup−r≤θ≤0χ({yns(θ):n≥1})ds+2MΓ(2β)∫t0(t−s)2β−1χ({Bvyn(s):n≥1})ds≤ 2MσΓ(2β)(1+2MM1Lc2βΓ(2β+1))‖η‖Ł2χ(BC(R)). |
The above facts together with (3.8) yield that
χ(Q(BC(R)))≤ 2supt∈[−r,0]χ({(Qyn)(t):n≥1})+2supt∈Uχ({(Qyn)(t):n≥1})≤ 4MσΓ(2β)(1+2MM1Lc2βΓ(2β+1))‖η‖Ł2χ(BC(R)). |
According to (3.5), we acquire that Q:BC(R)→BC(R) is a condensing mapping. By Sadovskii's fixed point theorem, there exists y∈BC(R) satisfying y=Qy and y(c)=ˉy. Therefore, the system (1.1) is exactly controllable on [−r,c].
Remark 3.3. In Theorem 3.4, we remove the assumption (P5) and the compactness of the sine family {T(t):t≥0}, which are essential assumptions in [7,8]. Hence, our results extend many existing research works.
Remark 3.4. In [7], under the global Lipschitz condition or certain compactness conditions on nonlinear term f, the exact controllability of the Caputo fractional evolution equations without delay was investigated. Compared with the main results of [7], we consider the delayed control system (1.1). Theorem 3.1 is obtained when the nonlinear term f is locally Lipschitz continuous. Theorem 3.2 and Theorem 3.3 are achieved under certain compactness conditions. The measure of noncompactness conditions are applied in Theorem 3.4. Therefore, our conclusions improve the major results of [7].
Let Ω⊂RN be an open subset with Dirichlet boundary conditions. We focus on the fractional delayed evolution system
{C∂32ty(t,z)=Δy(t,z)+f(t,z,yt)+Bv(t,z), t∈(0,1], z∈Ω, α∈(1,2),y(t,z)=ϕ(t,z), ∀t∈[−r,0],y′(0,z)=y1(z), | (4.1) |
where C∂32t represents the fractional partial derivative operator on t of order 32 in the Caputo sense, Δ represents the Laplace operator, v∈L2([0,1]×Ω,L2(Ω)) stands for the control function. f is the nonlinear function satisfying the following conditions.
(A1) f:[0,1]×Ω×C([−r,0],L2(Ω))→L2(Ω) is continuous and for each R>0, there exists a constant K(R)>0 such that
‖f(t,z,ϕ1)−f(t,z,ϕ2)‖L2(Ω)≤K(R)‖ϕ1−ϕ2‖C([−r,0],L2(Ω)) |
for any t∈[0,1] and ϕj∈C([−r,0],L2(Ω)) with ‖ϕj‖C([−r,0],L2(Ω))≤R, j=1,2.
(A2) There is φ∈L2([0,1],R+) such that
‖f(t,z,ϕ)‖L2(Ω)≤φ(t) |
for any t∈[0,1],z∈Ω and ϕ∈C([−r,0],L2(Ω)).
Let E=H=L2(Ω). We define
D(A)=W2,2(Ω)∩W1,20(Ω), |
Ay=Δy. |
Then, by [7,13], A:D(A)⊆E→E generates a strongly continuous cosine family {G(t):t≥0} in E satisfying ‖G(t)‖B≤1 for every t≥0.
Define B:H→E by
Bv=∞∑n=1μn⟨ˆv,ϖn⟩ϖn, |
where
ˆv={⟨v,ϖn⟩, n=1,2,⋯,ℓ,0, n=ℓ+1,ℓ+2,⋯ |
for ℓ∈N. μn=n2π2 is eigenvalues of A with the corresponding eigenvectors ϖn(z)=√2πsin(nπz) for n∈N. From [7], there is a positive constant M1 satisfying ‖B‖B≤M1.
Define the operator W:L2([0,1],L2(Ω))→L2(Ω) by
Wv=∫10P34(1−s)Bv(s)ds, |
where
P34(t)=t−14∫∞034θM34(θ)T(t34θ)dθ, t∈[0,1] |
and {T(t):t≥0} is the sine family corresponding to {G(t):t≥0} generated by A.
(A3) W−1 exists and takes values in L2([0,1],L2(Ω))∖KerW and there is M2>0 such that
‖W−1‖≤M2. |
Thus, we can rewrite the fractional delayed evolution system (4.1) into the abstract fractional control system (1.1). By Theorem 3.1, we can achieve the cxact controllability result.
Theorem 4.1. Assume that conditions (A1)−(A3) hold. Then the fractional delayed evolution system (4.1) is exactly controllable provided that
K(R)Γ(52)(1+M1M2Γ(52))<1. |
This paper deal with the exact controllability of the control system govern by evolution equations involving Caputo fractional derivatives of order α∈(1,2) in abstract spaces. At first, the exact controllability of the delayed system (1.1) is studied when f is local Lipschitz continuous. Then, the certain compactness conditions and the measure of noncompactness conditions are employed to demonstrate the exact controllability of (1.1) in this article. The results improve and generalize the conclusions of many researchers. In the future, the method can be applied to study the controllability of the Sobolev-type fractional evolution equations. By utilizing the compactness of the Sobolev operator, we can delete compactness conditions on the nonlinear term f and the sine family {T(t):t≥0}.
The author declare that they have not used Artificial Intelligence (AI) tools in the creation of this article.
The research is supported by the NNSF of China (No. 32060581).
The author declares that there is no conflict of interest.
[1] |
T. A. Burton, B. Zhang, Periodic solutions of abstract differential equations with infinite delay, J. Differ. Equ. , 90 (1991), 357–396. https://dx.doi.org/10.1016/0022-0396(91)90153-Z doi: 10.1016/0022-0396(91)90153-Z
![]() |
[2] | D. Henry, Geometric theory of semilinear parabolic equations, Berlin, Heidelberg: Springer, 1981. https://dx.doi.org/10.1007/BFb0089647 |
[3] |
K. X. Li, J. G. Peng, J. X. Jia, Cauchy problems for fractional differential equations with Riemann-Liouville fractional derivatives, J. Funct. Anal. , 263 (2012), 476–510. https://dx.doi.org/10.1016/j.jfa.2012.04.011 doi: 10.1016/j.jfa.2012.04.011
![]() |
[4] |
Y. N. Li, H. R. Sun, Z. S. Feng, Fractional abstract Cauchy problem with order α∈(1,2), Dyn. Partial Differ. Equ. , 13 (2016), 155–177. https://dx.doi.org/10.4310/DPDE.2016.v13.n2.a4 doi: 10.4310/DPDE.2016.v13.n2.a4
![]() |
[5] |
X. B. Shu, Q. Q. Wang, The existence and uniqueness of mild solutions for fractional differential equations with nonlocal conditions of order 1<α<2, Comput. Math. Appl. , 64 (2012), 2100–2110. https://dx.doi.org/10.1016/j.camwa.2012.04.006 doi: 10.1016/j.camwa.2012.04.006
![]() |
[6] |
H. Yang, Approximate controllability of Sobolev type fractional evolution equations of order α∈(1,2) via resolvent operators, J. Appl. Anal. Comput. , 11 (2021), 2981–3000. https://dx.doi.org/10.11948/20210086 doi: 10.11948/20210086
![]() |
[7] |
Y. Zhou, J. W. He, New results on controllability of fractional evolution systems with order α∈(1,2), Evol. Equ. Control Theory, 10 (2021), 491–509. https://dx.doi.org/10.3934/eect.2020077 doi: 10.3934/eect.2020077
![]() |
[8] |
H. Yang, Existence and approximate controllability of Riemann-Liouville fractional evolution equations of order 1<μ<2 with weighted time delay, Bull. Sci. Math. , 187 (2023), 103303. https://doi.org/10.1016/j.bulsci.2023.103303 doi: 10.1016/j.bulsci.2023.103303
![]() |
[9] | C. Travis, G. Webb, Consine families and abstract nonlinear second order differential equations, Acta Math. Hungar. , 32 (1978), 75–96. |
[10] | Y. X. Li, Existence of solutions of initial value problems for abstract semilinear evolution equations (in Chinese), Acta. Math. Sin., 48 (2005), 1089–1094. |
[11] | D. J. Guo, J. X. Sun, Ordinary differential equations in abstract spaces (in Chinese), Jinan: Shandong Science and Technology, 1989. |
[12] |
H. P. Heinz, On the behaviour of measure of noncompactness with respect to differentiation and integration of vector-valued functions, Nonlinear Anal. Theor., 7 (1983), 1351–1371. https://dx.doi.org/10.1016/0362-546X(83)90006-8 doi: 10.1016/0362-546X(83)90006-8
![]() |
[13] | W. Arendt, C. J. K. Batty, M. Hieber, F. Neubrander, Vector-valued Laplace transforms and Cauchy problems, 2 Eds., Birkhäuser Basel, 2011. https://doi.org/10.1007/978-3-0348-0087-7 |