On equilibrium in control problems with applications to evolution systems

Abstract

In this paper we examine a mutual control problem for systems of two abstract evolution equations subject to a proportionality final condition. Related observability and semi-observability problems are discussed. The analysis employs a vector fixed-point approach, using matrices rather than constants, and applies the technique of Bielecki equivalent norms.

Authors

Radu Precup
Department of Mathematics Babes-Bolyai University, Cluj-Napoca, Romania
Tiberiu Popoviciu Institute of Numerical Analysis, Romanian Academy, Cluj-Napoca, Romania

Andrei Stan
Department of Mathematics Babeş-Bolyai University, Cluj-Napoca, Romania
Tiberiu Popoviciu Institute of Numerical Analysis, Romanian Academy, Cluj-Napoca, Romania

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R. Precup, A. Stan, On equilibrium in control problems with applications to evolution systems, arXiv:2409.09805, 2024.

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On equilibrium in control problems with applications to evolution systems

Radu Precup Faculty of Mathematics and Computer Science and Institute of Advanced Studies in Science and Technology, Babeş-Bolyai University, 400084 Cluj-Napoca, Romania & Tiberiu Popoviciu Institute of Numerical Analysis, Romanian Academy, P.O. Box 68-1, 400110 Cluj-Napoca, Romania  and  Andrei Stan A. Stan, Department of Mathematics, Babeş-Bolyai University, 400084 Cluj-Napoca, Romania & Tiberiu Popoviciu Institute of Numerical Analysis, Romanian Academy, P.O. Box 68-1, 400110 Cluj-Napoca, Romania
Abstract.

In this paper we examine a mutual control problem for systems of two abstract evolution equations subject to a proportionality final condition. Related observability and semi-observability problems are discussed. The analysis employs a vector fixed-point approach, using matrices rather than constants, and applies the technique of Bielecki equivalent norms.

Key words and phrases:
evolution equation; control; fixed point; semigroup
2010 Mathematics Subject Classification:
47J35, 34K35, 47H10

1. Introduction

In a recent paper [16], we introduced the concept of mutual control related to systems whose unknowns exert some control over each other. More exactly, we have considered four sets D1subscript𝐷1D_{1}italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT, D2subscript𝐷2D_{2}italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT , C1subscript𝐢1C_{1}italic_C start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT, C2subscript𝐢2C_{2}italic_C start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT with C1βŠ‚D1Γ—D2subscript𝐢1subscript𝐷1subscript𝐷2C_{1}\subset D_{1}\times D_{2}italic_C start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT βŠ‚ italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT, C2βŠ‚D2Γ—D1subscript𝐢2subscript𝐷2subscript𝐷1C_{2}\subset D_{2}\times D_{1}italic_C start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT βŠ‚ italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT Γ— italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT, a linear space Z,𝑍Z,italic_Z , two mappings E1subscript𝐸1E_{1}italic_E start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT, E2:D1Γ—D2β†’Z,:subscript𝐸2β†’subscript𝐷1subscript𝐷2𝑍E_{2}:D_{1}\times D_{2}\rightarrow Z,italic_E start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT : italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT β†’ italic_Z , and the problem

{E1⁒(x,y)=0ZE2⁒(x,y)=0Z(x,y)∈C1,(y,x)∈C2.casessubscript𝐸1π‘₯𝑦subscript0𝑍otherwisesubscript𝐸2π‘₯𝑦subscript0𝑍otherwiseformulae-sequenceπ‘₯𝑦subscript𝐢1𝑦π‘₯subscript𝐢2otherwise\begin{cases}E_{1}(x,y)=0_{Z}\\ E_{2}(x,y)=0_{Z}\\ (x,y)\in C_{1},(y,x)\in C_{2}.\end{cases}{ start_ROW start_CELL italic_E start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) = 0 start_POSTSUBSCRIPT italic_Z end_POSTSUBSCRIPT end_CELL start_CELL end_CELL end_ROW start_ROW start_CELL italic_E start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) = 0 start_POSTSUBSCRIPT italic_Z end_POSTSUBSCRIPT end_CELL start_CELL end_CELL end_ROW start_ROW start_CELL ( italic_x , italic_y ) ∈ italic_C start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , ( italic_y , italic_x ) ∈ italic_C start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT . end_CELL start_CELL end_CELL end_ROW

In this context, y𝑦yitalic_y controls the state xπ‘₯xitalic_x in the first equation, and xπ‘₯xitalic_x controls the state y𝑦yitalic_y in the second. The controllability conditions on xπ‘₯xitalic_x and y𝑦yitalic_y are expressed by the appartenence to the sets C1subscript𝐢1C_{1}italic_C start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT and C2subscript𝐢2C_{2}italic_C start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT, respectively. We call this problem the mutual control problem.

One way to solve such a problem, is to incorporate the controllability conditions into the equations and give the problem a fixed point formulation

(x,y)∈(N1⁒(x,y),N2⁒(x,y)),π‘₯𝑦subscript𝑁1π‘₯𝑦subscript𝑁2π‘₯𝑦\left(x,y\right)\in\left(N_{1}(x,y),\ N_{2}(x,y)\right),( italic_x , italic_y ) ∈ ( italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) ) ,

where N1,N2subscript𝑁1subscript𝑁2N_{1},N_{2}italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT are set-valued mappings N1:D1Γ—D2β†’D1,:subscript𝑁1β†’subscript𝐷1subscript𝐷2subscript𝐷1N_{1}:D_{1}\times D_{2}\rightarrow D_{1},italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT : italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT β†’ italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , N2:D1Γ—D2β†’D2.:subscript𝑁2β†’subscript𝐷1subscript𝐷2subscript𝐷2N_{2}:D_{1}\times D_{2}\rightarrow D_{2}.italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT : italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT β†’ italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT . A solution (x,y)π‘₯𝑦\left(x,y\right)( italic_x , italic_y ) of this fixed point equation is said to be a solution of the mutual control problem, while the problem is said to be mutually controllable if such a solution exists.

Also, in [16], we showed that the concept of mutual controllability is related to the notion of equilibrium in general, and includes in particular the concept of a Nash equilibrium ([2, 8, 10, 11, 14, 15, 17, 18, 19]).

In this paper, we illustrate the notion of a mutual control by studying a system of abstract evolution equations

(1.1) {x′⁒(t)=A⁒x⁒(t)+F⁒(x⁒(t),y⁒(t))y′⁒(t)=A⁒y⁒(t)+G⁒(x⁒(t),y⁒(t))⁒t∈[0,T],casessuperscriptπ‘₯′𝑑𝐴π‘₯𝑑𝐹π‘₯𝑑𝑦𝑑otherwisesuperscript𝑦′𝑑𝐴𝑦𝑑𝐺π‘₯𝑑𝑦𝑑otherwise𝑑0𝑇\begin{cases}x^{\prime}(t)=A\,x(t)+F\left(x(t),y(t)\right)\\ y^{\prime}(t)=A\,y(t)+G\left(x(t),y(t)\right)\end{cases}t\in[0,T],{ start_ROW start_CELL italic_x start_POSTSUPERSCRIPT β€² end_POSTSUPERSCRIPT ( italic_t ) = italic_A italic_x ( italic_t ) + italic_F ( italic_x ( italic_t ) , italic_y ( italic_t ) ) end_CELL start_CELL end_CELL end_ROW start_ROW start_CELL italic_y start_POSTSUPERSCRIPT β€² end_POSTSUPERSCRIPT ( italic_t ) = italic_A italic_y ( italic_t ) + italic_G ( italic_x ( italic_t ) , italic_y ( italic_t ) ) end_CELL start_CELL end_CELL end_ROW italic_t ∈ [ 0 , italic_T ] ,

together with the controllability condition

(1.2) x⁒(T)βˆ’a⁒x⁒(0)=k⁒(y⁒(T)βˆ’b⁒y⁒(0)).π‘₯π‘‡π‘Žπ‘₯0π‘˜π‘¦π‘‡π‘π‘¦0x\left(T\right)-ax(0)=k\left(y\left(T\right)-by\left(0\right)\right).italic_x ( italic_T ) - italic_a italic_x ( 0 ) = italic_k ( italic_y ( italic_T ) - italic_b italic_y ( 0 ) ) .

Here, a,b,k>0π‘Žπ‘π‘˜0a,b,k>0italic_a , italic_b , italic_k > 0 are given numbers, A𝐴Aitalic_A is a linear operator generating a semigroup of operators, and F,G:X2β†’X:𝐹𝐺→superscript𝑋2𝑋F,G:X^{2}\rightarrow Xitalic_F , italic_G : italic_X start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT β†’ italic_X are continuous mappings.

We note that the controllability condition (1.2) under consideration is non-standard. Unlike the conventional requirement [3], [21], where the final values x⁒(T)π‘₯𝑇x\left(T\right)italic_x ( italic_T ) and y⁒(T)𝑦𝑇y\left(T\right)italic_y ( italic_T ) of the two unknowns are specified, it instead demands a proportional relationship between their deviations from the initial states x⁒(0)π‘₯0x\left(0\right)italic_x ( 0 ) and y⁒(0),𝑦0y\left(0\right),italic_y ( 0 ) , respectively.

Such a control condition is of interest in dynamics of populations when it expresses the requirement that at a certain moment T𝑇Titalic_T the ratio between proliferations of two populations, for example prey and predators, should be the desired k.π‘˜k.italic_k . Similarly, for the control of epidemics, it expresses the requirement that at some time one reach a certain ratio between the infected population and that susceptible to infection. Analogous interpretations can be given in the case of some chemical or medical reaction models.

Our results target two aspects:

a):

The problem as an observability one, consisting in determination of the initial states x⁒(0)π‘₯0x\left(0\right)italic_x ( 0 ) and y⁒(0)𝑦0y\left(0\right)italic_y ( 0 ) from the observable final relations;

b):

A semi-observability problem, that is, finding a solution of the mutual problem when only one of the initial states is given, consequently leading to the determination of the other initial state.

We solve the problem (1.1)-(1.2) using an equivalent formulation as a fixed-point equation. This approach allows for the application of vector techniques based on fixed-point theorems, Bielecki-type norms, and matrices instead of constants. The advantages of each fixed-point method are emphasized, considering specific assumptions about F𝐹Fitalic_F and G𝐺Gitalic_G to ensure uniqueness and localization of the solutions.

2. Preliminaries

Let (X,|β‹…|X)\left(X,|\cdot|_{X}\right)( italic_X , | β‹… | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ) be a Banach space, and let ℒ⁑(X)ℒ𝑋\operatorname{\mathcal{L}}(X)caligraphic_L ( italic_X ) be the set of all bounded linear operators from X𝑋Xitalic_X to X𝑋Xitalic_X. Endowed with the norm

|U|ℒ⁒(X)=supx∈Xβˆ–{0}|U⁒x|X|x|X,subscriptπ‘ˆβ„’π‘‹subscriptsupremumπ‘₯𝑋0subscriptπ‘ˆπ‘₯𝑋subscriptπ‘₯𝑋|U|_{\mathcal{L}(X)}=\sup_{x\in X\setminus\{0\}}\frac{|Ux|_{X}}{|x|_{X}},| italic_U | start_POSTSUBSCRIPT caligraphic_L ( italic_X ) end_POSTSUBSCRIPT = roman_sup start_POSTSUBSCRIPT italic_x ∈ italic_X βˆ– { 0 } end_POSTSUBSCRIPT divide start_ARG | italic_U italic_x | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT end_ARG start_ARG | italic_x | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT end_ARG ,

ℒ⁒(X)β„’X\operatorname{\mathcal{L}(X)}caligraphic_L ( roman_X ) is a Banach space.

2.1. Abstract evolution equations

Let T>0𝑇0T>0italic_T > 0 and A:D⁒(A)βŠ‚Xβ†’X:𝐴𝐷𝐴𝑋→𝑋A\colon D(A)\subset X\rightarrow Xitalic_A : italic_D ( italic_A ) βŠ‚ italic_X β†’ italic_X be the generator of a C0subscript𝐢0C_{0}italic_C start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT-semigroup {S⁒(t):tβ‰₯0}conditional-set𝑆𝑑𝑑0\{S(t)\,:\,t\geq 0\}{ italic_S ( italic_t ) : italic_t β‰₯ 0 }.

A function u∈C⁒([0,T];X)𝑒𝐢0𝑇𝑋u\in C\left([0,T];X\right)italic_u ∈ italic_C ( [ 0 , italic_T ] ; italic_X ) is said to be a mild solution of the equation

u′⁒(t)=A⁒u⁒(t)+F⁒(t,u⁒(t))(t∈[0,T]),superscript𝑒′𝑑𝐴𝑒𝑑𝐹𝑑𝑒𝑑𝑑0𝑇u^{\prime}(t)=Au(t)+F(t,u(t))\ \ \ \,(t\in\left[0,T\right]),italic_u start_POSTSUPERSCRIPT β€² end_POSTSUPERSCRIPT ( italic_t ) = italic_A italic_u ( italic_t ) + italic_F ( italic_t , italic_u ( italic_t ) ) ( italic_t ∈ [ 0 , italic_T ] ) ,

if it satisfies

u⁒(t)=S⁒(t)⁒u⁒(0)+∫0tS⁒(tβˆ’s)⁒F⁒(s,u⁒(s))⁒𝑑s, for all t∈[0,T].𝑒𝑑𝑆𝑑𝑒0superscriptsubscript0𝑑𝑆𝑑𝑠𝐹𝑠𝑒𝑠differential-d𝑠 for all t∈[0,T].u\left(t\right)=S\left(t\right)u(0)+\int_{0}^{t}S\left(t-s\right)F\left(s,u% \left(s\right)\right)ds,\,\text{ for all $t\in[0,T]$.}italic_u ( italic_t ) = italic_S ( italic_t ) italic_u ( 0 ) + ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_t end_POSTSUPERSCRIPT italic_S ( italic_t - italic_s ) italic_F ( italic_s , italic_u ( italic_s ) ) italic_d italic_s , for all italic_t ∈ [ 0 , italic_T ] .

Throughout this paper, the number CAsubscript𝐢𝐴C_{A}italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT stands for upper bound for the norm in ℒ⁒(X)ℒ𝑋\mathcal{L}(X)caligraphic_L ( italic_X ) of the operators S⁒(t)𝑆𝑑S(t)italic_S ( italic_t ), uniform with respect to t∈[0,2⁒T]𝑑02𝑇t\in\left[0,2T\right]italic_t ∈ [ 0 , 2 italic_T ], that is

(2.1) |S⁒(t)|ℒ⁒(X)≀CA, subscript𝑆𝑑ℒ𝑋subscript𝐢𝐴 \left|S(t)\right|_{\mathcal{L}(X)}\leq C_{A},\text{ }| italic_S ( italic_t ) | start_POSTSUBSCRIPT caligraphic_L ( italic_X ) end_POSTSUBSCRIPT ≀ italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ,

for all t∈[0,2⁒T].𝑑02𝑇t\in\left[0,2T\right].italic_t ∈ [ 0 , 2 italic_T ] . If A𝐴Aitalic_A generates a semigroup of contractions, then CA=1.subscript𝐢𝐴1C_{A}=1.italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT = 1 .

For details about semigroups of linear operators and abstract evolution equations we refer to the books [7] and [20].

2.2. Bielecki-type norms

For each number ΞΈβ‰₯0πœƒ0\theta\geq 0italic_ΞΈ β‰₯ 0, on the space C⁒([0,T];X)𝐢0𝑇𝑋C([0,T];X)italic_C ( [ 0 , italic_T ] ; italic_X ), we define the Bielecki norm

|u|ΞΈ:=maxt∈[0,T]⁑eβˆ’ΞΈβ’t⁒|u⁒(t)|X.assignsubscriptπ‘’πœƒsubscript𝑑0𝑇superscriptπ‘’πœƒπ‘‘subscript𝑒𝑑𝑋|u|_{\theta}:=\max_{t\in[0,T]}e^{-\theta t}|u(t)|_{X}.| italic_u | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT := roman_max start_POSTSUBSCRIPT italic_t ∈ [ 0 , italic_T ] end_POSTSUBSCRIPT italic_e start_POSTSUPERSCRIPT - italic_ΞΈ italic_t end_POSTSUPERSCRIPT | italic_u ( italic_t ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT .

Note that when ΞΈ=0,πœƒ0\theta=0,italic_ΞΈ = 0 , the Bieleki norm |β‹…|0\left|\cdot\right|_{0}| β‹… | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT is equivalent to the usual Chebyshev (uniform) norm |β‹…|∞\left|\cdot\right|_{\infty}| β‹… | start_POSTSUBSCRIPT ∞ end_POSTSUBSCRIPT. We mention that with a suitable choice of ΞΈπœƒ\thetaitalic_ΞΈ, the Bielecki-type norms allow us to relax the strict conditions on constants such as Lipschitz or growth conditions required by fixed point theorems.

2.3. Matrices convergent to zero

Dealing with systems of equations it is convenient (see, e.g., [9, 13]) to use a vector approach based on matrices instead of constants.

A square matrix Mβˆˆβ„³nΓ—n⁒(ℝ+)𝑀subscriptℳ𝑛𝑛subscriptℝM\in\mathcal{M}_{n\times n}\left(\mathbb{R}_{+}\right)italic_M ∈ caligraphic_M start_POSTSUBSCRIPT italic_n Γ— italic_n end_POSTSUBSCRIPT ( blackboard_R start_POSTSUBSCRIPT + end_POSTSUBSCRIPT ) is said to be convergent to zero if its power Mksuperscriptπ‘€π‘˜M^{k}italic_M start_POSTSUPERSCRIPT italic_k end_POSTSUPERSCRIPT tends to the zero matrix as kβ†’βˆžβ†’π‘˜k\rightarrow\inftyitalic_k β†’ ∞. The next lemma provides equivalent conditions for a square matrix to be convergent to zero (see, e.g., [9]).

Lemma 2.1.

Let Mβˆˆβ„³nΓ—n⁒(ℝ+)𝑀subscriptℳ𝑛𝑛subscriptℝM\in\mathcal{M}_{n\times n}\left(\mathbb{R}_{+}\right)italic_M ∈ caligraphic_M start_POSTSUBSCRIPT italic_n Γ— italic_n end_POSTSUBSCRIPT ( blackboard_R start_POSTSUBSCRIPT + end_POSTSUBSCRIPT ) be a square matrix. The following statements are equivalent:

(a):

The matrix M𝑀Mitalic_M is convergent to zero.

(b):

The spectral radius of M𝑀Mitalic_M is less than 1111, i.e., ρ⁒(M)<1πœŒπ‘€1\rho(M)<1italic_ρ ( italic_M ) < 1.

(c):

The matrix Iβˆ’M,𝐼𝑀I-M,italic_I - italic_M , where I𝐼Iitalic_I is the unit matrix of the same size, is invertible and its inverse has nonnegative entries, i.e., (Iβˆ’M)βˆ’1βˆˆβ„³nΓ—n⁒(ℝ+).superscript𝐼𝑀1subscriptℳ𝑛𝑛subscriptℝ\left(I-M\right)^{-1}\in\mathcal{M}_{n\times n}\left(\mathbb{R}_{+}\right).( italic_I - italic_M ) start_POSTSUPERSCRIPT - 1 end_POSTSUPERSCRIPT ∈ caligraphic_M start_POSTSUBSCRIPT italic_n Γ— italic_n end_POSTSUBSCRIPT ( blackboard_R start_POSTSUBSCRIPT + end_POSTSUBSCRIPT ) .

In case n=2𝑛2n=2italic_n = 2, we have the following characterization.

Lemma 2.2.

A square matrix M=[ai⁒j]1≀i,j≀2βˆˆβ„³2Γ—2⁒(ℝ+)𝑀subscriptdelimited-[]subscriptπ‘Žπ‘–π‘—formulae-sequence1𝑖𝑗2subscriptβ„³22subscriptℝM=[a_{ij}]_{1\leq i,j\leq 2}\in\mathcal{M}_{2\times 2}\left(\mathbb{R}_{+}\right)italic_M = [ italic_a start_POSTSUBSCRIPT italic_i italic_j end_POSTSUBSCRIPT ] start_POSTSUBSCRIPT 1 ≀ italic_i , italic_j ≀ 2 end_POSTSUBSCRIPT ∈ caligraphic_M start_POSTSUBSCRIPT 2 Γ— 2 end_POSTSUBSCRIPT ( blackboard_R start_POSTSUBSCRIPT + end_POSTSUBSCRIPT ) is convergent to zero if and only if

a11,a22<1subscriptπ‘Ž11subscriptπ‘Ž221a_{11},\ \ a_{22}<1italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT , italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT < 1

and

tr⁒(M)<1+det⁒(M),i.e.,⁒a11+a22<1+a11⁒a22βˆ’a12⁒a21.formulae-sequencetr𝑀1det𝑀i.e.,subscriptπ‘Ž11subscriptπ‘Ž221subscriptπ‘Ž11subscriptπ‘Ž22subscriptπ‘Ž12subscriptπ‘Ž21\text{tr}(M)<1+\text{det}(M),\,\ \text{i.e.,}\,\ a_{11}+a_{22}<1+a_{11}a_{22}-% a_{12}a_{21}.tr ( italic_M ) < 1 + det ( italic_M ) , i.e., italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT < 1 + italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT - italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT .

In the next Section 3, we use the matrix

M⁒(ΞΈ)=[a11a12⁒eθ⁒Tβˆ’1ΞΈa21a22⁒1βˆ’eβˆ’ΞΈβ’TΞΈ],π‘€πœƒmatrixsubscriptπ‘Ž11subscriptπ‘Ž12superscriptπ‘’πœƒπ‘‡1πœƒsubscriptπ‘Ž21subscriptπ‘Ž221superscriptπ‘’πœƒπ‘‡πœƒM(\theta)=\begin{bmatrix}a_{11}&a_{12}\frac{e^{\theta T}-1}{\theta}\\[3.0pt] a_{21}&a_{22}\frac{1-e^{-\theta T}}{\theta}\end{bmatrix},italic_M ( italic_ΞΈ ) = [ start_ARG start_ROW start_CELL italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT end_CELL start_CELL italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT divide start_ARG italic_e start_POSTSUPERSCRIPT italic_ΞΈ italic_T end_POSTSUPERSCRIPT - 1 end_ARG start_ARG italic_ΞΈ end_ARG end_CELL end_ROW start_ROW start_CELL italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT end_CELL start_CELL italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT divide start_ARG 1 - italic_e start_POSTSUPERSCRIPT - italic_ΞΈ italic_T end_POSTSUPERSCRIPT end_ARG start_ARG italic_ΞΈ end_ARG end_CELL end_ROW end_ARG ] ,

where ΞΈβ‰₯0,πœƒ0\theta\geq 0,italic_ΞΈ β‰₯ 0 , and we aim to find ΞΈπœƒ\thetaitalic_ΞΈ such that M⁒(ΞΈ)π‘€πœƒM(\theta)italic_M ( italic_ΞΈ ) is convergent to zero. Here, ai⁒j(i,j=1,2)a_{ij}\,(i,j=1,2)italic_a start_POSTSUBSCRIPT italic_i italic_j end_POSTSUBSCRIPT ( italic_i , italic_j = 1 , 2 ) are nonnegative numbers with a11<1subscriptπ‘Ž111\ a_{11}<1italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT < 1 and a22<1T.subscriptπ‘Ž221𝑇a_{22}<\frac{1}{T}.italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT < divide start_ARG 1 end_ARG start_ARG italic_T end_ARG . Notice that the last inequality guarantees

a22⁒1βˆ’eβˆ’ΞΈβ’TΞΈ<1subscriptπ‘Ž221superscriptπ‘’πœƒπ‘‡πœƒ1a_{22}\frac{1-e^{-\theta T}}{\theta}<1italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT divide start_ARG 1 - italic_e start_POSTSUPERSCRIPT - italic_ΞΈ italic_T end_POSTSUPERSCRIPT end_ARG start_ARG italic_ΞΈ end_ARG < 1

since 1βˆ’eβˆ’ΞΈβ’Tθ≀T1superscriptπ‘’πœƒπ‘‡πœƒπ‘‡\frac{1-e^{-\theta T}}{\theta}\leq Tdivide start_ARG 1 - italic_e start_POSTSUPERSCRIPT - italic_ΞΈ italic_T end_POSTSUPERSCRIPT end_ARG start_ARG italic_ΞΈ end_ARG ≀ italic_T for every ΞΈβ‰₯0.πœƒ0\theta\geq 0.italic_ΞΈ β‰₯ 0 .

The next lemma proved in [16] deals with the existence of a ΞΈβ‰₯0πœƒ0\theta\geq 0italic_ΞΈ β‰₯ 0 for which matrix M⁒(ΞΈ)π‘€πœƒM\left(\theta\right)italic_M ( italic_ΞΈ ) is convergent to zero. It shows us that there can be values of ΞΈ>0πœƒ0\theta>0italic_ΞΈ > 0 for which the matrix M⁒(ΞΈ)π‘€πœƒM\left(\theta\right)italic_M ( italic_ΞΈ ) is convergent to zero, although the matrix M⁒(0)𝑀0M(0)italic_M ( 0 ) corresponding to the Chebyshev norm is not convergent to zero.

From Lemma 2.2, the matrix M⁒(ΞΈ)π‘€πœƒM(\theta)italic_M ( italic_ΞΈ ) is convergent to zero if and only if h⁒(ΞΈ)<0β„Žπœƒ0h(\theta)<0italic_h ( italic_ΞΈ ) < 0, where

h⁒(ΞΈ)β„Žπœƒ\displaystyle h(\theta)italic_h ( italic_ΞΈ ) =tr⁒(M⁒(ΞΈ))βˆ’1βˆ’det⁒(M⁒(ΞΈ))absenttrπ‘€πœƒ1detπ‘€πœƒ\displaystyle=\text{tr}(M(\theta))-1-\text{det}(M(\theta))= tr ( italic_M ( italic_ΞΈ ) ) - 1 - det ( italic_M ( italic_ΞΈ ) )
=a11+a22⁒1βˆ’eβˆ’ΞΈβ’TΞΈβˆ’1βˆ’a11⁒a22⁒1βˆ’eβˆ’ΞΈβ’TΞΈ+a12⁒a21⁒eθ⁒Tβˆ’1ΞΈ(ΞΈβ‰₯0).absentsubscriptπ‘Ž11subscriptπ‘Ž221superscriptπ‘’πœƒπ‘‡πœƒ1subscriptπ‘Ž11subscriptπ‘Ž221superscriptπ‘’πœƒπ‘‡πœƒsubscriptπ‘Ž12subscriptπ‘Ž21superscriptπ‘’πœƒπ‘‡1πœƒπœƒ0\displaystyle=a_{11}+a_{22}\frac{1-e^{-\theta T}}{\theta}-1-a_{11}a_{22}\frac{% 1-e^{-\theta T}}{\theta}+a_{12}a_{21}\frac{e^{\theta T}-1}{\theta}\ \ \left(% \theta\geq 0\right).= italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT divide start_ARG 1 - italic_e start_POSTSUPERSCRIPT - italic_ΞΈ italic_T end_POSTSUPERSCRIPT end_ARG start_ARG italic_ΞΈ end_ARG - 1 - italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT divide start_ARG 1 - italic_e start_POSTSUPERSCRIPT - italic_ΞΈ italic_T end_POSTSUPERSCRIPT end_ARG start_ARG italic_ΞΈ end_ARG + italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT divide start_ARG italic_e start_POSTSUPERSCRIPT italic_ΞΈ italic_T end_POSTSUPERSCRIPT - 1 end_ARG start_ARG italic_ΞΈ end_ARG ( italic_ΞΈ β‰₯ 0 ) .
Lemma 2.3.

Assume 0≀a11<10subscriptπ‘Ž1110\leq a_{11}<10 ≀ italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT < 1 and 0<a22<1T0subscriptπ‘Ž221𝑇0<a_{22}<\frac{1}{T}0 < italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT < divide start_ARG 1 end_ARG start_ARG italic_T end_ARG.

  • (i)

    If h⁒(0)<0β„Ž00h(0)<0italic_h ( 0 ) < 0, then M⁒(0)𝑀0M(0)italic_M ( 0 ) converges to zero.

  • (ii)

    If h⁒(0)β‰₯0β„Ž00h(0)\geq 0italic_h ( 0 ) β‰₯ 0, then there exists ΞΈ1>0subscriptπœƒ10\theta_{1}>0italic_ΞΈ start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT > 0 with h′⁒(ΞΈ1)=0superscriptβ„Žβ€²subscriptπœƒ10h^{\prime}(\theta_{1})=0italic_h start_POSTSUPERSCRIPT β€² end_POSTSUPERSCRIPT ( italic_ΞΈ start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ) = 0 and

    • (a)

      if h⁒(ΞΈ1)<0β„Žsubscriptπœƒ10h(\theta_{1})<0italic_h ( italic_ΞΈ start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ) < 0, then the matrix M⁒(ΞΈ)π‘€πœƒM(\theta)italic_M ( italic_ΞΈ ) converges to zero for every ΞΈπœƒ\thetaitalic_ΞΈ between the zeroes of hβ„Žhitalic_h and does not converge to zero otherwise;

    • (b)

      if h⁒(ΞΈ1)β‰₯0β„Žsubscriptπœƒ10h(\theta_{1})\geq 0italic_h ( italic_ΞΈ start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ) β‰₯ 0, then there are no ΞΈπœƒ\thetaitalic_ΞΈ such that M⁒(ΞΈ)π‘€πœƒM(\theta)italic_M ( italic_ΞΈ ) converges to zero.

2.4. Fixed point theorems

Next, we recall two fixed point theorems, which, along with the well-known Schauder fixed point theorem, will play a key role in our analysis. The first result is Perov’s fixed point theorem (see, e.g., [13]) for mappings on the Cartesian product of two metric spaces.

Theorem 2.4 (Perov).

Let (Xi,di),subscript𝑋𝑖subscript𝑑𝑖\left(X_{i},d_{i}\right),( italic_X start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT , italic_d start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT ) , i=1,2𝑖12i=1,2italic_i = 1 , 2 be complete metric spaces and Ni:X1Γ—X2β†’Xi:subscript𝑁𝑖→subscript𝑋1subscript𝑋2subscript𝑋𝑖N_{i}:X_{1}\times X_{2}\rightarrow X_{i}italic_N start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT : italic_X start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_X start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT β†’ italic_X start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT be two mappings for which there exists a square matrix M𝑀Mitalic_M of size two with nonnegative entries and the spectral radius ρ⁒(M)<1πœŒπ‘€1\rho\left(M\right)<1italic_ρ ( italic_M ) < 1 such that the following vector inequality

(d1⁒(N1⁒(x,y),N1⁒(u,v))d2⁒(N2⁒(x,y),N2⁒(u,v)))≀M⁒(d1⁒(x,u)d2⁒(y,v))subscript𝑑1subscript𝑁1π‘₯𝑦subscript𝑁1𝑒𝑣subscript𝑑2subscript𝑁2π‘₯𝑦subscript𝑁2𝑒𝑣𝑀subscript𝑑1π‘₯𝑒subscript𝑑2𝑦𝑣\left(\begin{array}[]{c}d_{1}\left(N_{1}\left(x,y\right),N_{1}\left(u,v\right)% \right)\\ d_{2}\left(N_{2}\left(x,y\right),N_{2}\left(u,v\right)\right)\end{array}\right% )\leq M\left(\begin{array}[]{c}d_{1}\left(x,u\right)\\ d_{2}\left(y,v\right)\end{array}\right)( start_ARRAY start_ROW start_CELL italic_d start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) , italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_u , italic_v ) ) end_CELL end_ROW start_ROW start_CELL italic_d start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_u , italic_v ) ) end_CELL end_ROW end_ARRAY ) ≀ italic_M ( start_ARRAY start_ROW start_CELL italic_d start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_u ) end_CELL end_ROW start_ROW start_CELL italic_d start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_y , italic_v ) end_CELL end_ROW end_ARRAY )

holds for all (x,y),(u,v)∈X1Γ—X2.π‘₯𝑦𝑒𝑣subscript𝑋1subscript𝑋2\left(x,y\right),\left(u,v\right)\in X_{1}\times X_{2}.( italic_x , italic_y ) , ( italic_u , italic_v ) ∈ italic_X start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_X start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT . Then, there exists a unique point (x,y)∈X1Γ—X2π‘₯𝑦subscript𝑋1subscript𝑋2\left(x,y\right)\in X_{1}\times X_{2}( italic_x , italic_y ) ∈ italic_X start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_X start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT with

(x,y)=(N1⁒(x,y),N2⁒(x,y)).π‘₯𝑦subscript𝑁1π‘₯𝑦subscript𝑁2π‘₯𝑦(x,y)=\left(N_{1}\left(x,y\right),N_{2}\left(x,y\right)\right).( italic_x , italic_y ) = ( italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) ) .

The second result is Avramescu’s fixed point theorem [1].

Theorem 2.5 (Avramescu).

Let D1subscript𝐷1D_{1}italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT be a closed convex subset of a normed space Yπ‘ŒYitalic_Y, (D2,d)subscript𝐷2𝑑(D_{2},d)( italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT , italic_d ) a complete metric space, and let Ni:D1Γ—D2β†’Di:subscript𝑁𝑖→subscript𝐷1subscript𝐷2subscript𝐷𝑖N_{i}:D_{1}\times D_{2}\rightarrow D_{i}italic_N start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT : italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT β†’ italic_D start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT, i=1,2𝑖12i=1,2italic_i = 1 , 2 be continuous mappings. Assume that the following conditions are satisfied:

  1. (a)

    N1⁒(D1Γ—D2)subscript𝑁1subscript𝐷1subscript𝐷2N_{1}(D_{1}\times D_{2})italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ) is a relatively compact subset of Yπ‘ŒYitalic_Y;

  2. (b)

    There is a constant L∈[0,1)𝐿01L\in[0,1)italic_L ∈ [ 0 , 1 ) such that

    d⁒(N2⁒(x,y),N2⁒(x,yβ€²))≀L⁒d⁒(y,yβ€²)𝑑subscript𝑁2π‘₯𝑦subscript𝑁2π‘₯superscript𝑦′𝐿𝑑𝑦superscript𝑦′d(N_{2}(x,y),N_{2}(x,y^{\prime}))\leq L\,d(y,y^{\prime})italic_d ( italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y start_POSTSUPERSCRIPT β€² end_POSTSUPERSCRIPT ) ) ≀ italic_L italic_d ( italic_y , italic_y start_POSTSUPERSCRIPT β€² end_POSTSUPERSCRIPT )

    for all x∈D1π‘₯subscript𝐷1x\in D_{1}italic_x ∈ italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT and y,yβ€²βˆˆD2𝑦superscript𝑦′subscript𝐷2y,y^{\prime}\in D_{2}italic_y , italic_y start_POSTSUPERSCRIPT β€² end_POSTSUPERSCRIPT ∈ italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT.

Then, there exists (x,y)∈D1Γ—D2π‘₯𝑦subscript𝐷1subscript𝐷2(x,y)\in D_{1}\times D_{2}( italic_x , italic_y ) ∈ italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT such that

N1⁒(x,y)=x,N2⁒(x,y)=y.formulae-sequencesubscript𝑁1π‘₯𝑦π‘₯subscript𝑁2π‘₯𝑦𝑦N_{1}(x,y)=x,\quad N_{2}(x,y)=y.italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) = italic_x , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) = italic_y .

Some reference works in fixed point theory are the books [4], [5] and [6].

3. Mutual control for abstract evolution equations

In this section, we aim to find a mild solution of the control problem (1.1)-(1.2). More exactly, we look for x,y∈C⁒([0,T];X)π‘₯𝑦𝐢0𝑇𝑋x,y\in C\left(\left[0,T\right];X\right)italic_x , italic_y ∈ italic_C ( [ 0 , italic_T ] ; italic_X ) such that, for all t∈[0,T]𝑑0𝑇t\in[0,T]italic_t ∈ [ 0 , italic_T ], the following relations hold

(3.1) {x⁒(t)=S⁒(t)⁒x⁒(0)+∫0tS⁒(tβˆ’s)⁒F⁒(x⁒(s),y⁒(s))⁒𝑑sy⁒(t)=S⁒(t)⁒y⁒(0)+∫0tS⁒(tβˆ’s)⁒G⁒(x⁒(s),y⁒(s))⁒𝑑s,casesπ‘₯𝑑𝑆𝑑π‘₯0superscriptsubscript0𝑑𝑆𝑑𝑠𝐹π‘₯𝑠𝑦𝑠differential-d𝑠otherwise𝑦𝑑𝑆𝑑𝑦0superscriptsubscript0𝑑𝑆𝑑𝑠𝐺π‘₯𝑠𝑦𝑠differential-d𝑠otherwise\begin{cases}x\left(t\right)=S\left(t\right)x\left(0\right)+\int_{0}^{t}S\left% (t-s\right)F\left(x\left(s\right),y\left(s\right)\right)ds\\ y\left(t\right)=S\left(t\right)y\left(0\right)+\int_{0}^{t}S\left(t-s\right)G% \left(x\left(s\right),y\left(s\right)\right)ds,\end{cases}{ start_ROW start_CELL italic_x ( italic_t ) = italic_S ( italic_t ) italic_x ( 0 ) + ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_t end_POSTSUPERSCRIPT italic_S ( italic_t - italic_s ) italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s end_CELL start_CELL end_CELL end_ROW start_ROW start_CELL italic_y ( italic_t ) = italic_S ( italic_t ) italic_y ( 0 ) + ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_t end_POSTSUPERSCRIPT italic_S ( italic_t - italic_s ) italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s , end_CELL start_CELL end_CELL end_ROW
(3.2) x⁒(T)βˆ’a⁒x⁒(0)=k⁒(y⁒(T)βˆ’b⁒y⁒(0)).π‘₯π‘‡π‘Žπ‘₯0π‘˜π‘¦π‘‡π‘π‘¦0x\left(T\right)-ax\left(0\right)=k\left(y\left(T\right)-by\left(0\right)\right).italic_x ( italic_T ) - italic_a italic_x ( 0 ) = italic_k ( italic_y ( italic_T ) - italic_b italic_y ( 0 ) ) .

3.1. Fixed point formulation.

Our first aim is to combine the controllability condition (3.2) with (3.1) into a single system that takes the form of a fixed-point equation. Assume (x,y)π‘₯𝑦\left(x,y\right)( italic_x , italic_y ) is a solution of the mutual control problem. Then, we have

x⁒(T)βˆ’a⁒x⁒(0)=S⁒(T)⁒x⁒(0)βˆ’a⁒x⁒(0)+∫0TS⁒(Tβˆ’s)⁒F⁒(x⁒(s),y⁒(s))⁒𝑑s,π‘₯π‘‡π‘Žπ‘₯0𝑆𝑇π‘₯0π‘Žπ‘₯0superscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle x\left(T\right)-ax\left(0\right)=S\left(T\right)x\left(0\right)-% ax\left(0\right)+\int_{0}^{T}S\left(T-s\right)F\left(x\left(s\right),y\left(s% \right)\right)ds,italic_x ( italic_T ) - italic_a italic_x ( 0 ) = italic_S ( italic_T ) italic_x ( 0 ) - italic_a italic_x ( 0 ) + ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s ,
y⁒(T)βˆ’b⁒y⁒(0)=S⁒(T)⁒y⁒(0)βˆ’b⁒y⁒(0)+∫0TS⁒(Tβˆ’s)⁒G⁒(x⁒(s),y⁒(s))⁒𝑑s,𝑦𝑇𝑏𝑦0𝑆𝑇𝑦0𝑏𝑦0superscriptsubscript0𝑇𝑆𝑇𝑠𝐺π‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle y\left(T\right)-by\left(0\right)=S\left(T\right)y\left(0\right)-% by\left(0\right)+\int_{0}^{T}S\left(T-s\right)G\left(x\left(s\right),y\left(s% \right)\right)ds,italic_y ( italic_T ) - italic_b italic_y ( 0 ) = italic_S ( italic_T ) italic_y ( 0 ) - italic_b italic_y ( 0 ) + ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s ,

and using (3.2) yields

(3.3) 00\displaystyle 0 =S⁒(T)⁒x⁒(0)βˆ’k⁒S⁒(T)⁒y⁒(0)βˆ’a⁒x⁒(0)+k⁒b⁒y⁒(0)absent𝑆𝑇π‘₯0π‘˜π‘†π‘‡π‘¦0π‘Žπ‘₯0π‘˜π‘π‘¦0\displaystyle=S\left(T\right)x\left(0\right)-kS\left(T\right)y\left(0\right)-% ax\left(0\right)+kby\left(0\right)= italic_S ( italic_T ) italic_x ( 0 ) - italic_k italic_S ( italic_T ) italic_y ( 0 ) - italic_a italic_x ( 0 ) + italic_k italic_b italic_y ( 0 )
+∫0TS⁒(Tβˆ’s)⁒(F⁒(x⁒(s),y⁒(s))βˆ’k⁒G⁒(x⁒(s),y⁒(s)))⁒𝑑s.superscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯π‘ π‘¦π‘ π‘˜πΊπ‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+\int_{0}^{T}S\left(T-s\right)\left(F\left(x\left(s\right),y% \left(s\right)\right)-kG\left(x\left(s\right),y\left(s\right)\right)\right)ds.+ ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s .

When we express x⁒(0)π‘₯0x\left(0\right)italic_x ( 0 ) and y⁒(0)𝑦0y\left(0\right)italic_y ( 0 ) from (3.3)3.3\left(\ref{eq1}\right)( ) and replace them in (3.1), we obtain

(3.4) {x⁒(t)=N1⁒(x,y)⁒(t)y⁒(t)=N2⁒(x,y)⁒(t),casesπ‘₯𝑑subscript𝑁1π‘₯𝑦𝑑otherwise𝑦𝑑subscript𝑁2π‘₯𝑦𝑑otherwise\begin{cases}x\left(t\right)=N_{1}\left(x,y\right)\left(t\right)\\ y\left(t\right)=N_{2}\left(x,y\right)\left(t\right),\end{cases}{ start_ROW start_CELL italic_x ( italic_t ) = italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) ( italic_t ) end_CELL start_CELL end_CELL end_ROW start_ROW start_CELL italic_y ( italic_t ) = italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) ( italic_t ) , end_CELL start_CELL end_CELL end_ROW

where N1,N2:C⁒([0,T];X)2β†’C⁒([0,T];X)2:subscript𝑁1subscript𝑁2→𝐢superscript0𝑇𝑋2𝐢superscript0𝑇𝑋2N_{1},N_{2}\colon C\left(\left[0,T\right];X\right)^{2}\rightarrow C\left(\left% [0,T\right];X\right)^{2}italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT : italic_C ( [ 0 , italic_T ] ; italic_X ) start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT β†’ italic_C ( [ 0 , italic_T ] ; italic_X ) start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT are given by

N1⁒(x,y)⁒(t)subscript𝑁1π‘₯𝑦𝑑\displaystyle N_{1}(x,y)(t)italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) ( italic_t ) =1a⁒S⁒(t)⁒[S⁒(T)⁒x⁒(0)βˆ’k⁒S⁒(T)⁒y⁒(0)+k⁒b⁒y⁒(0)]absent1π‘Žπ‘†π‘‘delimited-[]𝑆𝑇π‘₯0π‘˜π‘†π‘‡π‘¦0π‘˜π‘π‘¦0\displaystyle=\frac{1}{a}S(t)\left[S(T)x(0)-kS(T)y(0)+kby(0)\right]= divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_S ( italic_t ) [ italic_S ( italic_T ) italic_x ( 0 ) - italic_k italic_S ( italic_T ) italic_y ( 0 ) + italic_k italic_b italic_y ( 0 ) ]
+1a⁒∫0TS⁒(Tβˆ’s)⁒(F⁒(x⁒(s),y⁒(s))βˆ’k⁒G⁒(x⁒(s),y⁒(s)))⁒𝑑s1π‘Žsuperscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯π‘ π‘¦π‘ π‘˜πΊπ‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+\frac{1}{a}\int_{0}^{T}S(T-s)\left(F(x(s),y(s))-kG(x(s),y(s% ))\right)ds+ divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s
+∫0tS⁒(tβˆ’s)⁒F⁒(x⁒(s),y⁒(s))⁒𝑑s,superscriptsubscript0𝑑𝑆𝑑𝑠𝐹π‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+\int_{0}^{t}S(t-s)F(x(s),y(s))ds,+ ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_t end_POSTSUPERSCRIPT italic_S ( italic_t - italic_s ) italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s ,
N2⁒(x,y)⁒(t)subscript𝑁2π‘₯𝑦𝑑\displaystyle N_{2}(x,y)(t)italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) ( italic_t ) =1k⁒b⁒S⁒(t)⁒[βˆ’S⁒(T)⁒x⁒(0)+k⁒S⁒(T)⁒y⁒(0)+a⁒x⁒(0)]absent1π‘˜π‘π‘†π‘‘delimited-[]𝑆𝑇π‘₯0π‘˜π‘†π‘‡π‘¦0π‘Žπ‘₯0\displaystyle=\frac{1}{kb}S(t)\left[-S(T)x(0)+kS(T)y(0)+ax(0)\right]= divide start_ARG 1 end_ARG start_ARG italic_k italic_b end_ARG italic_S ( italic_t ) [ - italic_S ( italic_T ) italic_x ( 0 ) + italic_k italic_S ( italic_T ) italic_y ( 0 ) + italic_a italic_x ( 0 ) ]
βˆ’1k⁒b⁒∫0TS⁒(Tβˆ’s)⁒(F⁒(x⁒(s),y⁒(s))βˆ’k⁒G⁒(x⁒(s),y⁒(s)))⁒𝑑s1π‘˜π‘superscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯π‘ π‘¦π‘ π‘˜πΊπ‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad-\frac{1}{kb}\int_{0}^{T}S(T-s)\left(F(x(s),y(s))-kG(x(s),y(% s))\right)ds- divide start_ARG 1 end_ARG start_ARG italic_k italic_b end_ARG ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s
+∫0tS⁒(tβˆ’s)⁒G⁒(x⁒(s),y⁒(s))⁒𝑑s.superscriptsubscript0𝑑𝑆𝑑𝑠𝐺π‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+\int_{0}^{t}S(t-s)G(x(s),y(s))ds.+ ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_t end_POSTSUPERSCRIPT italic_S ( italic_t - italic_s ) italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s .

Thus, the pair (x,y)π‘₯𝑦\left(x,y\right)( italic_x , italic_y ) is a fixed point of the operator (N1,N2)subscript𝑁1subscript𝑁2\left(N_{1},N_{2}\right)( italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ). In the following lemma, we show that the converse also holds, i.e., any fixed point of the operator (N1,N2)subscript𝑁1subscript𝑁2\left(N_{1},N_{2}\right)( italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ) satisfies both (3.1)3.1\left(\ref{el}\right)( ) and (3.2)3.2\left(\ref{3.1'}\right)( ).

Lemma 3.1.

Any fixed point of the operator (N1,N2)subscript𝑁1subscript𝑁2(N_{1},N_{2})( italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ) satisfy (3.1)3.1\left(\ref{el}\right)( ) and (3.2)3.2\left(\ref{3.1'}\right)( ).

Proof.

Assume that (x,y)π‘₯𝑦\left(x,y\right)( italic_x , italic_y ) is a solution of (3.4). Setting t=0𝑑0t=0italic_t = 0, we obtain

a⁒x⁒(0)π‘Žπ‘₯0\displaystyle ax\left(0\right)italic_a italic_x ( 0 ) =\displaystyle== S⁒(T)⁒x⁒(0)βˆ’k⁒S⁒(T)⁒y⁒(0)+k⁒b⁒y⁒(0)𝑆𝑇π‘₯0π‘˜π‘†π‘‡π‘¦0π‘˜π‘π‘¦0\displaystyle S\left(T\right)x\left(0\right)-kS\left(T\right)y\left(0\right)+% kby\left(0\right)italic_S ( italic_T ) italic_x ( 0 ) - italic_k italic_S ( italic_T ) italic_y ( 0 ) + italic_k italic_b italic_y ( 0 )
+∫0TS⁒(Tβˆ’s)⁒(F⁒(x⁒(s),y⁒(s))βˆ’k⁒G⁒(x⁒(s),y⁒(s)))⁒𝑑s,superscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯π‘ π‘¦π‘ π‘˜πΊπ‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle+\int_{0}^{T}S\left(T-s\right)\left(F\left(x\left(s\right),y\left% (s\right)\right)-kG\left(x\left(s\right),y\left(s\right)\right)\right)ds,+ ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s ,
k⁒b⁒y⁒(0)π‘˜π‘π‘¦0\displaystyle kby\left(0\right)italic_k italic_b italic_y ( 0 ) =\displaystyle== βˆ’S⁒(T)⁒x⁒(0)+k⁒S⁒(T)⁒y⁒(0)+a⁒x⁒(0)𝑆𝑇π‘₯0π‘˜π‘†π‘‡π‘¦0π‘Žπ‘₯0\displaystyle-S\left(T\right)x\left(0\right)+kS\left(T\right)y\left(0\right)+% ax\left(0\right)- italic_S ( italic_T ) italic_x ( 0 ) + italic_k italic_S ( italic_T ) italic_y ( 0 ) + italic_a italic_x ( 0 )
βˆ’βˆ«0TS⁒(Tβˆ’s)⁒(F⁒(x⁒(s),y⁒(s))βˆ’k⁒G⁒(x⁒(s),y⁒(s)))⁒𝑑s,superscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯π‘ π‘¦π‘ π‘˜πΊπ‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle-\int_{0}^{T}S\left(T-s\right)\left(F\left(x\left(s\right),y\left% (s\right)\right)-kG\left(x\left(s\right),y\left(s\right)\right)\right)ds,- ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s ,

whence

a⁒x⁒(0)βˆ’k⁒b⁒y⁒(0)π‘Žπ‘₯0π‘˜π‘π‘¦0\displaystyle ax\left(0\right)-kby\left(0\right)italic_a italic_x ( 0 ) - italic_k italic_b italic_y ( 0 ) =2⁒S⁒(T)⁒x⁒(0)βˆ’2⁒k⁒S⁒(T)⁒y⁒(0)βˆ’(a⁒x⁒(0)βˆ’k⁒b⁒y⁒(0))absent2𝑆𝑇π‘₯02π‘˜π‘†π‘‡π‘¦0π‘Žπ‘₯0π‘˜π‘π‘¦0\displaystyle=2S\left(T\right)x\left(0\right)-2kS\left(T\right)y\left(0\right)% -\left(ax\left(0\right)-kby\left(0\right)\right)= 2 italic_S ( italic_T ) italic_x ( 0 ) - 2 italic_k italic_S ( italic_T ) italic_y ( 0 ) - ( italic_a italic_x ( 0 ) - italic_k italic_b italic_y ( 0 ) )
+2⁒∫0TS⁒(Tβˆ’s)⁒(F⁒(x⁒(s),y⁒(s))βˆ’k⁒G⁒(x⁒(s),y⁒(s)))⁒𝑑s,2superscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯π‘ π‘¦π‘ π‘˜πΊπ‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+2\int_{0}^{T}S\left(T-s\right)\left(F\left(x\left(s\right),% y\left(s\right)\right)-kG\left(x\left(s\right),y\left(s\right)\right)\right)ds,+ 2 ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s ,

that is

(3.5) a⁒x⁒(0)βˆ’k⁒b⁒y⁒(0)π‘Žπ‘₯0π‘˜π‘π‘¦0\displaystyle ax\left(0\right)-kby\left(0\right)italic_a italic_x ( 0 ) - italic_k italic_b italic_y ( 0 ) =S⁒(T)⁒x⁒(0)βˆ’k⁒S⁒(T)⁒y⁒(0)absent𝑆𝑇π‘₯0π‘˜π‘†π‘‡π‘¦0\displaystyle=S\left(T\right)x\left(0\right)-kS\left(T\right)y\left(0\right)= italic_S ( italic_T ) italic_x ( 0 ) - italic_k italic_S ( italic_T ) italic_y ( 0 )
+∫0TS⁒(Tβˆ’s)⁒(F⁒(x⁒(s),y⁒(s))βˆ’k⁒G⁒(x⁒(s),y⁒(s)))⁒𝑑s.superscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯π‘ π‘¦π‘ π‘˜πΊπ‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+\int_{0}^{T}S\left(T-s\right)\left(F\left(x\left(s\right),y% \left(s\right)\right)-kG\left(x\left(s\right),y\left(s\right)\right)\right)ds.+ ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s .

Letting t=T𝑑𝑇t=Titalic_t = italic_T in (3.4) gives

x⁒(T)π‘₯𝑇\displaystyle x\left(T\right)italic_x ( italic_T ) =1a[S(T)(S(T)x(0)βˆ’kS(T)y(0)+kby(0)]\displaystyle=\frac{1}{a}\left[S\left(T\right)\left(S\left(T\right)x\left(0% \right)-kS\left(T\right)y\left(0\right)+kby\left(0\right)\right.\right]= divide start_ARG 1 end_ARG start_ARG italic_a end_ARG [ italic_S ( italic_T ) ( italic_S ( italic_T ) italic_x ( 0 ) - italic_k italic_S ( italic_T ) italic_y ( 0 ) + italic_k italic_b italic_y ( 0 ) ]
+1a⁒S⁒(T)⁒∫0TS⁒(Tβˆ’s)⁒(F⁒(x⁒(s),y⁒(s))βˆ’k⁒G⁒(x⁒(s),y⁒(s)))⁒𝑑s1π‘Žπ‘†π‘‡superscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯π‘ π‘¦π‘ π‘˜πΊπ‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+\frac{1}{a}S\left(T\right)\int_{0}^{T}S\left(T-s\right)% \left(F\left(x\left(s\right),y\left(s\right)\right)-kG\left(x\left(s\right),y% \left(s\right)\right)\right)ds+ divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_S ( italic_T ) ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s
+∫0TS⁒(Tβˆ’s)⁒F⁒(x⁒(s),y⁒(s))⁒𝑑s,superscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+\int_{0}^{T}S\left(T-s\right)F\left(x\left(s\right),y\left(% s\right)\right)ds,+ ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s ,

and

k⁒y⁒(T)π‘˜π‘¦π‘‡\displaystyle ky\left(T\right)italic_k italic_y ( italic_T ) =1b[S(T)(βˆ’S(T)x(0)+kS(T)y(0)+ax(0)]\displaystyle=\frac{1}{b}\left[S\left(T\right)\left(-S\left(T\right)x\left(0% \right)+kS\left(T\right)y\left(0\right)+ax\left(0\right)\right.\right]= divide start_ARG 1 end_ARG start_ARG italic_b end_ARG [ italic_S ( italic_T ) ( - italic_S ( italic_T ) italic_x ( 0 ) + italic_k italic_S ( italic_T ) italic_y ( 0 ) + italic_a italic_x ( 0 ) ]
βˆ’1b⁒S⁒(T)⁒∫0TS⁒(Tβˆ’s)⁒(F⁒(x⁒(s),y⁒(s))βˆ’k⁒G⁒(x⁒(s),y⁒(s)))⁒𝑑s1𝑏𝑆𝑇superscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯π‘ π‘¦π‘ π‘˜πΊπ‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad-\frac{1}{b}S\left(T\right)\int_{0}^{T}S\left(T-s\right)% \left(F\left(x\left(s\right),y\left(s\right)\right)-kG\left(x\left(s\right),y% \left(s\right)\right)\right)ds- divide start_ARG 1 end_ARG start_ARG italic_b end_ARG italic_S ( italic_T ) ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s
+k⁒∫0TS⁒(Tβˆ’s)⁒G⁒(x⁒(s),y⁒(s))⁒𝑑s.π‘˜superscriptsubscript0𝑇𝑆𝑇𝑠𝐺π‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+k\int_{0}^{T}S\left(T-s\right)G\left(x\left(s\right),y\left% (s\right)\right)ds.+ italic_k ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s .

Whence

x⁒(T)βˆ’k⁒y⁒(T)π‘₯π‘‡π‘˜π‘¦π‘‡\displaystyle x\left(T\right)-ky\left(T\right)italic_x ( italic_T ) - italic_k italic_y ( italic_T ) =1aS(T)[S(T)x(0)βˆ’kS(T)y(0)+kkby(0)\displaystyle=\frac{1}{a}S\left(T\right)\big{[}S\left(T\right)x\left(0\right)-% kS\left(T\right)y\left(0\right)+kkby\left(0\right)= divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_S ( italic_T ) [ italic_S ( italic_T ) italic_x ( 0 ) - italic_k italic_S ( italic_T ) italic_y ( 0 ) + italic_k italic_k italic_b italic_y ( 0 )
+∫0TS(Tβˆ’s)(F(x(s),y(s))βˆ’kG(x(s),y(s)))ds]\displaystyle\quad+\int_{0}^{T}S\left(T-s\right)\left(F\left(x\left(s\right),y% \left(s\right)\right)-kG\left(x\left(s\right),y\left(s\right)\right)\right)ds% \big{]}+ ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s ]
+∫0TS⁒(Tβˆ’s)⁒F⁒(x⁒(s),y⁒(s))⁒𝑑ssuperscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+\int_{0}^{T}S\left(T-s\right)F\left(x\left(s\right),y\left(% s\right)\right)ds+ ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s
+1bS(T)[S(T)x(0)βˆ’kS(T)y(0)βˆ’ax(0)\displaystyle\quad+\frac{1}{b}S\left(T\right)\big{[}S\left(T\right)x\left(0% \right)-kS\left(T\right)y\left(0\right)-ax\left(0\right)+ divide start_ARG 1 end_ARG start_ARG italic_b end_ARG italic_S ( italic_T ) [ italic_S ( italic_T ) italic_x ( 0 ) - italic_k italic_S ( italic_T ) italic_y ( 0 ) - italic_a italic_x ( 0 )
+∫0TS(Tβˆ’s)(F(x(s),y(s))βˆ’kG(x(s),y(s)))ds]\displaystyle\quad+\int_{0}^{T}S\left(T-s\right)\left(F\left(x\left(s\right),y% \left(s\right)\right)-kG\left(x\left(s\right),y\left(s\right)\right)\right)ds% \big{]}+ ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s ]
βˆ’k⁒∫0TS⁒(Tβˆ’s)⁒G⁒(x⁒(s),y⁒(s))⁒𝑑s.π‘˜superscriptsubscript0𝑇𝑆𝑇𝑠𝐺π‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad-k\int_{0}^{T}S\left(T-s\right)G\left(x\left(s\right),y\left% (s\right)\right)ds.- italic_k ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s .

Since, by (3.3), the expressions within the square brackets equal a⁒x⁒(0)π‘Žπ‘₯0ax\left(0\right)italic_a italic_x ( 0 ) and βˆ’k⁒b⁒y⁒(0)π‘˜π‘π‘¦0-kby\left(0\right)- italic_k italic_b italic_y ( 0 ), respectively, we deduce:

(3.6) x⁒(T)βˆ’k⁒y⁒(T)π‘₯π‘‡π‘˜π‘¦π‘‡\displaystyle x\left(T\right)-ky\left(T\right)italic_x ( italic_T ) - italic_k italic_y ( italic_T ) =S⁒(T)⁒x⁒(0)βˆ’k⁒S⁒(T)⁒y⁒(0)absent𝑆𝑇π‘₯0π‘˜π‘†π‘‡π‘¦0\displaystyle=S\left(T\right)x\left(0\right)-kS\left(T\right)y\left(0\right)= italic_S ( italic_T ) italic_x ( 0 ) - italic_k italic_S ( italic_T ) italic_y ( 0 )
+∫0TS⁒(Tβˆ’s)⁒(F⁒(x⁒(s),y⁒(s))βˆ’k⁒G⁒(x⁒(s),y⁒(s)))⁒𝑑s.superscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯π‘ π‘¦π‘ π‘˜πΊπ‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle+\int_{0}^{T}S\left(T-s\right)\left(F\left(x\left(s\right),y\left% (s\right)\right)-kG\left(x\left(s\right),y\left(s\right)\right)\right)ds.+ ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s .

Now (3.5) and (3.6) imply

a⁒x⁒(0)βˆ’k⁒b⁒y⁒(0)=x⁒(T)βˆ’k⁒y⁒(T),π‘Žπ‘₯0π‘˜π‘π‘¦0π‘₯π‘‡π‘˜π‘¦π‘‡ax\left(0\right)-kby\left(0\right)=x\left(T\right)-ky\left(T\right),italic_a italic_x ( 0 ) - italic_k italic_b italic_y ( 0 ) = italic_x ( italic_T ) - italic_k italic_y ( italic_T ) ,

and so the controllability condition is satisfied.

Finally, (3.5) and (3.4) imply that (x,y)π‘₯𝑦\left(x,y\right)( italic_x , italic_y ) satisfies (3.1). ∎

3.2. Existence

Using Perov’s and Leray-Schauder’s fixed point theorems, we obtain the following existence result.

Theorem 3.2.

Assume that the following conditions are satisfied:

  • (i)

    There are constants aF,bF,aG,bGβ‰₯0subscriptπ‘ŽπΉsubscript𝑏𝐹subscriptπ‘ŽπΊsubscript𝑏𝐺0a_{F},b_{F},a_{G},b_{G}\geq 0italic_a start_POSTSUBSCRIPT italic_F end_POSTSUBSCRIPT , italic_b start_POSTSUBSCRIPT italic_F end_POSTSUBSCRIPT , italic_a start_POSTSUBSCRIPT italic_G end_POSTSUBSCRIPT , italic_b start_POSTSUBSCRIPT italic_G end_POSTSUBSCRIPT β‰₯ 0 such that

    (3.7) |F⁒(x,y)βˆ’F⁒(xΒ―,yΒ―)|X≀aF⁒|xβˆ’xΒ―|X+bF⁒|yβˆ’yΒ―|X,subscript𝐹π‘₯𝑦𝐹¯π‘₯¯𝑦𝑋subscriptπ‘ŽπΉsubscriptπ‘₯Β―π‘₯𝑋subscript𝑏𝐹subscript𝑦¯𝑦𝑋\displaystyle|F(x,y)-F(\overline{x},\overline{y})|_{X}\leq a_{F}|x-\overline{x% }|_{X}+b_{F}|y-\overline{y}|_{X},| italic_F ( italic_x , italic_y ) - italic_F ( overΒ― start_ARG italic_x end_ARG , overΒ― start_ARG italic_y end_ARG ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ≀ italic_a start_POSTSUBSCRIPT italic_F end_POSTSUBSCRIPT | italic_x - overΒ― start_ARG italic_x end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_b start_POSTSUBSCRIPT italic_F end_POSTSUBSCRIPT | italic_y - overΒ― start_ARG italic_y end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ,
    |G⁒(x,y)βˆ’G⁒(xΒ―,yΒ―)|X≀aG⁒|xβˆ’xΒ―|X+bG⁒|yβˆ’yΒ―|X,subscript𝐺π‘₯𝑦𝐺¯π‘₯¯𝑦𝑋subscriptπ‘ŽπΊsubscriptπ‘₯Β―π‘₯𝑋subscript𝑏𝐺subscript𝑦¯𝑦𝑋\displaystyle|G(x,y)-G(\overline{x},\overline{y})|_{X}\leq a_{G}|x-\overline{x% }|_{X}+b_{G}|y-\overline{y}|_{X},| italic_G ( italic_x , italic_y ) - italic_G ( overΒ― start_ARG italic_x end_ARG , overΒ― start_ARG italic_y end_ARG ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ≀ italic_a start_POSTSUBSCRIPT italic_G end_POSTSUBSCRIPT | italic_x - overΒ― start_ARG italic_x end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_b start_POSTSUBSCRIPT italic_G end_POSTSUBSCRIPT | italic_y - overΒ― start_ARG italic_y end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ,

    for all x,xΒ―,y,y¯∈Xπ‘₯Β―π‘₯𝑦¯𝑦𝑋x,\overline{x},y,\overline{y}\in Xitalic_x , overΒ― start_ARG italic_x end_ARG , italic_y , overΒ― start_ARG italic_y end_ARG ∈ italic_X and t∈[0,T];𝑑0𝑇t\in\left[0,T\right];italic_t ∈ [ 0 , italic_T ] ;

  • (ii)

    The map H:=Fβˆ’k⁒Gassignπ»πΉπ‘˜πΊH:=F-kGitalic_H := italic_F - italic_k italic_G is bounded on X2;superscript𝑋2X^{2};italic_X start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT ;

  • (iii)

    The matrix

    (3.8) M:=T⁒CA⁒[1a⁒CA⁒(aF+k⁒aG)+aF1a⁒CA⁒(bF+k⁒bG)+bF1k⁒b⁒CA⁒(aF+k⁒aG)+aG1k⁒b⁒CA⁒(bF+k⁒bG)+bG]assign𝑀𝑇subscript𝐢𝐴delimited-[]1π‘Žsubscript𝐢𝐴subscriptπ‘ŽπΉπ‘˜subscriptπ‘ŽπΊsubscriptπ‘ŽπΉ1π‘Žsubscript𝐢𝐴subscriptπ‘πΉπ‘˜subscript𝑏𝐺subscript𝑏𝐹1π‘˜π‘subscript𝐢𝐴subscriptπ‘ŽπΉπ‘˜subscriptπ‘ŽπΊsubscriptπ‘ŽπΊ1π‘˜π‘subscript𝐢𝐴subscriptπ‘πΉπ‘˜subscript𝑏𝐺subscript𝑏𝐺M:=TC_{A}\left[\begin{array}[]{ll}\frac{1}{a}C_{A}\left(a_{F}+ka_{G}\right)+a_% {F}&\frac{1}{a}C_{A}\left(b_{F}+kb_{G}\right)+b_{F}\vskip 3.0pt plus 1.0pt % minus 1.0pt\\ \frac{1}{kb}C_{A}\left(a_{F}+ka_{G}\right)+a_{G}&\frac{1}{kb}C_{A}\left(b_{F}+% kb_{G}\right)+b_{G}\end{array}\right]italic_M := italic_T italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT [ start_ARRAY start_ROW start_CELL divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( italic_a start_POSTSUBSCRIPT italic_F end_POSTSUBSCRIPT + italic_k italic_a start_POSTSUBSCRIPT italic_G end_POSTSUBSCRIPT ) + italic_a start_POSTSUBSCRIPT italic_F end_POSTSUBSCRIPT end_CELL start_CELL divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( italic_b start_POSTSUBSCRIPT italic_F end_POSTSUBSCRIPT + italic_k italic_b start_POSTSUBSCRIPT italic_G end_POSTSUBSCRIPT ) + italic_b start_POSTSUBSCRIPT italic_F end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL divide start_ARG 1 end_ARG start_ARG italic_k italic_b end_ARG italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( italic_a start_POSTSUBSCRIPT italic_F end_POSTSUBSCRIPT + italic_k italic_a start_POSTSUBSCRIPT italic_G end_POSTSUBSCRIPT ) + italic_a start_POSTSUBSCRIPT italic_G end_POSTSUBSCRIPT end_CELL start_CELL divide start_ARG 1 end_ARG start_ARG italic_k italic_b end_ARG italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( italic_b start_POSTSUBSCRIPT italic_F end_POSTSUBSCRIPT + italic_k italic_b start_POSTSUBSCRIPT italic_G end_POSTSUBSCRIPT ) + italic_b start_POSTSUBSCRIPT italic_G end_POSTSUBSCRIPT end_CELL end_ROW end_ARRAY ]

    is convergent to zero;

  • (iv)

    Semigroup {S⁒(t);tβ‰₯0}𝑆𝑑𝑑0\left\{S\left(t\right);\ t\geq 0\right\}{ italic_S ( italic_t ) ; italic_t β‰₯ 0 } is compact and |S⁒(T)|ℒ⁒(X)<21a+1b.subscript𝑆𝑇ℒ𝑋21π‘Ž1𝑏\left|S\left(T\right)\right|_{\mathcal{L}\left(X\right)}<\frac{2}{\frac{1}{a}+% \frac{1}{b}}.| italic_S ( italic_T ) | start_POSTSUBSCRIPT caligraphic_L ( italic_X ) end_POSTSUBSCRIPT < divide start_ARG 2 end_ARG start_ARG divide start_ARG 1 end_ARG start_ARG italic_a end_ARG + divide start_ARG 1 end_ARG start_ARG italic_b end_ARG end_ARG .

Then problem (3.1)-(3.2) has at least one solution (x,y)π‘₯𝑦\left(x,y\right)( italic_x , italic_y ) in C⁒([0,T];X)2.𝐢superscript0𝑇𝑋2C\left(\left[0,T\right];X\right)^{2}.italic_C ( [ 0 , italic_T ] ; italic_X ) start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT .

Proof.

We prove the result in two steps: (a) First, using Perov’s fixed point theorem we prove that for any Ξ±,β∈X,𝛼𝛽𝑋\alpha,\beta\in X,italic_Ξ± , italic_Ξ² ∈ italic_X , there exists in C⁒([0,T];X)2𝐢superscript0𝑇𝑋2C\left(\left[0,T\right];X\right)^{2}italic_C ( [ 0 , italic_T ] ; italic_X ) start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT a unique fixed point (xΞ±,Ξ²,yΞ±,Ξ²)subscriptπ‘₯𝛼𝛽subscript𝑦𝛼𝛽\left(x_{\alpha,\beta},y_{\alpha,\beta}\right)( italic_x start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT , italic_y start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT ) of the operator (N1,N2)subscript𝑁1subscript𝑁2(N_{1},N_{2})( italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ) defined as follows:

(3.9) N1⁒(x,y)⁒(t)subscript𝑁1π‘₯𝑦𝑑\displaystyle N_{1}\left(x,y\right)\left(t\right)italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) ( italic_t ) =1a⁒S⁒(t)⁒[S⁒(T)β’Ξ±βˆ’k⁒S⁒(T)⁒β+k⁒b⁒β]absent1π‘Žπ‘†π‘‘delimited-[]π‘†π‘‡π›Όπ‘˜π‘†π‘‡π›½π‘˜π‘π›½\displaystyle=\frac{1}{a}S\left(t\right)\left[S\left(T\right)\alpha-kS\left(T% \right)\beta+kb\beta\right]= divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_S ( italic_t ) [ italic_S ( italic_T ) italic_Ξ± - italic_k italic_S ( italic_T ) italic_Ξ² + italic_k italic_b italic_Ξ² ]
+1a⁒S⁒(t)⁒∫0TS⁒(Tβˆ’s)⁒(F⁒(x⁒(s),y⁒(s))βˆ’k⁒G⁒(x⁒(s),y⁒(s)))⁒𝑑s1π‘Žπ‘†π‘‘superscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯π‘ π‘¦π‘ π‘˜πΊπ‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+\frac{1}{a}S(t)\int_{0}^{T}S\left(T-s\right)\left(F\left(x% \left(s\right),y\left(s\right)\right)-kG\left(x\left(s\right),y\left(s\right)% \right)\right)ds+ divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_S ( italic_t ) ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s
+∫0tS⁒(tβˆ’s)⁒F⁒(x⁒(s),y⁒(s))⁒𝑑s.superscriptsubscript0𝑑𝑆𝑑𝑠𝐹π‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+\int_{0}^{t}S\left(t-s\right)F\left(x\left(s\right),y\left(% s\right)\right)ds.+ ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_t end_POSTSUPERSCRIPT italic_S ( italic_t - italic_s ) italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s .
N2⁒(x,y)⁒(t)subscript𝑁2π‘₯𝑦𝑑\displaystyle N_{2}\left(x,y\right)\left(t\right)italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) ( italic_t ) =1k⁒b⁒S⁒(t)⁒[βˆ’S⁒(T)⁒α+k⁒S⁒(T)⁒β+a⁒α]absent1π‘˜π‘π‘†π‘‘delimited-[]π‘†π‘‡π›Όπ‘˜π‘†π‘‡π›½π‘Žπ›Ό\displaystyle=\frac{1}{kb}S\left(t\right)\left[-S\left(T\right)\alpha+kS\left(% T\right)\beta+a\alpha\right]= divide start_ARG 1 end_ARG start_ARG italic_k italic_b end_ARG italic_S ( italic_t ) [ - italic_S ( italic_T ) italic_Ξ± + italic_k italic_S ( italic_T ) italic_Ξ² + italic_a italic_Ξ± ]
βˆ’1k⁒b⁒S⁒(t)⁒∫0TS⁒(Tβˆ’s)⁒(F⁒(x⁒(s),y⁒(s))βˆ’k⁒G⁒(x⁒(s),y⁒(s)))⁒𝑑s1π‘˜π‘π‘†π‘‘superscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯π‘ π‘¦π‘ π‘˜πΊπ‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad-\frac{1}{kb}S\left(t\right)\int_{0}^{T}S\left(T-s\right)% \left(F\left(x\left(s\right),y\left(s\right)\right)-kG\left(x\left(s\right),y% \left(s\right)\right)\right)ds- divide start_ARG 1 end_ARG start_ARG italic_k italic_b end_ARG italic_S ( italic_t ) ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s
+∫0tS⁒(tβˆ’s)⁒G⁒(x⁒(s),y⁒(s))⁒𝑑s.superscriptsubscript0𝑑𝑆𝑑𝑠𝐺π‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+\int_{0}^{t}S\left(t-s\right)G\left(x\left(s\right),y\left(% s\right)\right)ds.+ ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_t end_POSTSUPERSCRIPT italic_S ( italic_t - italic_s ) italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s .

For any x,xΒ―,y,y¯∈C⁒([0,T];X),π‘₯Β―π‘₯𝑦¯𝑦𝐢0𝑇𝑋x,\overline{x},y,\overline{y}\in C\left(\left[0,T\right];X\right),italic_x , overΒ― start_ARG italic_x end_ARG , italic_y , overΒ― start_ARG italic_y end_ARG ∈ italic_C ( [ 0 , italic_T ] ; italic_X ) , one has

|N1⁒(x,y)βˆ’N1⁒(xΒ―,yΒ―)|0subscriptsubscript𝑁1π‘₯𝑦subscript𝑁1Β―π‘₯¯𝑦0\displaystyle\left|N_{1}\left(x,y\right)-N_{1}\left(\overline{x},\overline{y}% \right)\right|_{0}| italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) - italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( overΒ― start_ARG italic_x end_ARG , overΒ― start_ARG italic_y end_ARG ) | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT ≀T⁒CA⁒(1a⁒CA⁒(aF+k⁒aG)+aF)⁒|xβˆ’xΒ―|0absent𝑇subscript𝐢𝐴1π‘Žsubscript𝐢𝐴subscriptπ‘ŽπΉπ‘˜subscriptπ‘ŽπΊsubscriptπ‘ŽπΉsubscriptπ‘₯Β―π‘₯0\displaystyle\leq TC_{A}\left(\frac{1}{a}C_{A}\left(a_{F}+ka_{G}\right)+a_{F}% \right)\left|x-\overline{x}\right|_{0}≀ italic_T italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( italic_a start_POSTSUBSCRIPT italic_F end_POSTSUBSCRIPT + italic_k italic_a start_POSTSUBSCRIPT italic_G end_POSTSUBSCRIPT ) + italic_a start_POSTSUBSCRIPT italic_F end_POSTSUBSCRIPT ) | italic_x - overΒ― start_ARG italic_x end_ARG | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT
+T⁒CA⁒(1a⁒CA⁒(bF+k⁒bG)+bF)⁒|yβˆ’yΒ―|0,𝑇subscript𝐢𝐴1π‘Žsubscript𝐢𝐴subscriptπ‘πΉπ‘˜subscript𝑏𝐺subscript𝑏𝐹subscript𝑦¯𝑦0\displaystyle\quad+TC_{A}\left(\frac{1}{a}C_{A}\left(b_{F}+kb_{G}\right)+b_{F}% \right)\left|y-\overline{y}\right|_{0},+ italic_T italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( italic_b start_POSTSUBSCRIPT italic_F end_POSTSUBSCRIPT + italic_k italic_b start_POSTSUBSCRIPT italic_G end_POSTSUBSCRIPT ) + italic_b start_POSTSUBSCRIPT italic_F end_POSTSUBSCRIPT ) | italic_y - overΒ― start_ARG italic_y end_ARG | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT ,

and

|N2⁒(x,y)βˆ’N2⁒(xΒ―,yΒ―)|0subscriptsubscript𝑁2π‘₯𝑦subscript𝑁2Β―π‘₯¯𝑦0\displaystyle\left|N_{2}\left(x,y\right)-N_{2}\left(\overline{x},\overline{y}% \right)\right|_{0}| italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) - italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( overΒ― start_ARG italic_x end_ARG , overΒ― start_ARG italic_y end_ARG ) | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT ≀T⁒CA⁒(1k⁒b⁒CA⁒(aF+k⁒aG)+aG)⁒|xβˆ’xΒ―|0absent𝑇subscript𝐢𝐴1π‘˜π‘subscript𝐢𝐴subscriptπ‘ŽπΉπ‘˜subscriptπ‘ŽπΊsubscriptπ‘ŽπΊsubscriptπ‘₯Β―π‘₯0\displaystyle\leq TC_{A}\left(\frac{1}{kb}C_{A}\left(a_{F}+ka_{G}\right)+a_{G}% \right)\left|x-\overline{x}\right|_{0}≀ italic_T italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( divide start_ARG 1 end_ARG start_ARG italic_k italic_b end_ARG italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( italic_a start_POSTSUBSCRIPT italic_F end_POSTSUBSCRIPT + italic_k italic_a start_POSTSUBSCRIPT italic_G end_POSTSUBSCRIPT ) + italic_a start_POSTSUBSCRIPT italic_G end_POSTSUBSCRIPT ) | italic_x - overΒ― start_ARG italic_x end_ARG | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT
+T⁒CA⁒(1k⁒b⁒CA⁒(bF+k⁒bG)+bG)⁒|yβˆ’yΒ―|0.𝑇subscript𝐢𝐴1π‘˜π‘subscript𝐢𝐴subscriptπ‘πΉπ‘˜subscript𝑏𝐺subscript𝑏𝐺subscript𝑦¯𝑦0\displaystyle\quad+TC_{A}\left(\frac{1}{kb}C_{A}\left(b_{F}+kb_{G}\right)+b_{G% }\right)\left|y-\overline{y}\right|_{0}.+ italic_T italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( divide start_ARG 1 end_ARG start_ARG italic_k italic_b end_ARG italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( italic_b start_POSTSUBSCRIPT italic_F end_POSTSUBSCRIPT + italic_k italic_b start_POSTSUBSCRIPT italic_G end_POSTSUBSCRIPT ) + italic_b start_POSTSUBSCRIPT italic_G end_POSTSUBSCRIPT ) | italic_y - overΒ― start_ARG italic_y end_ARG | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT .

Writing the above relations in the vector form, we obtain

[|N1⁒(x,y)βˆ’N1⁒(xΒ―,yΒ―)|0|N2⁒(x,y)βˆ’N2⁒(xΒ―,yΒ―)|0]≀M⁒[|xβˆ’xΒ―|0|yβˆ’yΒ―|0].delimited-[]subscriptsubscript𝑁1π‘₯𝑦subscript𝑁1Β―π‘₯¯𝑦0subscriptsubscript𝑁2π‘₯𝑦subscript𝑁2Β―π‘₯¯𝑦0𝑀delimited-[]subscriptπ‘₯Β―π‘₯0subscript𝑦¯𝑦0\left[\begin{array}[]{c}\left|N_{1}\left(x,y\right)-N_{1}\left(\overline{x},% \overline{y}\right)\right|_{0}\\[5.0pt] \left|N_{2}\left(x,y\right)-N_{2}\left(\overline{x},\overline{y}\right)\right|% _{0}\end{array}\right]\leq M\left[\begin{array}[]{c}\left|x-\overline{x}\right% |_{0}\\[5.0pt] \left|y-\overline{y}\right|_{0}\end{array}\right].[ start_ARRAY start_ROW start_CELL | italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) - italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( overΒ― start_ARG italic_x end_ARG , overΒ― start_ARG italic_y end_ARG ) | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL | italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) - italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( overΒ― start_ARG italic_x end_ARG , overΒ― start_ARG italic_y end_ARG ) | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT end_CELL end_ROW end_ARRAY ] ≀ italic_M [ start_ARRAY start_ROW start_CELL | italic_x - overΒ― start_ARG italic_x end_ARG | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL | italic_y - overΒ― start_ARG italic_y end_ARG | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT end_CELL end_ROW end_ARRAY ] .

Consequently, N=(N1,N2)𝑁subscript𝑁1subscript𝑁2N=(N_{1},N_{2})italic_N = ( italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ) is a Perov contraction on C⁒([0,T];X)2𝐢superscript0𝑇𝑋2C\left(\left[0,T\right];X\right)^{2}italic_C ( [ 0 , italic_T ] ; italic_X ) start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT and thus it has a unique fixed point.

(b) Using Leray-Schauder’s fixed point theorem we prove that the map H:X2β†’X2,:𝐻→superscript𝑋2superscript𝑋2H:X^{2}\rightarrow X^{2},italic_H : italic_X start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT β†’ italic_X start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT ,

(Ξ±,Ξ²)↦(xΞ±,β⁒(0),yΞ±,β⁒(0)),maps-to𝛼𝛽subscriptπ‘₯𝛼𝛽0subscript𝑦𝛼𝛽0\left(\alpha,\beta\right)\mapsto\left(x_{\alpha,\beta}\left(0\right),y_{\alpha% ,\beta}\left(0\right)\right),( italic_Ξ± , italic_Ξ² ) ↦ ( italic_x start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT ( 0 ) , italic_y start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT ( 0 ) ) ,

has at least one fixed point (Ξ±βˆ—,Ξ²βˆ—).superscriptπ›Όβˆ—superscriptπ›½βˆ—\left(\alpha^{\ast},\beta^{\ast}\right).( italic_Ξ± start_POSTSUPERSCRIPT βˆ— end_POSTSUPERSCRIPT , italic_Ξ² start_POSTSUPERSCRIPT βˆ— end_POSTSUPERSCRIPT ) . Then the pair (xΞ±βˆ—,Ξ²βˆ—,yΞ±βˆ—,Ξ²βˆ—)subscriptπ‘₯superscriptπ›Όβˆ—superscriptπ›½βˆ—subscript𝑦superscriptπ›Όβˆ—superscriptπ›½βˆ—\left(x_{\alpha^{\ast},\beta^{\ast}},y_{\alpha^{\ast},\beta^{\ast}}\right)( italic_x start_POSTSUBSCRIPT italic_Ξ± start_POSTSUPERSCRIPT βˆ— end_POSTSUPERSCRIPT , italic_Ξ² start_POSTSUPERSCRIPT βˆ— end_POSTSUPERSCRIPT end_POSTSUBSCRIPT , italic_y start_POSTSUBSCRIPT italic_Ξ± start_POSTSUPERSCRIPT βˆ— end_POSTSUPERSCRIPT , italic_Ξ² start_POSTSUPERSCRIPT βˆ— end_POSTSUPERSCRIPT end_POSTSUBSCRIPT ) is a solution of the mutual control problem. To start, we show that H𝐻Hitalic_H is continuous. Indeed, denoting

Ξ³1⁒(Ξ±,Ξ²)subscript𝛾1𝛼𝛽\displaystyle\gamma_{1}(\alpha,\beta)italic_Ξ³ start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_Ξ± , italic_Ξ² ) =1a⁒S⁒(t)⁒(S⁒(T)β’Ξ±βˆ’k⁒S⁒(T)⁒β+k⁒b⁒β),absent1π‘Žπ‘†π‘‘π‘†π‘‡π›Όπ‘˜π‘†π‘‡π›½π‘˜π‘π›½\displaystyle=\frac{1}{a}S(t)\left(S(T)\alpha-kS(T)\beta+kb\beta\right),= divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_S ( italic_t ) ( italic_S ( italic_T ) italic_Ξ± - italic_k italic_S ( italic_T ) italic_Ξ² + italic_k italic_b italic_Ξ² ) ,
Ξ³2⁒(Ξ±,Ξ²)subscript𝛾2𝛼𝛽\displaystyle\gamma_{2}(\alpha,\beta)italic_Ξ³ start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_Ξ± , italic_Ξ² ) =1k⁒b⁒S⁒(t)⁒(βˆ’S⁒(T)⁒α+k⁒S⁒(T)⁒β+a⁒α),absent1π‘˜π‘π‘†π‘‘π‘†π‘‡π›Όπ‘˜π‘†π‘‡π›½π‘Žπ›Ό\displaystyle=\frac{1}{kb}S(t)\left(-S(T)\alpha+kS(T)\beta+a\alpha\right),= divide start_ARG 1 end_ARG start_ARG italic_k italic_b end_ARG italic_S ( italic_t ) ( - italic_S ( italic_T ) italic_Ξ± + italic_k italic_S ( italic_T ) italic_Ξ² + italic_a italic_Ξ± ) ,

one has

|Ξ³1⁒(Ξ±,Ξ²)βˆ’Ξ³1⁒(Ξ±Β―,Ξ²Β―)|Xsubscriptsubscript𝛾1𝛼𝛽subscript𝛾1¯𝛼¯𝛽𝑋\displaystyle\left|\gamma_{1}(\alpha,\beta)-\gamma_{1}(\overline{\alpha},% \overline{\beta})\right|_{X}| italic_Ξ³ start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_Ξ± , italic_Ξ² ) - italic_Ξ³ start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( overΒ― start_ARG italic_Ξ± end_ARG , overΒ― start_ARG italic_Ξ² end_ARG ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ≀C⁒(|Ξ±βˆ’Ξ±Β―|X+|Ξ²βˆ’Ξ²Β―|X),absent𝐢subscript𝛼¯𝛼𝑋subscript𝛽¯𝛽𝑋\displaystyle\leq C\left(\left|\alpha-\overline{\alpha}\right|_{X}+\left|\beta% -\overline{\beta}\right|_{X}\right),≀ italic_C ( | italic_Ξ± - overΒ― start_ARG italic_Ξ± end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + | italic_Ξ² - overΒ― start_ARG italic_Ξ² end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ) ,
|Ξ³2⁒(Ξ±,Ξ²)βˆ’Ξ³2⁒(Ξ±Β―,Ξ²Β―)|Xsubscriptsubscript𝛾2𝛼𝛽subscript𝛾2¯𝛼¯𝛽𝑋\displaystyle\left|\gamma_{2}(\alpha,\beta)-\gamma_{2}(\overline{\alpha},% \overline{\beta})\right|_{X}| italic_Ξ³ start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_Ξ± , italic_Ξ² ) - italic_Ξ³ start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( overΒ― start_ARG italic_Ξ± end_ARG , overΒ― start_ARG italic_Ξ² end_ARG ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ≀C⁒(|Ξ±βˆ’Ξ±Β―|X+|Ξ²βˆ’Ξ²Β―|X).absent𝐢subscript𝛼¯𝛼𝑋subscript𝛽¯𝛽𝑋\displaystyle\leq C\left(\left|\alpha-\overline{\alpha}\right|_{X}+\left|\beta% -\overline{\beta}\right|_{X}\right).≀ italic_C ( | italic_Ξ± - overΒ― start_ARG italic_Ξ± end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + | italic_Ξ² - overΒ― start_ARG italic_Ξ² end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ) .

for a suitable constant C>0.𝐢0C>0.italic_C > 0 . Then

|xΞ±,Ξ²βˆ’xΞ±Β―,Ξ²Β―|0subscriptsubscriptπ‘₯𝛼𝛽subscriptπ‘₯¯𝛼¯𝛽0\displaystyle\left|x_{\alpha,\beta}-x_{\overline{\alpha},\overline{\beta}}% \right|_{0}| italic_x start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT - italic_x start_POSTSUBSCRIPT overΒ― start_ARG italic_Ξ± end_ARG , overΒ― start_ARG italic_Ξ² end_ARG end_POSTSUBSCRIPT | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT ≀C⁒(|Ξ±βˆ’Ξ±Β―|X+|Ξ²βˆ’Ξ²Β―|X)absent𝐢subscript𝛼¯𝛼𝑋subscript𝛽¯𝛽𝑋\displaystyle\leq C\left(\left|\alpha-\overline{\alpha}\right|_{X}+\left|\beta% -\overline{\beta}\right|_{X}\right)≀ italic_C ( | italic_Ξ± - overΒ― start_ARG italic_Ξ± end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + | italic_Ξ² - overΒ― start_ARG italic_Ξ² end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT )
+m11⁒|xΞ±,Ξ²βˆ’xΞ±Β―,Ξ²Β―|0+m12⁒|yΞ±,Ξ²βˆ’yΞ±Β―,Ξ²Β―|0,subscriptπ‘š11subscriptsubscriptπ‘₯𝛼𝛽subscriptπ‘₯¯𝛼¯𝛽0subscriptπ‘š12subscriptsubscript𝑦𝛼𝛽subscript𝑦¯𝛼¯𝛽0\displaystyle\quad+m_{11}\left|x_{\alpha,\beta}-x_{\overline{\alpha},\overline% {\beta}}\right|_{0}+m_{12}\left|y_{\alpha,\beta}-y_{\overline{\alpha},% \overline{\beta}}\right|_{0},+ italic_m start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT | italic_x start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT - italic_x start_POSTSUBSCRIPT overΒ― start_ARG italic_Ξ± end_ARG , overΒ― start_ARG italic_Ξ² end_ARG end_POSTSUBSCRIPT | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT + italic_m start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT | italic_y start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT - italic_y start_POSTSUBSCRIPT overΒ― start_ARG italic_Ξ± end_ARG , overΒ― start_ARG italic_Ξ² end_ARG end_POSTSUBSCRIPT | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT ,
|yΞ±,Ξ²βˆ’yΞ±Β―,Ξ²Β―|0subscriptsubscript𝑦𝛼𝛽subscript𝑦¯𝛼¯𝛽0\displaystyle\left|y_{\alpha,\beta}-y_{\overline{\alpha},\overline{\beta}}% \right|_{0}| italic_y start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT - italic_y start_POSTSUBSCRIPT overΒ― start_ARG italic_Ξ± end_ARG , overΒ― start_ARG italic_Ξ² end_ARG end_POSTSUBSCRIPT | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT ≀C⁒(|Ξ±βˆ’Ξ±Β―|X+|Ξ²βˆ’Ξ²Β―|X)absent𝐢subscript𝛼¯𝛼𝑋subscript𝛽¯𝛽𝑋\displaystyle\leq C\left(\left|\alpha-\overline{\alpha}\right|_{X}+\left|\beta% -\overline{\beta}\right|_{X}\right)≀ italic_C ( | italic_Ξ± - overΒ― start_ARG italic_Ξ± end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + | italic_Ξ² - overΒ― start_ARG italic_Ξ² end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT )
+m21⁒|xΞ±,Ξ²βˆ’xΞ±Β―,Ξ²Β―|0+m22⁒|yΞ±,Ξ²βˆ’yΞ±Β―,Ξ²Β―|0.subscriptπ‘š21subscriptsubscriptπ‘₯𝛼𝛽subscriptπ‘₯¯𝛼¯𝛽0subscriptπ‘š22subscriptsubscript𝑦𝛼𝛽subscript𝑦¯𝛼¯𝛽0\displaystyle\quad+m_{21}\left|x_{\alpha,\beta}-x_{\overline{\alpha},\overline% {\beta}}\right|_{0}+m_{22}\left|y_{\alpha,\beta}-y_{\overline{\alpha},% \overline{\beta}}\right|_{0}.+ italic_m start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT | italic_x start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT - italic_x start_POSTSUBSCRIPT overΒ― start_ARG italic_Ξ± end_ARG , overΒ― start_ARG italic_Ξ² end_ARG end_POSTSUBSCRIPT | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT + italic_m start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT | italic_y start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT - italic_y start_POSTSUBSCRIPT overΒ― start_ARG italic_Ξ± end_ARG , overΒ― start_ARG italic_Ξ² end_ARG end_POSTSUBSCRIPT | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT .

where mi⁒jsubscriptπ‘šπ‘–π‘—m_{ij}italic_m start_POSTSUBSCRIPT italic_i italic_j end_POSTSUBSCRIPT are the entries of matrix M.𝑀M.italic_M . Hence

[|xΞ±,Ξ²βˆ’xΞ±Β―,Ξ²Β―|0|yΞ±,Ξ²βˆ’yΞ±Β―,Ξ²Β―|0]≀M⁒[|xΞ±,Ξ²βˆ’xΞ±Β―,Ξ²Β―|0|yΞ±,Ξ²βˆ’yΞ±Β―,Ξ²Β―|0]+[C⁒(|Ξ±βˆ’Ξ±Β―|X+|Ξ²βˆ’Ξ²Β―|X)C⁒(|Ξ±βˆ’Ξ±Β―|X+|Ξ²βˆ’Ξ²Β―|X)],matrixsubscriptsubscriptπ‘₯𝛼𝛽subscriptπ‘₯¯𝛼¯𝛽0subscriptsubscript𝑦𝛼𝛽subscript𝑦¯𝛼¯𝛽0𝑀matrixsubscriptsubscriptπ‘₯𝛼𝛽subscriptπ‘₯¯𝛼¯𝛽0subscriptsubscript𝑦𝛼𝛽subscript𝑦¯𝛼¯𝛽0matrix𝐢subscript𝛼¯𝛼𝑋subscript𝛽¯𝛽𝑋𝐢subscript𝛼¯𝛼𝑋subscript𝛽¯𝛽𝑋\begin{bmatrix}\left|x_{\alpha,\beta}-x_{\overline{\alpha},\overline{\beta}}% \right|_{0}\\[7.0pt] \left|y_{\alpha,\beta}-y_{\overline{\alpha},\overline{\beta}}\right|_{0}\end{% bmatrix}\leq M\begin{bmatrix}\left|x_{\alpha,\beta}-x_{\overline{\alpha},% \overline{\beta}}\right|_{0}\\[7.0pt] \left|y_{\alpha,\beta}-y_{\overline{\alpha},\overline{\beta}}\right|_{0}\end{% bmatrix}+\begin{bmatrix}C\left(\left|\alpha-\overline{\alpha}\right|_{X}+\left% |\beta-\overline{\beta}\right|_{X}\right)\\[7.0pt] C\left(\left|\alpha-\overline{\alpha}\right|_{X}+\left|\beta-\overline{\beta}% \right|_{X}\right)\end{bmatrix},[ start_ARG start_ROW start_CELL | italic_x start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT - italic_x start_POSTSUBSCRIPT overΒ― start_ARG italic_Ξ± end_ARG , overΒ― start_ARG italic_Ξ² end_ARG end_POSTSUBSCRIPT | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL | italic_y start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT - italic_y start_POSTSUBSCRIPT overΒ― start_ARG italic_Ξ± end_ARG , overΒ― start_ARG italic_Ξ² end_ARG end_POSTSUBSCRIPT | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT end_CELL end_ROW end_ARG ] ≀ italic_M [ start_ARG start_ROW start_CELL | italic_x start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT - italic_x start_POSTSUBSCRIPT overΒ― start_ARG italic_Ξ± end_ARG , overΒ― start_ARG italic_Ξ² end_ARG end_POSTSUBSCRIPT | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL | italic_y start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT - italic_y start_POSTSUBSCRIPT overΒ― start_ARG italic_Ξ± end_ARG , overΒ― start_ARG italic_Ξ² end_ARG end_POSTSUBSCRIPT | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT end_CELL end_ROW end_ARG ] + [ start_ARG start_ROW start_CELL italic_C ( | italic_Ξ± - overΒ― start_ARG italic_Ξ± end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + | italic_Ξ² - overΒ― start_ARG italic_Ξ² end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ) end_CELL end_ROW start_ROW start_CELL italic_C ( | italic_Ξ± - overΒ― start_ARG italic_Ξ± end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + | italic_Ξ² - overΒ― start_ARG italic_Ξ² end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ) end_CELL end_ROW end_ARG ] ,

equivalently

[|xΞ±,Ξ²βˆ’xΞ±Β―,Ξ²Β―|0|yΞ±,Ξ²βˆ’yΞ±Β―,Ξ²Β―|0]≀(Iβˆ’M)βˆ’1⁒[C⁒(|Ξ±βˆ’Ξ±Β―|X+|Ξ²βˆ’Ξ²Β―|X)C⁒(|Ξ±βˆ’Ξ±Β―|X+|Ξ²βˆ’Ξ²Β―|X)],matrixsubscriptsubscriptπ‘₯𝛼𝛽subscriptπ‘₯¯𝛼¯𝛽0subscriptsubscript𝑦𝛼𝛽subscript𝑦¯𝛼¯𝛽0superscript𝐼𝑀1matrix𝐢subscript𝛼¯𝛼𝑋subscript𝛽¯𝛽𝑋𝐢subscript𝛼¯𝛼𝑋subscript𝛽¯𝛽𝑋\begin{bmatrix}\left|x_{\alpha,\beta}-x_{\overline{\alpha},\overline{\beta}}% \right|_{0}\\[7.0pt] \left|y_{\alpha,\beta}-y_{\overline{\alpha},\overline{\beta}}\right|_{0}\end{% bmatrix}\leq\left(I-M\right)^{-1}\begin{bmatrix}C\left(\left|\alpha-\overline{% \alpha}\right|_{X}+\left|\beta-\overline{\beta}\right|_{X}\right)\\[7.0pt] C\left(\left|\alpha-\overline{\alpha}\right|_{X}+\left|\beta-\overline{\beta}% \right|_{X}\right)\end{bmatrix},[ start_ARG start_ROW start_CELL | italic_x start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT - italic_x start_POSTSUBSCRIPT overΒ― start_ARG italic_Ξ± end_ARG , overΒ― start_ARG italic_Ξ² end_ARG end_POSTSUBSCRIPT | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL | italic_y start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT - italic_y start_POSTSUBSCRIPT overΒ― start_ARG italic_Ξ± end_ARG , overΒ― start_ARG italic_Ξ² end_ARG end_POSTSUBSCRIPT | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT end_CELL end_ROW end_ARG ] ≀ ( italic_I - italic_M ) start_POSTSUPERSCRIPT - 1 end_POSTSUPERSCRIPT [ start_ARG start_ROW start_CELL italic_C ( | italic_Ξ± - overΒ― start_ARG italic_Ξ± end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + | italic_Ξ² - overΒ― start_ARG italic_Ξ² end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ) end_CELL end_ROW start_ROW start_CELL italic_C ( | italic_Ξ± - overΒ― start_ARG italic_Ξ± end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + | italic_Ξ² - overΒ― start_ARG italic_Ξ² end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ) end_CELL end_ROW end_ARG ] ,

which clearly shows that xΞ±,Ξ²subscriptπ‘₯𝛼𝛽x_{\alpha,\beta}italic_x start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT and yΞ±,Ξ²subscript𝑦𝛼𝛽y_{\alpha,\beta}italic_y start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT depend continuously on α𝛼\alphaitalic_Ξ± and Ξ².𝛽\beta.italic_Ξ² . This implies the continuity of H.𝐻H.italic_H . Next we show that H𝐻Hitalic_H maps bounded sets into bounded sets. This follows from the estimate

[|xΞ±,Ξ²βˆ’x0,0|0|yΞ±,Ξ²βˆ’y0,0|0]≀(Iβˆ’M)βˆ’1⁒[C⁒(|Ξ±|X+|Ξ²|X)C⁒(|Ξ±|X+|Ξ²|X)].delimited-[]subscriptsubscriptπ‘₯𝛼𝛽subscriptπ‘₯000subscriptsubscript𝑦𝛼𝛽subscript𝑦000superscript𝐼𝑀1delimited-[]𝐢subscript𝛼𝑋subscript𝛽𝑋𝐢subscript𝛼𝑋subscript𝛽𝑋\left[\begin{array}[]{c}\left|x_{\alpha,\beta}-x_{0,0}\right|_{0}\vskip 3.0pt % plus 1.0pt minus 1.0pt\\ \left|y_{\alpha,\beta}-y_{0,0}\right|_{0}\end{array}\right]\leq\left(I-M\right% )^{-1}\left[\begin{array}[]{c}C\left(\left|\alpha\right|_{X}+\left|\beta\right% |_{X}\right)\vskip 3.0pt plus 1.0pt minus 1.0pt\\ C\left(\left|\alpha\right|_{X}+\left|\beta\right|_{X}\right)\end{array}\right].[ start_ARRAY start_ROW start_CELL | italic_x start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT - italic_x start_POSTSUBSCRIPT 0 , 0 end_POSTSUBSCRIPT | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL | italic_y start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT - italic_y start_POSTSUBSCRIPT 0 , 0 end_POSTSUBSCRIPT | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT end_CELL end_ROW end_ARRAY ] ≀ ( italic_I - italic_M ) start_POSTSUPERSCRIPT - 1 end_POSTSUPERSCRIPT [ start_ARRAY start_ROW start_CELL italic_C ( | italic_Ξ± | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + | italic_Ξ² | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ) end_CELL end_ROW start_ROW start_CELL italic_C ( | italic_Ξ± | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + | italic_Ξ² | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ) end_CELL end_ROW end_ARRAY ] .

Third, since the semigroup is compact, H𝐻Hitalic_H maps any bounded set into a compact set. Therefore, the map H𝐻Hitalic_H is completely continuous. The final step is to establish the boundedness of the set of all solutions to the family of equations

H⁒(Ξ±,Ξ²)=λ⁒(Ξ±,Ξ²),Ξ»>1.formulae-sequenceπ»π›Όπ›½πœ†π›Όπ›½πœ†1H\left(\alpha,\beta\right)=\lambda\left(\alpha,\beta\right),\ \ \ \lambda>1.italic_H ( italic_Ξ± , italic_Ξ² ) = italic_Ξ» ( italic_Ξ± , italic_Ξ² ) , italic_Ξ» > 1 .

If (Ξ±,Ξ²)𝛼𝛽\left(\alpha,\beta\right)( italic_Ξ± , italic_Ξ² ) is such a solution, then

Ξ»β’Ξ±πœ†π›Ό\displaystyle\lambda\alphaitalic_Ξ» italic_Ξ± =1a[S(T)Ξ±βˆ’kS(T)Ξ²+kbΞ²\displaystyle=\frac{1}{a}\big{[}S\left(T\right)\alpha-kS\left(T\right)\beta+kb\beta= divide start_ARG 1 end_ARG start_ARG italic_a end_ARG [ italic_S ( italic_T ) italic_Ξ± - italic_k italic_S ( italic_T ) italic_Ξ² + italic_k italic_b italic_Ξ²
(3.10) +∫0TS(Tβˆ’s)(F(xΞ±,Ξ²(s),yΞ±,Ξ²(s))βˆ’kG(xΞ±,Ξ²(s),yΞ±,Ξ²(s)))ds],\displaystyle\quad+\int_{0}^{T}S\left(T-s\right)\left(F\left(x_{\alpha,\beta}% \left(s\right),y_{\alpha,\beta}\left(s\right)\right)-kG\left(x_{\alpha,\beta}% \left(s\right),y_{\alpha,\beta}\left(s\right)\right)\right)ds\big{]},+ ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT ( italic_s ) , italic_y start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT ( italic_s ) ) - italic_k italic_G ( italic_x start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT ( italic_s ) , italic_y start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT ( italic_s ) ) ) italic_d italic_s ] ,
Ξ»β’Ξ²πœ†π›½\displaystyle\lambda\betaitalic_Ξ» italic_Ξ² =1k⁒b[βˆ’S(T)Ξ±+kS(T)Ξ²+aΞ±\displaystyle=\frac{1}{kb}\big{[}-S\left(T\right)\alpha+kS\left(T\right)\beta+a\alpha= divide start_ARG 1 end_ARG start_ARG italic_k italic_b end_ARG [ - italic_S ( italic_T ) italic_Ξ± + italic_k italic_S ( italic_T ) italic_Ξ² + italic_a italic_Ξ±
βˆ’βˆ«0TS(Tβˆ’s)(F(xΞ±,Ξ²(s),yΞ±,Ξ²(s))βˆ’kG(xΞ±,Ξ²(s),yΞ±,Ξ²(s)))ds].\displaystyle\quad-\int_{0}^{T}S\left(T-s\right)\left(F\left(x_{\alpha,\beta}% \left(s\right),y_{\alpha,\beta}\left(s\right)\right)-kG\left(x_{\alpha,\beta}% \left(s\right),y_{\alpha,\beta}\left(s\right)\right)\right)ds\big{]}.- ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT ( italic_s ) , italic_y start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT ( italic_s ) ) - italic_k italic_G ( italic_x start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT ( italic_s ) , italic_y start_POSTSUBSCRIPT italic_Ξ± , italic_Ξ² end_POSTSUBSCRIPT ( italic_s ) ) ) italic_d italic_s ] .

When we add the above two relations, we find

λ⁒(a⁒α+k⁒b⁒β)=a⁒α+k⁒b⁒β,πœ†π‘Žπ›Όπ‘˜π‘π›½π‘Žπ›Όπ‘˜π‘π›½\lambda\left(a\alpha+kb\beta\right)=a\alpha+kb\beta,italic_Ξ» ( italic_a italic_Ξ± + italic_k italic_b italic_Ξ² ) = italic_a italic_Ξ± + italic_k italic_b italic_Ξ² ,

and since Ξ»>1πœ†1\lambda>1italic_Ξ» > 1, this implies a⁒α+k⁒b⁒β=0π‘Žπ›Όπ‘˜π‘π›½0a\alpha+kb\beta=0italic_a italic_Ξ± + italic_k italic_b italic_Ξ² = 0. Substituting k⁒bβ’Ξ²π‘˜π‘π›½kb\betaitalic_k italic_b italic_Ξ² by βˆ’aβ’Ξ±π‘Žπ›Ό-a\alpha- italic_a italic_Ξ± in (3.10) and passing to the norm, in virtue of (ii), we obtain

2⁒|Ξ±|X⁒<(Ξ»+1)|⁒α|X≀(1a+1b)⁒|S⁒(T)|ℒ⁒(X)⁒|Ξ±|X+C~,evaluated-at2subscript𝛼𝑋braπœ†1𝛼𝑋1π‘Ž1𝑏subscript𝑆𝑇ℒ𝑋subscript𝛼𝑋~𝐢2\left|\alpha\right|_{X}<\left(\lambda+1\right)\left|\alpha\right|_{X}\leq% \left(\frac{1}{a}+\frac{1}{b}\right)\left|S\left(T\right)\right|_{\mathcal{L}% \left(X\right)}\left|\alpha\right|_{X}+\widetilde{C},2 | italic_Ξ± | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT < ( italic_Ξ» + 1 ) | italic_Ξ± | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ≀ ( divide start_ARG 1 end_ARG start_ARG italic_a end_ARG + divide start_ARG 1 end_ARG start_ARG italic_b end_ARG ) | italic_S ( italic_T ) | start_POSTSUBSCRIPT caligraphic_L ( italic_X ) end_POSTSUBSCRIPT | italic_Ξ± | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + over~ start_ARG italic_C end_ARG ,

for some constant C~.~𝐢\widetilde{C}.over~ start_ARG italic_C end_ARG . Using the condition on |S⁒(T)|ℒ⁒(X)subscript𝑆𝑇ℒ𝑋\left|S\left(T\right)\right|_{\mathcal{L}\left(X\right)}| italic_S ( italic_T ) | start_POSTSUBSCRIPT caligraphic_L ( italic_X ) end_POSTSUBSCRIPT from (iv), we deduce the boundedness of α𝛼\alphaitalic_Ξ± independently of Ξ».πœ†\lambda.italic_Ξ» . Next from α⁒α+k⁒b⁒β=0,π›Όπ›Όπ‘˜π‘π›½0\alpha\alpha+kb\beta=0,italic_Ξ± italic_Ξ± + italic_k italic_b italic_Ξ² = 0 , we also have that β𝛽\betaitalic_Ξ² is bounded. Therefore Leray-Schauder’s theorem applies and gives the result. ∎

Remark 3.3.

The previous existence result can be seen as an observability result. Indeed, having observed the final relation (3.2), we may guess one of the possible initial states (x⁒(0),y⁒(0))π‘₯0𝑦0\left(x\left(0\right),y\left(0\right)\right)( italic_x ( 0 ) , italic_y ( 0 ) ) of the process.

In the next section we deal with a semi-observability problem for the situation that one of the initial states, say y⁒(0),𝑦0y\left(0\right),italic_y ( 0 ) , is known while the second one x⁒(0)π‘₯0x\left(0\right)italic_x ( 0 ) is found after obtaining a solution of the mutual control problem.

4. A semi-observability problem

In this section, we aim to find a mild solution of the control problem (1.1)-(1.2) assuming that the initial state y⁒(0)=β𝑦0𝛽y\left(0\right)=\betaitalic_y ( 0 ) = italic_Ξ² is known. More exactly, we look for x,y∈C⁒([0,T];X)π‘₯𝑦𝐢0𝑇𝑋x,y\in C\left(\left[0,T\right];X\right)italic_x , italic_y ∈ italic_C ( [ 0 , italic_T ] ; italic_X ) such that, for all t∈[0,T]𝑑0𝑇t\in[0,T]italic_t ∈ [ 0 , italic_T ], the following relations hold:

(4.1) {x⁒(t)=S⁒(t)⁒x⁒(0)+∫0tS⁒(tβˆ’s)⁒F⁒(x⁒(s),y⁒(s))⁒𝑑sy⁒(t)=S⁒(t)⁒y⁒(0)+∫0tS⁒(tβˆ’s)⁒G⁒(x⁒(s),y⁒(s))⁒𝑑s,casesπ‘₯𝑑𝑆𝑑π‘₯0superscriptsubscript0𝑑𝑆𝑑𝑠𝐹π‘₯𝑠𝑦𝑠differential-d𝑠otherwise𝑦𝑑𝑆𝑑𝑦0superscriptsubscript0𝑑𝑆𝑑𝑠𝐺π‘₯𝑠𝑦𝑠differential-d𝑠otherwise\begin{cases}x\left(t\right)=S\left(t\right)x\left(0\right)+\int_{0}^{t}S\left% (t-s\right)F\left(x\left(s\right),y\left(s\right)\right)ds\\ y\left(t\right)=S\left(t\right)y\left(0\right)+\int_{0}^{t}S\left(t-s\right)G% \left(x\left(s\right),y\left(s\right)\right)ds,\end{cases}{ start_ROW start_CELL italic_x ( italic_t ) = italic_S ( italic_t ) italic_x ( 0 ) + ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_t end_POSTSUPERSCRIPT italic_S ( italic_t - italic_s ) italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s end_CELL start_CELL end_CELL end_ROW start_ROW start_CELL italic_y ( italic_t ) = italic_S ( italic_t ) italic_y ( 0 ) + ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_t end_POSTSUPERSCRIPT italic_S ( italic_t - italic_s ) italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s , end_CELL start_CELL end_CELL end_ROW
(4.2) y⁒(0)=Ξ²,𝑦0𝛽y\left(0\right)=\beta,italic_y ( 0 ) = italic_Ξ² ,
(4.3) x⁒(T)βˆ’a⁒x⁒(0)=k⁒(y⁒(T)βˆ’b⁒y⁒(0)).π‘₯π‘‡π‘Žπ‘₯0π‘˜π‘¦π‘‡π‘π‘¦0x\left(T\right)-ax\left(0\right)=k\left(y\left(T\right)-by\left(0\right)\right).italic_x ( italic_T ) - italic_a italic_x ( 0 ) = italic_k ( italic_y ( italic_T ) - italic_b italic_y ( 0 ) ) .

4.1. Fixed point formulation of the problem

Similar to the previous section, we try to incorporate all the equations in only one fixed point problem. Let (x,y)π‘₯𝑦\left(x,y\right)( italic_x , italic_y ) be a solution of (4.1)-(4.3). Then, using (4.1) and (4.3) gives

S⁒(T)⁒(x⁒(0)βˆ’k⁒β)+∫0TS⁒(Tβˆ’s)⁒(F⁒(x⁒(s),y⁒(s))βˆ’k⁒G⁒(x⁒(s),y⁒(s)))⁒𝑑s=a⁒x⁒(0)βˆ’k⁒b⁒β,𝑆𝑇π‘₯0π‘˜π›½superscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯π‘ π‘¦π‘ π‘˜πΊπ‘₯𝑠𝑦𝑠differential-dπ‘ π‘Žπ‘₯0π‘˜π‘π›½S\left(T\right)\left(x\left(0\right)-k\beta\right)+\int_{0}^{T}S\left(T-s% \right)\left(F\left(x(s),y(s)\right)-kG\left(x(s),y(s)\right)\right)ds=ax\left% (0\right)-kb\beta,italic_S ( italic_T ) ( italic_x ( 0 ) - italic_k italic_Ξ² ) + ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s = italic_a italic_x ( 0 ) - italic_k italic_b italic_Ξ² ,

whence

(4.4) x⁒(0)π‘₯0\displaystyle x\left(0\right)italic_x ( 0 ) =1a⁒(S⁒(T)⁒(x⁒(0)βˆ’k⁒β)+k⁒b⁒β)absent1π‘Žπ‘†π‘‡π‘₯0π‘˜π›½π‘˜π‘π›½\displaystyle=\frac{1}{a}\left(S\left(T\right)\left(x\left(0\right)-k\beta% \right)+kb\beta\right)= divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ( italic_S ( italic_T ) ( italic_x ( 0 ) - italic_k italic_Ξ² ) + italic_k italic_b italic_Ξ² )
+1a⁒∫0TS⁒(Tβˆ’s)⁒(F⁒(x⁒(s),y⁒(s))⁒d⁒sβˆ’k⁒G⁒(x⁒(s),y⁒(s)))⁒𝑑s.1π‘Žsuperscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯π‘ π‘¦π‘ π‘‘π‘ π‘˜πΊπ‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+\frac{1}{a}\int_{0}^{T}S\left(T-s\right)\left(F\left(x(s),y% (s)\right)ds-kG\left(x(s),y(s)\right)\right)\,ds.+ divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s .

When we substitute it in (4.1), one has

(4.5) {x⁒(t)=N1⁒(x,y)⁒(t)y⁒(t)=N2⁒(x,y)⁒(t),casesπ‘₯𝑑subscript𝑁1π‘₯𝑦𝑑otherwise𝑦𝑑subscript𝑁2π‘₯𝑦𝑑otherwise\begin{cases}x\left(t\right)=N_{1}\left(x,y\right)\left(t\right)\\ y\left(t\right)=N_{2}\left(x,y\right)\left(t\right),\end{cases}{ start_ROW start_CELL italic_x ( italic_t ) = italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) ( italic_t ) end_CELL start_CELL end_CELL end_ROW start_ROW start_CELL italic_y ( italic_t ) = italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) ( italic_t ) , end_CELL start_CELL end_CELL end_ROW

where

N1⁒(x,y)⁒(t)subscript𝑁1π‘₯𝑦𝑑\displaystyle N_{1}(x,y)(t)italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) ( italic_t ) =1a⁒S⁒(t+T)⁒(x⁒(0)βˆ’k⁒β)+k⁒ba⁒S⁒(t)⁒βabsent1π‘Žπ‘†π‘‘π‘‡π‘₯0π‘˜π›½π‘˜π‘π‘Žπ‘†π‘‘π›½\displaystyle=\frac{1}{a}S(t+T)\left(x(0)-k\beta\right)+k\frac{b}{a}S(t)\beta= divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_S ( italic_t + italic_T ) ( italic_x ( 0 ) - italic_k italic_Ξ² ) + italic_k divide start_ARG italic_b end_ARG start_ARG italic_a end_ARG italic_S ( italic_t ) italic_Ξ²
+∫0tS⁒(tβˆ’s)⁒F⁒(x⁒(s),y⁒(s))⁒𝑑ssuperscriptsubscript0𝑑𝑆𝑑𝑠𝐹π‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+\int_{0}^{t}S(t-s)F(x(s),y(s))\,ds+ ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_t end_POSTSUPERSCRIPT italic_S ( italic_t - italic_s ) italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s
+1a⁒∫0TS⁒(t+Tβˆ’s)⁒(F⁒(x,yβˆ’k⁒G⁒(x,y))),1π‘Žsuperscriptsubscript0𝑇𝑆𝑑𝑇𝑠𝐹π‘₯π‘¦π‘˜πΊπ‘₯𝑦\displaystyle\quad+\frac{1}{a}\int_{0}^{T}S(t+T-s)\left(F(x,y-kG(x,y))\right),+ divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_t + italic_T - italic_s ) ( italic_F ( italic_x , italic_y - italic_k italic_G ( italic_x , italic_y ) ) ) ,
N2⁒(x,y)⁒(t)subscript𝑁2π‘₯𝑦𝑑\displaystyle N_{2}(x,y)(t)italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) ( italic_t ) =S⁒(t)⁒β+∫0tS⁒(tβˆ’s)⁒G⁒(x⁒(s),y⁒(s))⁒𝑑s.absent𝑆𝑑𝛽superscriptsubscript0𝑑𝑆𝑑𝑠𝐺π‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle=S(t)\beta+\int_{0}^{t}S(t-s)G(x(s),y(s))\,ds.= italic_S ( italic_t ) italic_Ξ² + ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_t end_POSTSUPERSCRIPT italic_S ( italic_t - italic_s ) italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s .

The converse implication also holds.

Lemma 4.1.

A pair (x,y)π‘₯𝑦\left(x,y\right)( italic_x , italic_y ) solves the system (4.5)4.5(\ref{E0})( ) if and only if it solves (4.1)4.1(\ref{E1})( )-(4.3)4.3(\ref{E3})( ).

Proof.

We only have to prove that (4.5) implies (4.1)-(4.3). Clearly, (4.2) follows directly from the second equation in (4.5). Setting t=0𝑑0t=0italic_t = 0 in the first equation of (4.5) gives (4.4), while setting t=T𝑑𝑇t=Titalic_t = italic_T provides

x⁒(T)π‘₯𝑇\displaystyle x(T)italic_x ( italic_T ) =S⁒(T)⁒[1a⁒S⁒(T)⁒(x⁒(0)βˆ’k⁒β)+k⁒ba⁒β]absent𝑆𝑇delimited-[]1π‘Žπ‘†π‘‡π‘₯0π‘˜π›½π‘˜π‘π‘Žπ›½\displaystyle=S(T)\left[\frac{1}{a}S(T)\left(x(0)-k\beta\right)+k\frac{b}{a}% \beta\right]= italic_S ( italic_T ) [ divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_S ( italic_T ) ( italic_x ( 0 ) - italic_k italic_Ξ² ) + italic_k divide start_ARG italic_b end_ARG start_ARG italic_a end_ARG italic_Ξ² ]
+1a⁒S⁒(T)⁒∫0TS⁒(Tβˆ’s)⁒(F⁒(x⁒(s),y⁒(s))βˆ’k⁒G⁒(x⁒(s),y⁒(s)))⁒𝑑s1π‘Žπ‘†π‘‡superscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯π‘ π‘¦π‘ π‘˜πΊπ‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+\frac{1}{a}S(T)\int_{0}^{T}S(T-s)\left(F(x(s),y(s))-kG(x(s)% ,y(s))\right)ds+ divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_S ( italic_T ) ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s
+∫0TS⁒(Tβˆ’s)⁒F⁒(x⁒(s),y⁒(s))⁒𝑑s.superscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+\int_{0}^{T}S(T-s)F(x(s),y(s))ds.+ ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s .

From (4.4), one has

S⁒(T)⁒x⁒(0)=x⁒(T)βˆ’βˆ«0TS⁒(Tβˆ’s)⁒F⁒(x⁒(s),y⁒(s))⁒𝑑s,𝑆𝑇π‘₯0π‘₯𝑇superscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯𝑠𝑦𝑠differential-d𝑠S\left(T\right)x\left(0\right)=x\left(T\right)-\int_{0}^{T}S\left(T-s\right)F% \left(x(s),y(s)\right)ds,italic_S ( italic_T ) italic_x ( 0 ) = italic_x ( italic_T ) - ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s ,

and using it in (4.4) yields

x⁒(0)π‘₯0\displaystyle x(0)italic_x ( 0 ) =1a⁒x⁒(T)βˆ’1a⁒∫0TS⁒(Tβˆ’s)⁒F⁒(x⁒(s),y⁒(s))⁒𝑑sβˆ’k⁒1a⁒S⁒(T)⁒β+k⁒ba⁒βabsent1π‘Žπ‘₯𝑇1π‘Žsuperscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯𝑠𝑦𝑠differential-dπ‘ π‘˜1π‘Žπ‘†π‘‡π›½π‘˜π‘π‘Žπ›½\displaystyle=\frac{1}{a}x(T)-\frac{1}{a}\int_{0}^{T}S(T-s)F(x(s),y(s))ds-k% \frac{1}{a}S(T)\beta+k\frac{b}{a}\beta= divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_x ( italic_T ) - divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s - italic_k divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_S ( italic_T ) italic_Ξ² + italic_k divide start_ARG italic_b end_ARG start_ARG italic_a end_ARG italic_Ξ²
+1a⁒∫0TS⁒(Tβˆ’s)⁒(F⁒(x⁒(s),y⁒(s))βˆ’k⁒G⁒(x⁒(s),y⁒(s)))⁒𝑑s1π‘Žsuperscriptsubscript0𝑇𝑆𝑇𝑠𝐹π‘₯π‘ π‘¦π‘ π‘˜πΊπ‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle\quad+\frac{1}{a}\int_{0}^{T}S(T-s)\left(F(x(s),y(s))-kG(x(s),y(s% ))\right)ds+ divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) ( italic_F ( italic_x ( italic_s ) , italic_y ( italic_s ) ) - italic_k italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) ) italic_d italic_s
=1a⁒x⁒(T)βˆ’k⁒1a⁒S⁒(T)⁒β+k⁒baβ’Ξ²βˆ’k⁒1a⁒∫0TS⁒(Tβˆ’s)⁒G⁒(x⁒(s),y⁒(s))⁒𝑑sabsent1π‘Žπ‘₯π‘‡π‘˜1π‘Žπ‘†π‘‡π›½π‘˜π‘π‘Žπ›½π‘˜1π‘Žsuperscriptsubscript0𝑇𝑆𝑇𝑠𝐺π‘₯𝑠𝑦𝑠differential-d𝑠\displaystyle=\frac{1}{a}x(T)-k\frac{1}{a}S(T)\beta+k\frac{b}{a}\beta-k\frac{1% }{a}\int_{0}^{T}S(T-s)G(x(s),y(s))ds= divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_x ( italic_T ) - italic_k divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_S ( italic_T ) italic_Ξ² + italic_k divide start_ARG italic_b end_ARG start_ARG italic_a end_ARG italic_Ξ² - italic_k divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s
=1a⁒x⁒(T)βˆ’k⁒1a⁒[S⁒(T)⁒β+∫0TS⁒(Tβˆ’s)⁒G⁒(x⁒(s),y⁒(s))⁒𝑑s]+k⁒ba⁒βabsent1π‘Žπ‘₯π‘‡π‘˜1π‘Ždelimited-[]𝑆𝑇𝛽superscriptsubscript0𝑇𝑆𝑇𝑠𝐺π‘₯𝑠𝑦𝑠differential-dπ‘ π‘˜π‘π‘Žπ›½\displaystyle=\frac{1}{a}x(T)-k\frac{1}{a}\left[S(T)\beta+\int_{0}^{T}S(T-s)G(% x(s),y(s))ds\right]+k\frac{b}{a}\beta= divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_x ( italic_T ) - italic_k divide start_ARG 1 end_ARG start_ARG italic_a end_ARG [ italic_S ( italic_T ) italic_Ξ² + ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_S ( italic_T - italic_s ) italic_G ( italic_x ( italic_s ) , italic_y ( italic_s ) ) italic_d italic_s ] + italic_k divide start_ARG italic_b end_ARG start_ARG italic_a end_ARG italic_Ξ²
=1a⁒x⁒(T)βˆ’k⁒1a⁒y⁒(T)+k⁒ba⁒β,absent1π‘Žπ‘₯π‘‡π‘˜1π‘Žπ‘¦π‘‡π‘˜π‘π‘Žπ›½\displaystyle=\frac{1}{a}x(T)-k\frac{1}{a}y(T)+k\frac{b}{a}\beta,= divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_x ( italic_T ) - italic_k divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_y ( italic_T ) + italic_k divide start_ARG italic_b end_ARG start_ARG italic_a end_ARG italic_Ξ² ,

that is (4.3). Finally, combining (4.4) and the first equation of (4.5) results in the first equation of (4.1). ∎

4.2. Existence and uniqueness via Perov’s fixed point theorem

Using Perov’s fixed point theorem, we obtain the following existence and uniqueness result.

Theorem 4.2.

Assume that the following conditions are satisfied:

  • (i)

    There are nonnegative constants a11,a12,a21,a22subscriptπ‘Ž11subscriptπ‘Ž12subscriptπ‘Ž21subscriptπ‘Ž22a_{11},a_{12},a_{21},a_{22}italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT , italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT , italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT , italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT such that

    |F⁒(x,y)βˆ’F⁒(xΒ―,yΒ―)|X≀a11⁒|xβˆ’xΒ―|X+a12⁒|yβˆ’yΒ―|X,subscript𝐹π‘₯𝑦𝐹¯π‘₯¯𝑦𝑋subscriptπ‘Ž11subscriptπ‘₯Β―π‘₯𝑋subscriptπ‘Ž12subscript𝑦¯𝑦𝑋\displaystyle|F(x,y)-F(\overline{x},\overline{y})|_{X}\leq a_{11}|x-\overline{% x}|_{X}+a_{12}|y-\overline{y}|_{X},| italic_F ( italic_x , italic_y ) - italic_F ( overΒ― start_ARG italic_x end_ARG , overΒ― start_ARG italic_y end_ARG ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ≀ italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT | italic_x - overΒ― start_ARG italic_x end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT | italic_y - overΒ― start_ARG italic_y end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ,
    |G⁒(x,y)βˆ’G⁒(xΒ―,yΒ―)|X≀a21⁒|xβˆ’xΒ―|X+a22⁒|yβˆ’yΒ―|X,subscript𝐺π‘₯𝑦𝐺¯π‘₯¯𝑦𝑋subscriptπ‘Ž21subscriptπ‘₯Β―π‘₯𝑋subscriptπ‘Ž22subscript𝑦¯𝑦𝑋\displaystyle|G(x,y)-G(\overline{x},\overline{y})|_{X}\leq a_{21}|x-\overline{% x}|_{X}+a_{22}|y-\overline{y}|_{X},| italic_G ( italic_x , italic_y ) - italic_G ( overΒ― start_ARG italic_x end_ARG , overΒ― start_ARG italic_y end_ARG ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ≀ italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT | italic_x - overΒ― start_ARG italic_x end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT | italic_y - overΒ― start_ARG italic_y end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ,

    for all x,xΒ―,y,y¯∈Xπ‘₯Β―π‘₯𝑦¯𝑦𝑋x,\overline{x},y,\overline{y}\in Xitalic_x , overΒ― start_ARG italic_x end_ARG , italic_y , overΒ― start_ARG italic_y end_ARG ∈ italic_X and t∈[0,T];𝑑0𝑇t\in\left[0,T\right];italic_t ∈ [ 0 , italic_T ] ;

  • (ii)

    There exists ΞΈβ‰₯0πœƒ0\theta\geq 0italic_ΞΈ β‰₯ 0 such that the matrix

    M⁒(ΞΈ):=CA⁒[1a+(1+1a)⁒T⁒a11+ka⁒T⁒a21((1+1a)⁒a12+ka⁒a22)⁒eθ⁒Tβˆ’1ΞΈT⁒a21a22⁒1βˆ’eβˆ’ΞΈβ’TΞΈ]assignπ‘€πœƒsubscript𝐢𝐴matrix1π‘Ž11π‘Žπ‘‡subscriptπ‘Ž11π‘˜π‘Žπ‘‡subscriptπ‘Ž2111π‘Žsubscriptπ‘Ž12π‘˜π‘Žsubscriptπ‘Ž22superscriptπ‘’πœƒπ‘‡1πœƒπ‘‡subscriptπ‘Ž21subscriptπ‘Ž221superscriptπ‘’πœƒπ‘‡πœƒM(\theta):=C_{A}\begin{bmatrix}\frac{1}{a}+\left(1+\frac{1}{a}\right)Ta_{11}+% \frac{k}{a}Ta_{21}&\left(\left(1+\frac{1}{a}\right)a_{12}+\frac{k}{a}a_{22}% \right)\frac{e^{\theta T}-1}{\theta}\\[3.0pt] Ta_{21}&a_{22}\,\frac{1-e^{-\theta T}}{\theta}\end{bmatrix}italic_M ( italic_ΞΈ ) := italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT [ start_ARG start_ROW start_CELL divide start_ARG 1 end_ARG start_ARG italic_a end_ARG + ( 1 + divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ) italic_T italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT + divide start_ARG italic_k end_ARG start_ARG italic_a end_ARG italic_T italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT end_CELL start_CELL ( ( 1 + divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ) italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT + divide start_ARG italic_k end_ARG start_ARG italic_a end_ARG italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT ) divide start_ARG italic_e start_POSTSUPERSCRIPT italic_ΞΈ italic_T end_POSTSUPERSCRIPT - 1 end_ARG start_ARG italic_ΞΈ end_ARG end_CELL end_ROW start_ROW start_CELL italic_T italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT end_CELL start_CELL italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT divide start_ARG 1 - italic_e start_POSTSUPERSCRIPT - italic_ΞΈ italic_T end_POSTSUPERSCRIPT end_ARG start_ARG italic_ΞΈ end_ARG end_CELL end_ROW end_ARG ]

    is convergent to zero.

Then, for every β∈X𝛽𝑋\beta\in Xitalic_Ξ² ∈ italic_X, problem (3.1)-(3.2) has a unique solution (x,y)π‘₯𝑦\left(x,y\right)( italic_x , italic_y ) in C⁒([0,T];X)2𝐢superscript0𝑇𝑋2C\left(\left[0,T\right];X\right)^{2}italic_C ( [ 0 , italic_T ] ; italic_X ) start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT with y⁒(0)=Ξ².𝑦0𝛽y\left(0\right)=\beta.italic_y ( 0 ) = italic_Ξ² .

Proof.

We apply Perov’s fixed point theorem to the operator (N1,N2)subscript𝑁1subscript𝑁2(N_{1},N_{2})( italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ) with the following choice of spaces: X1=subscript𝑋1absentX_{1}=italic_X start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT = C⁒([0,T];X)𝐢0𝑇𝑋C([0,T];X)italic_C ( [ 0 , italic_T ] ; italic_X ) endowed with the uniform norm, and X2={y∈C⁒([0,T];X):y⁒(0)=Ξ²}subscript𝑋2conditional-set𝑦𝐢0𝑇𝑋𝑦0𝛽X_{2}=\left\{y\in C([0,T];X):\ y\left(0\right)=\beta\right\}italic_X start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT = { italic_y ∈ italic_C ( [ 0 , italic_T ] ; italic_X ) : italic_y ( 0 ) = italic_Ξ² } endowed with the metric induced by the Bielecki norm |β‹…|ΞΈ\left|\cdot\right|_{\theta}| β‹… | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT on C⁒([0,T];X)𝐢0𝑇𝑋C([0,T];X)italic_C ( [ 0 , italic_T ] ; italic_X ). Clearly, N1⁒(X1Γ—X2)βŠ‚X1,subscript𝑁1subscript𝑋1subscript𝑋2subscript𝑋1N_{1}\left(X_{1}\times X_{2}\right)\subset X_{1},italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_X start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_X start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ) βŠ‚ italic_X start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , while the inclusion N2⁒(X1Γ—X2)βŠ‚X2subscript𝑁2subscript𝑋1subscript𝑋2subscript𝑋2N_{2}\left(X_{1}\times X_{2}\right)\subset X_{2}italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_X start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_X start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ) βŠ‚ italic_X start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT is obvious from the definition of N2.subscript𝑁2N_{2}.italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT . Next, let x,x¯∈X1π‘₯Β―π‘₯subscript𝑋1x,\overline{x}\in X_{1}italic_x , overΒ― start_ARG italic_x end_ARG ∈ italic_X start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT and y,y¯∈X2𝑦¯𝑦subscript𝑋2y,\overline{y}\in X_{2}italic_y , overΒ― start_ARG italic_y end_ARG ∈ italic_X start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT. One has

|N1⁒(x,y)⁒(t)βˆ’N1⁒(xΒ―,yΒ―)⁒(t)|Xsubscriptsubscript𝑁1π‘₯𝑦𝑑subscript𝑁1Β―π‘₯¯𝑦𝑑𝑋\displaystyle\left|N_{1}(x,y)\left(t\right)-N_{1}(\overline{x},\overline{y})% \left(t\right)\right|_{X}| italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) ( italic_t ) - italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( overΒ― start_ARG italic_x end_ARG , overΒ― start_ARG italic_y end_ARG ) ( italic_t ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT
≀1a⁒CA⁒|xβˆ’xΒ―|0+((1+1a)⁒CA⁒T⁒a11+ka⁒CA⁒T⁒a21)⁒|xβˆ’xΒ―|0absent1π‘Žsubscript𝐢𝐴subscriptπ‘₯Β―π‘₯011π‘Žsubscript𝐢𝐴𝑇subscriptπ‘Ž11π‘˜π‘Žsubscript𝐢𝐴𝑇subscriptπ‘Ž21subscriptπ‘₯Β―π‘₯0\displaystyle\leq\frac{1}{a}C_{A}\left|x-\overline{x}\right|_{0}+\left(\left(1% +\frac{1}{a}\right)C_{A}Ta_{11}+\frac{k}{a}C_{A}Ta_{21}\right)\left|x-% \overline{x}\right|_{0}≀ divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT | italic_x - overΒ― start_ARG italic_x end_ARG | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT + ( ( 1 + divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ) italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT italic_T italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT + divide start_ARG italic_k end_ARG start_ARG italic_a end_ARG italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT italic_T italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT ) | italic_x - overΒ― start_ARG italic_x end_ARG | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT
+((1+1a)⁒CA⁒a12+ka⁒CA⁒a22)⁒∫0T|y⁒(s)βˆ’y¯⁒(s)|X⁒𝑑s11π‘Žsubscript𝐢𝐴subscriptπ‘Ž12π‘˜π‘Žsubscript𝐢𝐴subscriptπ‘Ž22superscriptsubscript0𝑇subscript𝑦𝑠¯𝑦𝑠𝑋differential-d𝑠\displaystyle\quad+\left(\left(1+\frac{1}{a}\right)C_{A}a_{12}+\frac{k}{a}C_{A% }a_{22}\right)\int_{0}^{T}\left|y\left(s\right)-\overline{y}\left(s\right)% \right|_{X}ds+ ( ( 1 + divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ) italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT + divide start_ARG italic_k end_ARG start_ARG italic_a end_ARG italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT ) ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT | italic_y ( italic_s ) - overΒ― start_ARG italic_y end_ARG ( italic_s ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT italic_d italic_s
≀m11⁒|xβˆ’xΒ―|0+m12⁒eθ⁒Tβˆ’1θ⁒|yβˆ’yΒ―|ΞΈ,absentsubscriptπ‘š11subscriptπ‘₯Β―π‘₯0subscriptπ‘š12superscriptπ‘’πœƒπ‘‡1πœƒsubscriptπ‘¦Β―π‘¦πœƒ\displaystyle\leq m_{11}\left|x-\overline{x}\right|_{0}+m_{12}\frac{e^{\theta T% }-1}{\theta}|y-\overline{y}|_{\theta},≀ italic_m start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT | italic_x - overΒ― start_ARG italic_x end_ARG | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT + italic_m start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT divide start_ARG italic_e start_POSTSUPERSCRIPT italic_ΞΈ italic_T end_POSTSUPERSCRIPT - 1 end_ARG start_ARG italic_ΞΈ end_ARG | italic_y - overΒ― start_ARG italic_y end_ARG | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT ,

where

m11subscriptπ‘š11\displaystyle m_{11}italic_m start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT =CA⁒(1a+(1+1a)⁒T⁒a11+ka⁒T⁒a21),absentsubscript𝐢𝐴1π‘Ž11π‘Žπ‘‡subscriptπ‘Ž11π‘˜π‘Žπ‘‡subscriptπ‘Ž21\displaystyle=C_{A}\left(\frac{1}{a}+\left(1+\frac{1}{a}\right)Ta_{11}+\frac{k% }{a}Ta_{21}\right),= italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( divide start_ARG 1 end_ARG start_ARG italic_a end_ARG + ( 1 + divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ) italic_T italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT + divide start_ARG italic_k end_ARG start_ARG italic_a end_ARG italic_T italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT ) ,
m12subscriptπ‘š12\displaystyle m_{12}italic_m start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT =CA⁒((1+1a)⁒a12+ka⁒a22).absentsubscript𝐢𝐴11π‘Žsubscriptπ‘Ž12π‘˜π‘Žsubscriptπ‘Ž22\displaystyle=C_{A}\left(\left(1+\frac{1}{a}\right)a_{12}+\frac{k}{a}a_{22}% \right).= italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( ( 1 + divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ) italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT + divide start_ARG italic_k end_ARG start_ARG italic_a end_ARG italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT ) .

Therefore, taking the supremum over t∈[0,T]𝑑0𝑇t\in[0,T]italic_t ∈ [ 0 , italic_T ] yields

(4.6) |N1⁒(x,y)βˆ’N1⁒(xΒ―,yΒ―)|0≀m11⁒|xβˆ’xΒ―|0+m12⁒eθ⁒Tβˆ’1θ⁒|yβˆ’yΒ―|ΞΈ.subscriptsubscript𝑁1π‘₯𝑦subscript𝑁1Β―π‘₯¯𝑦0subscriptπ‘š11subscriptπ‘₯Β―π‘₯0subscriptπ‘š12superscriptπ‘’πœƒπ‘‡1πœƒsubscriptπ‘¦Β―π‘¦πœƒ\left|N_{1}(x,y)-N_{1}(\overline{x},\overline{y})\right|_{0}\leq m_{11}|x-% \overline{x}|_{0}+m_{12}\frac{e^{\theta T}-1}{\theta}|y-\overline{y}|_{\theta}.| italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) - italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( overΒ― start_ARG italic_x end_ARG , overΒ― start_ARG italic_y end_ARG ) | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT ≀ italic_m start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT | italic_x - overΒ― start_ARG italic_x end_ARG | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT + italic_m start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT divide start_ARG italic_e start_POSTSUPERSCRIPT italic_ΞΈ italic_T end_POSTSUPERSCRIPT - 1 end_ARG start_ARG italic_ΞΈ end_ARG | italic_y - overΒ― start_ARG italic_y end_ARG | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT .

For the second operator N2subscript𝑁2N_{2}italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT, we estimate

|N2⁒(x,y)⁒(t)βˆ’N2⁒(xΒ―,yΒ―)⁒(t)|Xsubscriptsubscript𝑁2π‘₯𝑦𝑑subscript𝑁2Β―π‘₯¯𝑦𝑑𝑋\displaystyle\left|N_{2}(x,y)\left(t\right)-N_{2}(\overline{x},\overline{y})% \left(t\right)\right|_{X}| italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) ( italic_t ) - italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( overΒ― start_ARG italic_x end_ARG , overΒ― start_ARG italic_y end_ARG ) ( italic_t ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ≀CA⁒T⁒a21⁒|xβˆ’xΒ―|0absentsubscript𝐢𝐴𝑇subscriptπ‘Ž21subscriptπ‘₯Β―π‘₯0\displaystyle\leq\,\,C_{A}Ta_{21}|x-\overline{x}|_{0}≀ italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT italic_T italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT | italic_x - overΒ― start_ARG italic_x end_ARG | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT
+a22⁒CA⁒∫0t|y⁒(s)βˆ’y¯⁒(s)|X⁒𝑑ssubscriptπ‘Ž22subscript𝐢𝐴superscriptsubscript0𝑑subscript𝑦𝑠¯𝑦𝑠𝑋differential-d𝑠\displaystyle+a_{22}\,C_{A}\int_{0}^{t}|y(s)-\overline{y}(s)|_{X}ds+ italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_t end_POSTSUPERSCRIPT | italic_y ( italic_s ) - overΒ― start_ARG italic_y end_ARG ( italic_s ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT italic_d italic_s
≀m21⁒|xβˆ’xΒ―|0+m22⁒eθ⁒tβˆ’1θ⁒|yβˆ’yΒ―|ΞΈ,absentsubscriptπ‘š21subscriptπ‘₯Β―π‘₯0subscriptπ‘š22superscriptπ‘’πœƒπ‘‘1πœƒsubscriptπ‘¦Β―π‘¦πœƒ\displaystyle\leq m_{21}|x-\overline{x}|_{0}+m_{22}\frac{e^{\theta t}-1}{% \theta}|y-\overline{y}|_{\theta},≀ italic_m start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT | italic_x - overΒ― start_ARG italic_x end_ARG | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT + italic_m start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT divide start_ARG italic_e start_POSTSUPERSCRIPT italic_ΞΈ italic_t end_POSTSUPERSCRIPT - 1 end_ARG start_ARG italic_ΞΈ end_ARG | italic_y - overΒ― start_ARG italic_y end_ARG | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT ,

where

m21=CA⁒T⁒a21,m22=CA⁒a22.formulae-sequencesubscriptπ‘š21subscript𝐢𝐴𝑇subscriptπ‘Ž21subscriptπ‘š22subscript𝐢𝐴subscriptπ‘Ž22m_{21}=\,C_{A}Ta_{21},\,\ \ m_{22}=C_{A}a_{22}.italic_m start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT = italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT italic_T italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT , italic_m start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT = italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT .

Multiplying the both sides by eβˆ’ΞΈβ’tsuperscriptπ‘’πœƒπ‘‘e^{-\theta t}italic_e start_POSTSUPERSCRIPT - italic_ΞΈ italic_t end_POSTSUPERSCRIPT and taking the supremum over t∈[0,T]𝑑0𝑇t\in[0,T]italic_t ∈ [ 0 , italic_T ], we obtain

(4.7) |N2⁒(x,y)βˆ’N2⁒(xΒ―,yΒ―)|θ≀m21⁒|xβˆ’xΒ―|0+m22⁒1βˆ’eβˆ’ΞΈβ’Tθ⁒|yβˆ’yΒ―|ΞΈ.subscriptsubscript𝑁2π‘₯𝑦subscript𝑁2Β―π‘₯Β―π‘¦πœƒsubscriptπ‘š21subscriptπ‘₯Β―π‘₯0subscriptπ‘š221superscriptπ‘’πœƒπ‘‡πœƒsubscriptπ‘¦Β―π‘¦πœƒ\left|N_{2}(x,y)-N_{2}(\overline{x},\overline{y})\right|_{\theta}\leq m_{21}|x% -\overline{x}|_{0}+m_{22}\frac{1-e^{-\theta T}}{\theta}|y-\overline{y}|_{% \theta}.| italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) - italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( overΒ― start_ARG italic_x end_ARG , overΒ― start_ARG italic_y end_ARG ) | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT ≀ italic_m start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT | italic_x - overΒ― start_ARG italic_x end_ARG | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT + italic_m start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT divide start_ARG 1 - italic_e start_POSTSUPERSCRIPT - italic_ΞΈ italic_T end_POSTSUPERSCRIPT end_ARG start_ARG italic_ΞΈ end_ARG | italic_y - overΒ― start_ARG italic_y end_ARG | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT .

Now, writing inequalities (4.6) and (4.7) in a vector form, gives

[|N1⁒(x,y)βˆ’N1⁒(xΒ―,yΒ―)|0|N2⁒(x,y)βˆ’N2⁒(xΒ―,yΒ―)|ΞΈ]≀M⁒(ΞΈ)⁒[|xβˆ’xΒ―|0|yβˆ’yΒ―|ΞΈ],matrixsubscriptsubscript𝑁1π‘₯𝑦subscript𝑁1Β―π‘₯¯𝑦0subscriptsubscript𝑁2π‘₯𝑦subscript𝑁2Β―π‘₯Β―π‘¦πœƒπ‘€πœƒmatrixsubscriptπ‘₯Β―π‘₯0subscriptπ‘¦Β―π‘¦πœƒ\begin{bmatrix}\left|N_{1}(x,y)-N_{1}(\overline{x},\overline{y})\right|_{0}% \vskip 3.0pt plus 1.0pt minus 1.0pt\\ \left|N_{2}(x,y)-N_{2}(\overline{x},\overline{y})\right|_{\theta}\end{bmatrix}% \leq M(\theta)\begin{bmatrix}|x-\overline{x}|_{0}\vskip 3.0pt plus 1.0pt minus% 1.0pt\\ |y-\overline{y}|_{\theta}\end{bmatrix},[ start_ARG start_ROW start_CELL | italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) - italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( overΒ― start_ARG italic_x end_ARG , overΒ― start_ARG italic_y end_ARG ) | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL | italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) - italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( overΒ― start_ARG italic_x end_ARG , overΒ― start_ARG italic_y end_ARG ) | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT end_CELL end_ROW end_ARG ] ≀ italic_M ( italic_ΞΈ ) [ start_ARG start_ROW start_CELL | italic_x - overΒ― start_ARG italic_x end_ARG | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL | italic_y - overΒ― start_ARG italic_y end_ARG | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT end_CELL end_ROW end_ARG ] ,

where from assumption (ii), the matrix M⁒(ΞΈ)π‘€πœƒM(\theta)italic_M ( italic_ΞΈ ) is convergent to zero. Therefore, Perov’s fixed point theorem applies and guarantees the existence of a unique fixed point (x,y)∈X1Γ—X2π‘₯𝑦subscript𝑋1subscript𝑋2\left(x,y\right)\in X_{1}\times X_{2}( italic_x , italic_y ) ∈ italic_X start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_X start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT of the operator (N1,N2)subscript𝑁1subscript𝑁2(N_{1},N_{2})( italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ). ∎

4.3. Existence via Schauder’s fixed point theorem

The next result does not require Lipschitz conditions for F𝐹Fitalic_F and G,𝐺G,italic_G , but only linear growth ones. Although this sacrifices uniqueness, it offers the advantage of localizing the solution.

Theorem 4.3.

Assume the there are nonnegative constants ai⁒j,subscriptπ‘Žπ‘–π‘—a_{ij},italic_a start_POSTSUBSCRIPT italic_i italic_j end_POSTSUBSCRIPT , i=1,2;𝑖12i=1,2;italic_i = 1 , 2 ; j=1,2,3𝑗123j=1,2,3italic_j = 1 , 2 , 3 such that

(4.8) |F⁒(x,y)|X≀a11⁒|x|X+a12⁒|y|X+a13,subscript𝐹π‘₯𝑦𝑋subscriptπ‘Ž11subscriptπ‘₯𝑋subscriptπ‘Ž12subscript𝑦𝑋subscriptπ‘Ž13\displaystyle|F(x,y)|_{X}\leq a_{11}|x|_{X}+a_{12}|y|_{X}+a_{13},| italic_F ( italic_x , italic_y ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ≀ italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT | italic_x | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT | italic_y | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 13 end_POSTSUBSCRIPT ,
|G⁒(x,y)|X≀a21⁒|x|X+a22⁒|y|X+a23,subscript𝐺π‘₯𝑦𝑋subscriptπ‘Ž21subscriptπ‘₯𝑋subscriptπ‘Ž22subscript𝑦𝑋subscriptπ‘Ž23\displaystyle|G(x,y)|_{X}\leq a_{21}|x|_{X}+a_{22}|y|_{X}+a_{23},| italic_G ( italic_x , italic_y ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ≀ italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT | italic_x | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT | italic_y | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 23 end_POSTSUBSCRIPT ,

for all x,y∈Xπ‘₯𝑦𝑋x,y\in Xitalic_x , italic_y ∈ italic_X and t∈[0,T]𝑑0𝑇t\in\left[0,T\right]italic_t ∈ [ 0 , italic_T ]. In addition, assume that {S⁒(t);tβ‰₯0}𝑆𝑑𝑑0\left\{S\left(t\right);t\geq 0\right\}{ italic_S ( italic_t ) ; italic_t β‰₯ 0 } is a compact semigroup and condition (ii) in Theorem 3.2 holds.

Then, for each β∈X,𝛽𝑋\beta\in X,italic_Ξ² ∈ italic_X , problem (3.1)-(3.2) has at least one solution (x,y)π‘₯𝑦\left(x,y\right)( italic_x , italic_y ) in C⁒([0,T];X)2𝐢superscript0𝑇𝑋2C\left(\left[0,T\right];X\right)^{2}italic_C ( [ 0 , italic_T ] ; italic_X ) start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT with y⁒(0)=Ξ².𝑦0𝛽y\left(0\right)=\beta.italic_y ( 0 ) = italic_Ξ² .

Proof.

We shall apply the Schauder’s fixed point theorem to the operator (N1,N2)subscript𝑁1subscript𝑁2(N_{1},N_{2})( italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ) on a closed convex bounded subset of X1Γ—X2subscript𝑋1subscript𝑋2X_{1}\times X_{2}italic_X start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_X start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT of the form

(4.9) DΞ²;R1,R2:={(x,y)∈C⁒([0,T];X)2:y⁒(0)=Ξ²,|x|0≀R1,|y|θ≀R2},assignsubscript𝐷𝛽subscript𝑅1subscript𝑅2conditional-setπ‘₯𝑦𝐢superscript0𝑇𝑋2formulae-sequence𝑦0𝛽formulae-sequencesubscriptπ‘₯0subscript𝑅1subscriptπ‘¦πœƒsubscript𝑅2D_{\beta;R_{1},R_{2}}:=\left\{(x,y)\in C([0,T];X)^{2}\,:\,y\left(0\right)=% \beta,\ |x|_{0}\leq R_{1},\,|y|_{\theta}\leq R_{2}\right\},italic_D start_POSTSUBSCRIPT italic_Ξ² ; italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT end_POSTSUBSCRIPT := { ( italic_x , italic_y ) ∈ italic_C ( [ 0 , italic_T ] ; italic_X ) start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT : italic_y ( 0 ) = italic_Ξ² , | italic_x | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT ≀ italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , | italic_y | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT ≀ italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT } ,

where the positive numbers R1,subscript𝑅1R_{1},italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , R2subscript𝑅2R_{2}italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT will be determined in a such way that the operator (N1,N2)subscript𝑁1subscript𝑁2(N_{1},N_{2})( italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ) is invariant over DΞ²;R1,R2subscript𝐷𝛽subscript𝑅1subscript𝑅2D_{\beta;R_{1},R_{2}}italic_D start_POSTSUBSCRIPT italic_Ξ² ; italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT end_POSTSUBSCRIPT, i.e.,

|N1⁒(x,y)|0≀R1,|N2⁒(x,y)|θ≀R2⁒ whenever β’|x|0≀R1,|y|θ≀R2.formulae-sequenceformulae-sequencesubscriptsubscript𝑁1π‘₯𝑦0subscript𝑅1subscriptsubscript𝑁2π‘₯π‘¦πœƒsubscript𝑅2 whenever subscriptπ‘₯0subscript𝑅1subscriptπ‘¦πœƒsubscript𝑅2\left|N_{1}(x,y)\right|_{0}\leq R_{1},\ \left|N_{2}(x,y)\right|_{\theta}\leq R% _{2}\text{ \ whenever\ }|x|_{0}\leq R_{1},\ \,|y|_{\theta}\leq R_{2}.| italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT ≀ italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , | italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT ≀ italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT whenever | italic_x | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT ≀ italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , | italic_y | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT ≀ italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT .

Let (x,y)∈DΞ²;R1,R2.π‘₯𝑦subscript𝐷𝛽subscript𝑅1subscript𝑅2(x,y)\in D_{\beta;R_{1},R_{2}}.( italic_x , italic_y ) ∈ italic_D start_POSTSUBSCRIPT italic_Ξ² ; italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT end_POSTSUBSCRIPT . Then, for all t∈[0,T]𝑑0𝑇t\in[0,T]italic_t ∈ [ 0 , italic_T ], we have

|N1⁒(x,y)⁒(t)|Xsubscriptsubscript𝑁1π‘₯𝑦𝑑𝑋\displaystyle\left|N_{1}(x,y)\left(t\right)\right|_{X}| italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) ( italic_t ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ≀1a⁒CA⁒|x|0+1a⁒CA⁒(1+b)⁒k⁒|Ξ²|Xabsent1π‘Žsubscript𝐢𝐴subscriptπ‘₯01π‘Žsubscript𝐢𝐴1π‘π‘˜subscript𝛽𝑋\displaystyle\leq\frac{1}{a}C_{A}|x|_{0}+\frac{1}{a}C_{A}\left(1+b\right)k% \left|\beta\right|_{X}≀ divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT | italic_x | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT + divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( 1 + italic_b ) italic_k | italic_Ξ² | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT
+CA⁒ka⁒∫0T(a21⁒|x⁒(s)|X+a22⁒|y⁒(s)|X+a23)⁒𝑑ssubscriptπΆπ΄π‘˜π‘Žsuperscriptsubscript0𝑇subscriptπ‘Ž21subscriptπ‘₯𝑠𝑋subscriptπ‘Ž22subscript𝑦𝑠𝑋subscriptπ‘Ž23differential-d𝑠\displaystyle+C_{A}\,\frac{k}{a}\int_{0}^{T}\left(a_{21}|x(s)|_{X}+a_{22}|y(s)% |_{X}+a_{23}\right)ds+ italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT divide start_ARG italic_k end_ARG start_ARG italic_a end_ARG ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT ( italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT | italic_x ( italic_s ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT | italic_y ( italic_s ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 23 end_POSTSUBSCRIPT ) italic_d italic_s
+CA⁒(1+1a)⁒∫0T(a11⁒|x⁒(s)|X+a12⁒|y⁒(s)|X+a13)⁒𝑑ssubscript𝐢𝐴11π‘Žsuperscriptsubscript0𝑇subscriptπ‘Ž11subscriptπ‘₯𝑠𝑋subscriptπ‘Ž12subscript𝑦𝑠𝑋subscriptπ‘Ž13differential-d𝑠\displaystyle+C_{A}\left(1+\frac{1}{a}\right)\int_{0}^{T}\left(a_{11}|x(s)|_{X% }+a_{12}|y(s)|_{X}+a_{13}\right)ds+ italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( 1 + divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ) ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT ( italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT | italic_x ( italic_s ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT | italic_y ( italic_s ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 13 end_POSTSUBSCRIPT ) italic_d italic_s
≀m11⁒|x|0+m12⁒∫0Teθ⁒s⁒eβˆ’ΞΈβ’s⁒|y⁒(s)|X+C1absentsubscriptπ‘š11subscriptπ‘₯0subscriptπ‘š12superscriptsubscript0𝑇superscriptπ‘’πœƒπ‘ superscriptπ‘’πœƒπ‘ subscript𝑦𝑠𝑋subscript𝐢1\displaystyle\leq m_{11}|x|_{0}+m_{12}\int_{0}^{T}e^{\theta s}e^{-\theta s}|y(% s)|_{X}+C_{1}≀ italic_m start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT | italic_x | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT + italic_m start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_T end_POSTSUPERSCRIPT italic_e start_POSTSUPERSCRIPT italic_ΞΈ italic_s end_POSTSUPERSCRIPT italic_e start_POSTSUPERSCRIPT - italic_ΞΈ italic_s end_POSTSUPERSCRIPT | italic_y ( italic_s ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_C start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT
≀m11⁒R1+m12⁒R2⁒eθ⁒Tβˆ’1ΞΈ+C1,absentsubscriptπ‘š11subscript𝑅1subscriptπ‘š12subscript𝑅2superscriptπ‘’πœƒπ‘‡1πœƒsubscript𝐢1\displaystyle\leq m_{11}R_{1}+m_{12}R_{2}\frac{e^{\theta T}-1}{\theta}+C_{1},≀ italic_m start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT + italic_m start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT divide start_ARG italic_e start_POSTSUPERSCRIPT italic_ΞΈ italic_T end_POSTSUPERSCRIPT - 1 end_ARG start_ARG italic_ΞΈ end_ARG + italic_C start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ,

where

m11=CA⁒(1a+(1+1a)⁒T⁒a11+ka⁒T⁒a21),m12=CA⁒((1+1a)⁒a12+ka⁒a22), formulae-sequencesubscriptπ‘š11subscript𝐢𝐴1π‘Ž11π‘Žπ‘‡subscriptπ‘Ž11π‘˜π‘Žπ‘‡subscriptπ‘Ž21subscriptπ‘š12subscript𝐢𝐴11π‘Žsubscriptπ‘Ž12π‘˜π‘Žsubscriptπ‘Ž22 m_{11}=C_{A}\left(\frac{1}{a}+\left(1+\frac{1}{a}\right)Ta_{11}+\frac{k}{a}Ta_% {21}\right),\ \ m_{12}=C_{A}\left(\left(1+\frac{1}{a}\right)a_{12}+\frac{k}{a}% a_{22}\right),\text{ }italic_m start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT = italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( divide start_ARG 1 end_ARG start_ARG italic_a end_ARG + ( 1 + divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ) italic_T italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT + divide start_ARG italic_k end_ARG start_ARG italic_a end_ARG italic_T italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT ) , italic_m start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT = italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( ( 1 + divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ) italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT + divide start_ARG italic_k end_ARG start_ARG italic_a end_ARG italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT ) ,

and

C1=1a⁒CA⁒(1+b)⁒k⁒|Ξ²|X+CA⁒ka⁒T⁒a23+CA⁒(1+1a)⁒a13.subscript𝐢11π‘Žsubscript𝐢𝐴1π‘π‘˜subscript𝛽𝑋subscriptπΆπ΄π‘˜π‘Žπ‘‡subscriptπ‘Ž23subscript𝐢𝐴11π‘Žsubscriptπ‘Ž13C_{1}=\frac{1}{a}C_{A}\left(1+b\right)k\left|\beta\right|_{X}+C_{A}\frac{k}{a}% Ta_{23}+C_{A}\left(1+\frac{1}{a}\right)a_{13}.italic_C start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT = divide start_ARG 1 end_ARG start_ARG italic_a end_ARG italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( 1 + italic_b ) italic_k | italic_Ξ² | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT divide start_ARG italic_k end_ARG start_ARG italic_a end_ARG italic_T italic_a start_POSTSUBSCRIPT 23 end_POSTSUBSCRIPT + italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ( 1 + divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ) italic_a start_POSTSUBSCRIPT 13 end_POSTSUBSCRIPT .

Hence,

(4.10) |N1⁒(x,y)|0≀m11⁒R1+m12⁒R2⁒eθ⁒Tβˆ’1ΞΈ+C1.subscriptsubscript𝑁1π‘₯𝑦0subscriptπ‘š11subscript𝑅1subscriptπ‘š12subscript𝑅2superscriptπ‘’πœƒπ‘‡1πœƒsubscript𝐢1\left|N_{1}(x,y)\right|_{0}\leq m_{11}R_{1}+m_{12}R_{2}\frac{e^{\theta T}-1}{% \theta}+C_{1}.| italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT ≀ italic_m start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT + italic_m start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT divide start_ARG italic_e start_POSTSUPERSCRIPT italic_ΞΈ italic_T end_POSTSUPERSCRIPT - 1 end_ARG start_ARG italic_ΞΈ end_ARG + italic_C start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT .

For the second operator N2subscript𝑁2N_{2}italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT, we compute

|N2⁒(x,y)⁒(t)|Xsubscriptsubscript𝑁2π‘₯𝑦𝑑𝑋\displaystyle\left|N_{2}(x,y)\left(t\right)\right|_{X}| italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) ( italic_t ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ≀CA⁒|Ξ²|X+CA⁒∫0t(a21⁒|x⁒(s)|X+a22⁒|y⁒(s)|X+a23)⁒𝑑sabsentsubscript𝐢𝐴subscript𝛽𝑋subscript𝐢𝐴superscriptsubscript0𝑑subscriptπ‘Ž21subscriptπ‘₯𝑠𝑋subscriptπ‘Ž22subscript𝑦𝑠𝑋subscriptπ‘Ž23differential-d𝑠\displaystyle\leq C_{A}\left|\beta\right|_{X}+C_{A}\int_{0}^{t}\left(a_{21}|x(% s)|_{X}+a_{22}|y(s)|_{X}+a_{23}\right)ds≀ italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT | italic_Ξ² | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_t end_POSTSUPERSCRIPT ( italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT | italic_x ( italic_s ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT | italic_y ( italic_s ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 23 end_POSTSUBSCRIPT ) italic_d italic_s
≀CA⁒T⁒a21⁒|x|0+a22⁒CA⁒∫0teθ⁒s⁒eβˆ’ΞΈβ’s⁒|y⁒(s)|X⁒𝑑s+C2absentsubscript𝐢𝐴𝑇subscriptπ‘Ž21subscriptπ‘₯0subscriptπ‘Ž22subscript𝐢𝐴superscriptsubscript0𝑑superscriptπ‘’πœƒπ‘ superscriptπ‘’πœƒπ‘ subscript𝑦𝑠𝑋differential-d𝑠subscript𝐢2\displaystyle\leq\,C_{A}\,Ta_{21}|x|_{0}+a_{22}C_{A}\int_{0}^{t}e^{\theta s}e^% {-\theta s}|y(s)|_{X}ds+C_{2}≀ italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT italic_T italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT | italic_x | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT ∫ start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_t end_POSTSUPERSCRIPT italic_e start_POSTSUPERSCRIPT italic_ΞΈ italic_s end_POSTSUPERSCRIPT italic_e start_POSTSUPERSCRIPT - italic_ΞΈ italic_s end_POSTSUPERSCRIPT | italic_y ( italic_s ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT italic_d italic_s + italic_C start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT
≀m21⁒|x|0+m22⁒|y|θ⁒eθ⁒tβˆ’1ΞΈ+C2,absentsubscriptπ‘š21subscriptπ‘₯0subscriptπ‘š22subscriptπ‘¦πœƒsuperscriptπ‘’πœƒπ‘‘1πœƒsubscript𝐢2\displaystyle\leq m_{21}|x|_{0}+m_{22}|y|_{\theta}\frac{e^{\theta t}-1}{\theta% }+C_{2},≀ italic_m start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT | italic_x | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT + italic_m start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT | italic_y | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT divide start_ARG italic_e start_POSTSUPERSCRIPT italic_ΞΈ italic_t end_POSTSUPERSCRIPT - 1 end_ARG start_ARG italic_ΞΈ end_ARG + italic_C start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ,

where m21=CA⁒T⁒a21subscriptπ‘š21subscript𝐢𝐴𝑇subscriptπ‘Ž21m_{21}=\,C_{A}\,Ta_{21}italic_m start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT = italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT italic_T italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT, m22=CA⁒a22subscriptπ‘š22subscript𝐢𝐴subscriptπ‘Ž22m_{22}=C_{A}a_{22}italic_m start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT = italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT and C2=CA⁒|Ξ²|X+CA⁒T⁒a23.subscript𝐢2subscript𝐢𝐴subscript𝛽𝑋subscript𝐢𝐴𝑇subscriptπ‘Ž23C_{2}=C_{A}\left|\beta\right|_{X}+C_{A}Ta_{23}.italic_C start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT = italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT | italic_Ξ² | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT italic_T italic_a start_POSTSUBSCRIPT 23 end_POSTSUBSCRIPT . Dividing by eθ⁒tsuperscriptπ‘’πœƒπ‘‘e^{\theta t}italic_e start_POSTSUPERSCRIPT italic_ΞΈ italic_t end_POSTSUPERSCRIPT and taking the supremum over t∈[0,T]𝑑0𝑇t\in[0,T]italic_t ∈ [ 0 , italic_T ], we obtain

(4.11) |N2⁒(x,y)|θ≀m21⁒R1+m22⁒1βˆ’eβˆ’ΞΈβ’Tθ⁒R2+C2.subscriptsubscript𝑁2π‘₯π‘¦πœƒsubscriptπ‘š21subscript𝑅1subscriptπ‘š221superscriptπ‘’πœƒπ‘‡πœƒsubscript𝑅2subscript𝐢2\left|N_{2}(x,y)\right|_{\theta}\leq m_{21}R_{1}+m_{22}\frac{1-e^{-\theta T}}{% \theta}R_{2}+C_{2}.| italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT ≀ italic_m start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT + italic_m start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT divide start_ARG 1 - italic_e start_POSTSUPERSCRIPT - italic_ΞΈ italic_T end_POSTSUPERSCRIPT end_ARG start_ARG italic_ΞΈ end_ARG italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT + italic_C start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT .

In the matrix form, relations (4.10) and (4.11) read as

[|N1⁒(x,y)|0|N2⁒(x,y)|ΞΈ]≀M⁒(ΞΈ)⁒[R1R2]+[C1C2],matrixsubscriptsubscript𝑁1π‘₯𝑦0subscriptsubscript𝑁2π‘₯π‘¦πœƒπ‘€πœƒmatrixsubscript𝑅1subscript𝑅2matrixsubscript𝐢1subscript𝐢2\begin{bmatrix}\left|N_{1}(x,y)\right|_{0}\\ \left|N_{2}(x,y)\right|_{\theta}\end{bmatrix}\leq M(\theta)\begin{bmatrix}R_{1% }\\ R_{2}\end{bmatrix}+\begin{bmatrix}C_{1}\\ C_{2}\end{bmatrix},[ start_ARG start_ROW start_CELL | italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL | italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT end_CELL end_ROW end_ARG ] ≀ italic_M ( italic_ΞΈ ) [ start_ARG start_ROW start_CELL italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT end_CELL end_ROW end_ARG ] + [ start_ARG start_ROW start_CELL italic_C start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL italic_C start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT end_CELL end_ROW end_ARG ] ,

where M⁒(ΞΈ)π‘€πœƒM(\theta)italic_M ( italic_ΞΈ ) is given in (3.8). For the invariance condition it suffices to have

M⁒(ΞΈ)⁒[R1R2]+[C1C2]≀[R1R2],π‘€πœƒmatrixsubscript𝑅1subscript𝑅2matrixsubscript𝐢1subscript𝐢2matrixsubscript𝑅1subscript𝑅2M(\theta)\begin{bmatrix}R_{1}\\ R_{2}\end{bmatrix}+\begin{bmatrix}C_{1}\\ C_{2}\end{bmatrix}\leq\begin{bmatrix}R_{1}\\ R_{2}\end{bmatrix},italic_M ( italic_ΞΈ ) [ start_ARG start_ROW start_CELL italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT end_CELL end_ROW end_ARG ] + [ start_ARG start_ROW start_CELL italic_C start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL italic_C start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT end_CELL end_ROW end_ARG ] ≀ [ start_ARG start_ROW start_CELL italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT end_CELL end_ROW end_ARG ] ,

or equivalently

[C1C2]≀(Iβˆ’M⁒(ΞΈ))⁒[R1R2].matrixsubscript𝐢1subscript𝐢2πΌπ‘€πœƒmatrixsubscript𝑅1subscript𝑅2\begin{bmatrix}C_{1}\\ C_{2}\end{bmatrix}\leq\left(I-M\left(\theta\right)\right)\begin{bmatrix}R_{1}% \\ R_{2}\end{bmatrix}.[ start_ARG start_ROW start_CELL italic_C start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL italic_C start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT end_CELL end_ROW end_ARG ] ≀ ( italic_I - italic_M ( italic_ΞΈ ) ) [ start_ARG start_ROW start_CELL italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT end_CELL end_ROW end_ARG ] .

From assumption (ii), since the matrix M⁒(ΞΈ)π‘€πœƒM(\theta)italic_M ( italic_ΞΈ ) is convergent to zero, (Iβˆ’M⁒(ΞΈ))βˆ’1superscriptπΌπ‘€πœƒ1(I-M(\theta))^{-1}( italic_I - italic_M ( italic_ΞΈ ) ) start_POSTSUPERSCRIPT - 1 end_POSTSUPERSCRIPT has nonnegative entries. Therefore, the last inequality is equivalent to

(4.12) (Iβˆ’M⁒(ΞΈ))βˆ’1⁒[C1C2]≀[R1R2],superscriptπΌπ‘€πœƒ1matrixsubscript𝐢1subscript𝐢2matrixsubscript𝑅1subscript𝑅2(I-M(\theta))^{-1}\begin{bmatrix}C_{1}\\ C_{2}\end{bmatrix}\leq\begin{bmatrix}R_{1}\\ R_{2}\end{bmatrix},( italic_I - italic_M ( italic_ΞΈ ) ) start_POSTSUPERSCRIPT - 1 end_POSTSUPERSCRIPT [ start_ARG start_ROW start_CELL italic_C start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL italic_C start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT end_CELL end_ROW end_ARG ] ≀ [ start_ARG start_ROW start_CELL italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT end_CELL end_ROW start_ROW start_CELL italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT end_CELL end_ROW end_ARG ] ,

which clearly allows us to choose positive numbers R1,R2subscript𝑅1subscript𝑅2R_{1},R_{2}italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT such that the set DΞ²;R1,R2subscript𝐷𝛽subscript𝑅1subscript𝑅2D_{\beta;R_{1},R_{2}}italic_D start_POSTSUBSCRIPT italic_Ξ² ; italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT end_POSTSUBSCRIPT is invariant under the operator (N1,N2).subscript𝑁1subscript𝑁2(N_{1},N_{2}).( italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ) .

Note that, as the semigroup generated by A𝐴Aitalic_A is assumed to be compact, it follows from standard arguments that N1subscript𝑁1N_{1}italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT and N2subscript𝑁2N_{2}italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT are completely continuous operators (see, e.g., [13]). Consequently, Schauder’s fixed point theorem applies and guarantees the existence of at least one fixed point of (N1,N2)subscript𝑁1subscript𝑁2(N_{1},N_{2})( italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ) in DΞ²;R1,R2subscript𝐷𝛽subscript𝑅1subscript𝑅2D_{\beta;R_{1},R_{2}}italic_D start_POSTSUBSCRIPT italic_Ξ² ; italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT end_POSTSUBSCRIPT. ∎

Remark 4.4.

From the above result we have not only the existence of a solution, but also its localization, namely

(4.13) |x⁒(t)|X≀R1 and β’|y⁒(t)|X≀eθ⁒t⁒R2for all β’t∈[0,T],formulae-sequencesubscriptπ‘₯𝑑𝑋subscript𝑅1formulae-sequence and subscript𝑦𝑑𝑋superscriptπ‘’πœƒπ‘‘subscript𝑅2for all π‘‘0𝑇|x(t)|_{X}\leq R_{1}\ \ \ \text{ and\ \ \ }|y(t)|_{X}\leq e^{\theta t}R_{2}\ % \ \text{for all }t\in[0,T],| italic_x ( italic_t ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ≀ italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT and | italic_y ( italic_t ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ≀ italic_e start_POSTSUPERSCRIPT italic_ΞΈ italic_t end_POSTSUPERSCRIPT italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT for all italic_t ∈ [ 0 , italic_T ] ,

where ΞΈπœƒ\thetaitalic_ΞΈ is given in assumption (ii), and R1,R2subscript𝑅1subscript𝑅2R_{1},R_{2}italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT satisfy (4.12). Note that, due to the use of the Bielecki norm on the second component, we only have an exponential localization for y𝑦yitalic_y.

4.4. Existence via Avramescu’s fixed point theorem

We apply Avramescu’s fixed point theorem to obtain a fixed point for the operator (N1,N2)subscript𝑁1subscript𝑁2(N_{1},N_{2})( italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ). It is noteworthy that, given the fixed point obtained in Theorem 4.5 below, the uniqueness of the second component is guaranteed by Banach’s principle, while both components xπ‘₯xitalic_x and y𝑦yitalic_y satisfy (4.13) with ΞΈπœƒ\thetaitalic_ΞΈ given in assumption (ii) of Theorem 4.2, and R1,R2subscript𝑅1subscript𝑅2R_{1},R_{2}italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT satisfy (4.12).

Theorem 4.5.

Assume that there are nonnegative constants a11,a12,a13,a21,a22subscriptπ‘Ž11subscriptπ‘Ž12subscriptπ‘Ž13subscriptπ‘Ž21subscriptπ‘Ž22a_{11},a_{12},a_{13},a_{21},a_{22}italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT , italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT , italic_a start_POSTSUBSCRIPT 13 end_POSTSUBSCRIPT , italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT , italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT such that

(4.14) |F⁒(x,y)|X≀a11⁒|x|X+a12⁒|y|X+a13,subscript𝐹π‘₯𝑦𝑋subscriptπ‘Ž11subscriptπ‘₯𝑋subscriptπ‘Ž12subscript𝑦𝑋subscriptπ‘Ž13\displaystyle|F(x,y)|_{X}\leq a_{11}|x|_{X}+a_{12}|y|_{X}+a_{13},| italic_F ( italic_x , italic_y ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ≀ italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT | italic_x | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT | italic_y | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 13 end_POSTSUBSCRIPT ,
|G⁒(x,y)βˆ’G⁒(xΒ―,yΒ―)|X≀a21⁒|xβˆ’xΒ―|X+a22⁒|yβˆ’yΒ―|X,subscript𝐺π‘₯𝑦𝐺¯π‘₯¯𝑦𝑋subscriptπ‘Ž21subscriptπ‘₯Β―π‘₯𝑋subscriptπ‘Ž22subscript𝑦¯𝑦𝑋\displaystyle|G(x,y)-G(\overline{x},\overline{y})|_{X}\leq a_{21}|x-\overline{% x}|_{X}+a_{22}|y-\overline{y}|_{X},| italic_G ( italic_x , italic_y ) - italic_G ( overΒ― start_ARG italic_x end_ARG , overΒ― start_ARG italic_y end_ARG ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ≀ italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT | italic_x - overΒ― start_ARG italic_x end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT | italic_y - overΒ― start_ARG italic_y end_ARG | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ,

for all x,xΒ―,y,y¯∈Xπ‘₯Β―π‘₯𝑦¯𝑦𝑋x,\overline{x},y,\overline{y}\in Xitalic_x , overΒ― start_ARG italic_x end_ARG , italic_y , overΒ― start_ARG italic_y end_ARG ∈ italic_X and t∈[0,T].𝑑0𝑇t\in\left[0,T\right].italic_t ∈ [ 0 , italic_T ] . In addition assume that {S⁒(t);tβ‰₯0}𝑆𝑑𝑑0\left\{S\left(t\right);t\geq 0\right\}{ italic_S ( italic_t ) ; italic_t β‰₯ 0 } is a compact semigroup and condition (ii) in Theorem 4.2 holds.

Then, for each β∈X,𝛽𝑋\beta\in X,italic_Ξ² ∈ italic_X , problem (3.1)-(3.2) has at least one solution (x,y)π‘₯𝑦\left(x,y\right)( italic_x , italic_y ) in C⁒([0,T];X)2𝐢superscript0𝑇𝑋2C\left(\left[0,T\right];X\right)^{2}italic_C ( [ 0 , italic_T ] ; italic_X ) start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT with y⁒(0)=Ξ².𝑦0𝛽y\left(0\right)=\beta.italic_y ( 0 ) = italic_Ξ² .

Proof.

Let us consider the sets,

D1:={x∈C⁒([0,T];X):|x|0≀R1},assignsubscript𝐷1conditional-setπ‘₯𝐢0𝑇𝑋subscriptπ‘₯0subscript𝑅1\displaystyle D_{1}:=\left\{x\in C([0,T];X)\,:\,|x|_{0}\leq R_{1}\right\},italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT := { italic_x ∈ italic_C ( [ 0 , italic_T ] ; italic_X ) : | italic_x | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT ≀ italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT } ,
D2:={y∈C⁒([0,T];X):y⁒(0)=Ξ²,|y|θ≀R1},assignsubscript𝐷2conditional-set𝑦𝐢0𝑇𝑋formulae-sequence𝑦0𝛽subscriptπ‘¦πœƒsubscript𝑅1\displaystyle D_{2}:=\left\{y\in C([0,T];X)\,:\,y\left(0\right)=\beta,\ |y|_{% \theta}\leq R_{1}\right\},italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT := { italic_y ∈ italic_C ( [ 0 , italic_T ] ; italic_X ) : italic_y ( 0 ) = italic_Ξ² , | italic_y | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT ≀ italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT } ,

where R1,R2subscript𝑅1subscript𝑅2R_{1},R_{2}italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT are positive numbers which are chosen below. We observe that, from (4.14), function G𝐺Gitalic_G satisfies the growth condition

|G⁒(x,y)|X≀a21⁒|x|X+a22⁒|y|X+a23,subscript𝐺π‘₯𝑦𝑋subscriptπ‘Ž21subscriptπ‘₯𝑋subscriptπ‘Ž22subscript𝑦𝑋subscriptπ‘Ž23|G(x,y)|_{X}\leq a_{21}|x|_{X}+a_{22}|y|_{X}+a_{23},| italic_G ( italic_x , italic_y ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT ≀ italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT | italic_x | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT | italic_y | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT + italic_a start_POSTSUBSCRIPT 23 end_POSTSUBSCRIPT ,

where a23=|G⁒(0,0)|X.subscriptπ‘Ž23subscript𝐺00𝑋a_{23}=\left|G\left(0,0\right)\right|_{X}.italic_a start_POSTSUBSCRIPT 23 end_POSTSUBSCRIPT = | italic_G ( 0 , 0 ) | start_POSTSUBSCRIPT italic_X end_POSTSUBSCRIPT . Consequently, performing the same estimates as in the proof of Theorem 4.3 and using (ii), we conclude that

|N1⁒(x,y)|0≀R1,|N2⁒(x,y)|θ≀R2,formulae-sequencesubscriptsubscript𝑁1π‘₯𝑦0subscript𝑅1subscriptsubscript𝑁2π‘₯π‘¦πœƒsubscript𝑅2\left|N_{1}(x,y)\right|_{0}\leq R_{1},\ \ \ \left|N_{2}(x,y)\right|_{\theta}% \leq R_{2},| italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) | start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT ≀ italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , | italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT ≀ italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ,

for all (x,y)∈D1Γ—D2π‘₯𝑦subscript𝐷1subscript𝐷2(x,y)\in D_{1}\times D_{2}( italic_x , italic_y ) ∈ italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT, where R1,R2subscript𝑅1subscript𝑅2R_{1},R_{2}italic_R start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT , italic_R start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT are obtained as in the proof of the previous theorem. This guarantees that Ni⁒(D1Γ—D2)βŠ‚Disubscript𝑁𝑖subscript𝐷1subscript𝐷2subscript𝐷𝑖N_{i}\left(D_{1}\times D_{2}\right)\subset D_{i}italic_N start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT ( italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ) βŠ‚ italic_D start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT for i=1,2.𝑖12i=1,2.italic_i = 1 , 2 .

Since the matrix M⁒(ΞΈ)π‘€πœƒM(\theta)italic_M ( italic_ΞΈ ) converges to zero, the diagonal elements are strictly less than 1111, hence

a22⁒CA⁒1βˆ’eβˆ’ΞΈβ’TΞΈ<1.subscriptπ‘Ž22subscript𝐢𝐴1superscriptπ‘’πœƒπ‘‡πœƒ1\ a_{22}C_{A}\frac{1-e^{-\theta T}}{\theta}<1.italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT divide start_ARG 1 - italic_e start_POSTSUPERSCRIPT - italic_ΞΈ italic_T end_POSTSUPERSCRIPT end_ARG start_ARG italic_ΞΈ end_ARG < 1 .

This guarantees that N2⁒(x,β‹…)subscript𝑁2π‘₯β‹…N_{2}(x,\cdot)italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , β‹… ) is a contraction for all x∈C⁒([0,T];X)π‘₯𝐢0𝑇𝑋x\in C([0,T];X)italic_x ∈ italic_C ( [ 0 , italic_T ] ; italic_X ). Indeed, following a similar reasoning as in the proof of Theorem 4.2, we deduce

|N2⁒(x,y)βˆ’N2⁒(x,yΒ―)|θ≀a22⁒CA⁒1βˆ’eβˆ’ΞΈβ’Tθ⁒|yβˆ’yΒ―|ΞΈ,subscriptsubscript𝑁2π‘₯𝑦subscript𝑁2π‘₯Β―π‘¦πœƒsubscriptπ‘Ž22subscript𝐢𝐴1superscriptπ‘’πœƒπ‘‡πœƒsubscriptπ‘¦Β―π‘¦πœƒ\left|N_{2}(x,y)-N_{2}(x,\overline{y})\right|_{\theta}\leq a_{22}C_{A}\frac{1-% e^{-\theta T}}{\theta}|y-\overline{y}|_{\theta},| italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) - italic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , overΒ― start_ARG italic_y end_ARG ) | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT ≀ italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT divide start_ARG 1 - italic_e start_POSTSUPERSCRIPT - italic_ΞΈ italic_T end_POSTSUPERSCRIPT end_ARG start_ARG italic_ΞΈ end_ARG | italic_y - overΒ― start_ARG italic_y end_ARG | start_POSTSUBSCRIPT italic_ΞΈ end_POSTSUBSCRIPT ,

for all x∈D1π‘₯subscript𝐷1x\in D_{1}italic_x ∈ italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT and y,y¯∈D2𝑦¯𝑦subscript𝐷2y,\overline{y}\in D_{2}italic_y , overΒ― start_ARG italic_y end_ARG ∈ italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT. In addition, as above, N1⁒(D1Γ—D2)subscript𝑁1subscript𝐷1subscript𝐷2N_{1}\left(D_{1}\times D_{2}\right)italic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ) is relatively compact in C⁒([0,T];X).𝐢0𝑇𝑋C\left(\left[0,T\right];X\right).italic_C ( [ 0 , italic_T ] ; italic_X ) . Therefore, Avramescu’s theorem applies and guarantees the existence of a pair (x,y)∈D1Γ—D2π‘₯𝑦subscript𝐷1subscript𝐷2(x,y)\in D_{1}\times D_{2}( italic_x , italic_y ) ∈ italic_D start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT Γ— italic_D start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT such that N1⁒(x,y)=xsubscript𝑁1π‘₯𝑦π‘₯N_{1}(x,y)=xitalic_N start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( italic_x , italic_y ) = italic_x and N2⁒(x,y)=ysubscript𝑁2π‘₯𝑦𝑦N_{2}(x,y)=yitalic_N start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ( italic_x , italic_y ) = italic_y. ∎

5. Application

The results established in Section 4 can be easily applied to the diffusion system,

(5.1) {ut=Δ⁒u+f⁒(u,v)vt=Δ⁒v+g⁒(u,v)⁒ in β’Ξ©,u=v=0⁒ on β’βˆ‚Ξ©β’(t∈[0,T]),casessubscript𝑒𝑑Δ𝑒𝑓𝑒𝑣otherwisesubscript𝑣𝑑Δ𝑣𝑔𝑒𝑣 in Ξ©otherwise𝑒𝑣0 on Ξ©otherwise𝑑0𝑇\begin{cases}u_{t}=\Delta u+f(u,v)\\ v_{t}=\Delta v+g(u,v)\,\text{ in }\Omega,\\ u=v=0\,\text{ on }\partial\Omega\end{cases}(t\in[0,T]),{ start_ROW start_CELL italic_u start_POSTSUBSCRIPT italic_t end_POSTSUBSCRIPT = roman_Ξ” italic_u + italic_f ( italic_u , italic_v ) end_CELL start_CELL end_CELL end_ROW start_ROW start_CELL italic_v start_POSTSUBSCRIPT italic_t end_POSTSUBSCRIPT = roman_Ξ” italic_v + italic_g ( italic_u , italic_v ) in roman_Ξ© , end_CELL start_CELL end_CELL end_ROW start_ROW start_CELL italic_u = italic_v = 0 on βˆ‚ roman_Ξ© end_CELL start_CELL end_CELL end_ROW ( italic_t ∈ [ 0 , italic_T ] ) ,

with the controllability condition

(5.2) u⁒(T)βˆ’a⁒u⁒(0)=k⁒(v⁒(T)βˆ’b⁒v⁒(0)),π‘’π‘‡π‘Žπ‘’0π‘˜π‘£π‘‡π‘π‘£0u(T)-au\left(0\right)=k\left(v(T)-bv\left(0\right)\right),italic_u ( italic_T ) - italic_a italic_u ( 0 ) = italic_k ( italic_v ( italic_T ) - italic_b italic_v ( 0 ) ) ,

where a,b,k>0.π‘Žπ‘π‘˜0a,b,k>0.italic_a , italic_b , italic_k > 0 .

The functions f,g:ℝ2→ℝ:𝑓𝑔→superscriptℝ2ℝf,g\colon\mathbb{R}^{2}\rightarrow\mathbb{R}italic_f , italic_g : blackboard_R start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT β†’ blackboard_R are assumed to be continuous, and there exist nonnegative constants a11,a12,a21,a22,cf,cgsubscriptπ‘Ž11subscriptπ‘Ž12subscriptπ‘Ž21subscriptπ‘Ž22subscript𝑐𝑓subscript𝑐𝑔a_{11},a_{12},a_{21},a_{22},c_{f},c_{g}italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT , italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT , italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT , italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT , italic_c start_POSTSUBSCRIPT italic_f end_POSTSUBSCRIPT , italic_c start_POSTSUBSCRIPT italic_g end_POSTSUBSCRIPT such that one of the following three conditions is satisfied:

(c1):{|f⁒(p,q)βˆ’f⁒(pΒ―,qΒ―)|≀a11⁒|pβˆ’pΒ―|+a12⁒|qβˆ’qΒ―||g⁒(p,q)βˆ’g⁒(pΒ―,qΒ―)|≀a21⁒|pβˆ’pΒ―|+a22⁒|qβˆ’qΒ―|:subscriptc1casesπ‘“π‘π‘žπ‘“Β―π‘Β―π‘žsubscriptπ‘Ž11𝑝¯𝑝subscriptπ‘Ž12π‘žΒ―π‘žotherwiseπ‘”π‘π‘žπ‘”Β―π‘Β―π‘žsubscriptπ‘Ž21𝑝¯𝑝subscriptπ‘Ž22π‘žΒ―π‘žotherwise\displaystyle(\text{c}_{1}):\begin{cases}\left|f(p,q)-f(\overline{p},\overline% {q})\right|\leq a_{11}|p-\overline{p}|+a_{12}|q-\overline{q}|\\ \left|g(p,q)-g(\overline{p},\overline{q})\right|\leq a_{21}|p-\overline{p}|+a_% {22}|q-\overline{q}|\end{cases}( c start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ) : { start_ROW start_CELL | italic_f ( italic_p , italic_q ) - italic_f ( overΒ― start_ARG italic_p end_ARG , overΒ― start_ARG italic_q end_ARG ) | ≀ italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT | italic_p - overΒ― start_ARG italic_p end_ARG | + italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT | italic_q - overΒ― start_ARG italic_q end_ARG | end_CELL start_CELL end_CELL end_ROW start_ROW start_CELL | italic_g ( italic_p , italic_q ) - italic_g ( overΒ― start_ARG italic_p end_ARG , overΒ― start_ARG italic_q end_ARG ) | ≀ italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT | italic_p - overΒ― start_ARG italic_p end_ARG | + italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT | italic_q - overΒ― start_ARG italic_q end_ARG | end_CELL start_CELL end_CELL end_ROW
(c2):{|f⁒(p,q)|≀a11⁒|p|+a12⁒|q|+cf|g⁒(p,q)|≀a21⁒|p|+a22⁒|q|+cg:subscriptc2casesπ‘“π‘π‘žsubscriptπ‘Ž11𝑝subscriptπ‘Ž12π‘žsubscript𝑐𝑓otherwiseπ‘”π‘π‘žsubscriptπ‘Ž21𝑝subscriptπ‘Ž22π‘žsubscript𝑐𝑔otherwise\displaystyle(\text{c}_{2}):\begin{cases}\left|f(p,q)\right|\leq a_{11}|p|+a_{% 12}|q|+c_{f}\\ \left|g(p,q)\right|\leq a_{21}|p|+a_{22}|q|+c_{g}\end{cases}( c start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ) : { start_ROW start_CELL | italic_f ( italic_p , italic_q ) | ≀ italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT | italic_p | + italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT | italic_q | + italic_c start_POSTSUBSCRIPT italic_f end_POSTSUBSCRIPT end_CELL start_CELL end_CELL end_ROW start_ROW start_CELL | italic_g ( italic_p , italic_q ) | ≀ italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT | italic_p | + italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT | italic_q | + italic_c start_POSTSUBSCRIPT italic_g end_POSTSUBSCRIPT end_CELL start_CELL end_CELL end_ROW
(c3):{|f⁒(p,q)|≀a11⁒|p|+a12⁒|q|+cf|g⁒(p,q)βˆ’g⁒(pΒ―,qΒ―)|≀a21⁒|pβˆ’pΒ―|+a22⁒|qβˆ’qΒ―|:subscriptc3casesπ‘“π‘π‘žsubscriptπ‘Ž11𝑝subscriptπ‘Ž12π‘žsubscript𝑐𝑓otherwiseπ‘”π‘π‘žπ‘”Β―π‘Β―π‘žsubscriptπ‘Ž21𝑝¯𝑝subscriptπ‘Ž22π‘žΒ―π‘žotherwise\displaystyle(\text{c}_{3}):\begin{cases}\left|f(p,q)\right|\leq a_{11}|p|+a_{% 12}|q|+c_{f}\\ \left|g(p,q)-g(\overline{p},\overline{q})\right|\leq a_{21}|p-\overline{p}|+a_% {22}|q-\overline{q}|\end{cases}( c start_POSTSUBSCRIPT 3 end_POSTSUBSCRIPT ) : { start_ROW start_CELL | italic_f ( italic_p , italic_q ) | ≀ italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT | italic_p | + italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT | italic_q | + italic_c start_POSTSUBSCRIPT italic_f end_POSTSUBSCRIPT end_CELL start_CELL end_CELL end_ROW start_ROW start_CELL | italic_g ( italic_p , italic_q ) - italic_g ( overΒ― start_ARG italic_p end_ARG , overΒ― start_ARG italic_q end_ARG ) | ≀ italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT | italic_p - overΒ― start_ARG italic_p end_ARG | + italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT | italic_q - overΒ― start_ARG italic_q end_ARG | end_CELL start_CELL end_CELL end_ROW

for all p,q,pΒ―,qΒ―βˆˆβ„π‘π‘žΒ―π‘Β―π‘žβ„p,q,\overline{p},\overline{q}\in\mathbb{R}italic_p , italic_q , overΒ― start_ARG italic_p end_ARG , overΒ― start_ARG italic_q end_ARG ∈ blackboard_R.

Here, Ξ©βŠ‚β„nΞ©superscriptℝ𝑛\Omega\subset\mathbb{R}^{n}roman_Ξ© βŠ‚ blackboard_R start_POSTSUPERSCRIPT italic_n end_POSTSUPERSCRIPT is a bounded open set, X𝑋Xitalic_X is the Banach space L2⁒(Ξ©)superscript𝐿2Ξ©L^{2}(\Omega)italic_L start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT ( roman_Ξ© ) endowed with the usual |β‹…|L2|\cdot|_{L^{2}}| β‹… | start_POSTSUBSCRIPT italic_L start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT end_POSTSUBSCRIPT norm, A=Δ𝐴ΔA=\Deltaitalic_A = roman_Ξ”, with

D⁒(A)={u∈H01⁒(Ξ©):Δ⁒u∈L2⁒(Ξ©)}.𝐷𝐴conditional-set𝑒superscriptsubscript𝐻01ΩΔ𝑒superscript𝐿2Ξ©D(A)=\left\{u\in H_{0}^{1}(\Omega)\,:\,\Delta u\in L^{2}(\Omega)\right\}.italic_D ( italic_A ) = { italic_u ∈ italic_H start_POSTSUBSCRIPT 0 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT 1 end_POSTSUPERSCRIPT ( roman_Ξ© ) : roman_Ξ” italic_u ∈ italic_L start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT ( roman_Ξ© ) } .

Note that A𝐴Aitalic_A is the infinitesimal generator of a compact semigroup of contractions in L2⁒(Ξ©)superscript𝐿2Ξ©L^{2}(\Omega)italic_L start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT ( roman_Ξ© ) (cf, [20, Theorem 7.2.5]). Hence, the constant CAsubscript𝐢𝐴C_{A}italic_C start_POSTSUBSCRIPT italic_A end_POSTSUBSCRIPT given in (2.1) is 1.11.1 . Also F𝐹Fitalic_F and G𝐺Gitalic_G are the superposition operators F,G:L2⁒(Ξ©)2β†’L2⁒(Ξ©),:𝐹𝐺→superscript𝐿2superscriptΞ©2superscript𝐿2Ξ©\ F,G:L^{2}\left(\Omega\right)^{2}\rightarrow L^{2}\left(\Omega\right),italic_F , italic_G : italic_L start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT ( roman_Ξ© ) start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT β†’ italic_L start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT ( roman_Ξ© ) ,

F⁒(u,v)⁒(x)=f⁒(u⁒(x),v⁒(x)),G⁒(u,v)⁒(x)=g⁒(u⁒(x),v⁒(x))(x∈Ω).formulae-sequence𝐹𝑒𝑣π‘₯𝑓𝑒π‘₯𝑣π‘₯𝐺𝑒𝑣π‘₯𝑔𝑒π‘₯𝑣π‘₯π‘₯Ξ©F\left(u,v\right)\left(x\right)=f\left(u\left(x\right),v\left(x\right)\right),% \ \ \ G\left(u,v\right)\left(x\right)=g\left(u\left(x\right),v\left(x\right)% \right)\ \ \ \left(x\in\Omega\right).italic_F ( italic_u , italic_v ) ( italic_x ) = italic_f ( italic_u ( italic_x ) , italic_v ( italic_x ) ) , italic_G ( italic_u , italic_v ) ( italic_x ) = italic_g ( italic_u ( italic_x ) , italic_v ( italic_x ) ) ( italic_x ∈ roman_Ξ© ) .

Simple computations show that if either ((((c)1{}_{1})start_FLOATSUBSCRIPT 1 end_FLOATSUBSCRIPT ), ((((c)2{}_{2})start_FLOATSUBSCRIPT 2 end_FLOATSUBSCRIPT ), or ((((c)3{}_{3})start_FLOATSUBSCRIPT 3 end_FLOATSUBSCRIPT ) holds, then assumption (i) of Theorem 4.2, Theorem 4.3, or Theorem 4.5 is satisfied with a13=cf⁒m⁒(Ξ©)1/2,a23=cg⁒m⁒(Ξ©)1/2formulae-sequencesubscriptπ‘Ž13subscriptπ‘π‘“π‘šsuperscriptΞ©12subscriptπ‘Ž23subscriptπ‘π‘”π‘šsuperscriptΞ©12a_{13}=c_{f}m(\Omega)^{1/2},\ a_{23}=c_{g}m(\Omega)^{1/2}italic_a start_POSTSUBSCRIPT 13 end_POSTSUBSCRIPT = italic_c start_POSTSUBSCRIPT italic_f end_POSTSUBSCRIPT italic_m ( roman_Ξ© ) start_POSTSUPERSCRIPT 1 / 2 end_POSTSUPERSCRIPT , italic_a start_POSTSUBSCRIPT 23 end_POSTSUBSCRIPT = italic_c start_POSTSUBSCRIPT italic_g end_POSTSUBSCRIPT italic_m ( roman_Ξ© ) start_POSTSUPERSCRIPT 1 / 2 end_POSTSUPERSCRIPT and the constants a11,a12,a21,a22subscriptπ‘Ž11subscriptπ‘Ž12subscriptπ‘Ž21subscriptπ‘Ž22a_{11},a_{12},a_{21},a_{22}italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT , italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT , italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT , italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT.

Additionally, if we assume there exists ΞΈβ‰₯0πœƒ0\theta\geq 0italic_ΞΈ β‰₯ 0 such that the matrix

M⁒(ΞΈ):=[1a+(1+1a)⁒T⁒a11+ka⁒T⁒a21((1+1a)⁒a12+ka⁒a22)⁒eθ⁒Tβˆ’1ΞΈT⁒a21a22⁒1βˆ’eβˆ’ΞΈβ’TΞΈ]assignπ‘€πœƒmatrix1π‘Ž11π‘Žπ‘‡subscriptπ‘Ž11π‘˜π‘Žπ‘‡subscriptπ‘Ž2111π‘Žsubscriptπ‘Ž12π‘˜π‘Žsubscriptπ‘Ž22superscriptπ‘’πœƒπ‘‡1πœƒπ‘‡subscriptπ‘Ž21subscriptπ‘Ž221superscriptπ‘’πœƒπ‘‡πœƒM(\theta):=\begin{bmatrix}\frac{1}{a}+\left(1+\frac{1}{a}\right)Ta_{11}+\frac{% k}{a}Ta_{21}&\left(\left(1+\frac{1}{a}\right)a_{12}+\frac{k}{a}a_{22}\right)% \frac{e^{\theta T}-1}{\theta}\\[3.0pt] Ta_{21}&a_{22}\,\frac{1-e^{-\theta T}}{\theta}\end{bmatrix}italic_M ( italic_ΞΈ ) := [ start_ARG start_ROW start_CELL divide start_ARG 1 end_ARG start_ARG italic_a end_ARG + ( 1 + divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ) italic_T italic_a start_POSTSUBSCRIPT 11 end_POSTSUBSCRIPT + divide start_ARG italic_k end_ARG start_ARG italic_a end_ARG italic_T italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT end_CELL start_CELL ( ( 1 + divide start_ARG 1 end_ARG start_ARG italic_a end_ARG ) italic_a start_POSTSUBSCRIPT 12 end_POSTSUBSCRIPT + divide start_ARG italic_k end_ARG start_ARG italic_a end_ARG italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT ) divide start_ARG italic_e start_POSTSUPERSCRIPT italic_ΞΈ italic_T end_POSTSUPERSCRIPT - 1 end_ARG start_ARG italic_ΞΈ end_ARG end_CELL end_ROW start_ROW start_CELL italic_T italic_a start_POSTSUBSCRIPT 21 end_POSTSUBSCRIPT end_CELL start_CELL italic_a start_POSTSUBSCRIPT 22 end_POSTSUBSCRIPT divide start_ARG 1 - italic_e start_POSTSUPERSCRIPT - italic_ΞΈ italic_T end_POSTSUPERSCRIPT end_ARG start_ARG italic_ΞΈ end_ARG end_CELL end_ROW end_ARG ]

converges to zero, then condition (ii) of the Theorem 4.2 is verified. Consequently, depending on the conditions imposed ((c1), (c2), or (c3)), there exists a weakly solution for the mutual control problem (5.1)-(5.2), which is either unique; localized; or unique in one component and localized in both.

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