On the Well-Posedness of a Two-Point Boundary-Value Problem for a System with Pseudodifferential Operators

We investigate the problem of the well-posedness of a boundary-value problem for a system of pseudodifferential equations of arbitrary order with nonlocal conditions. The equation and boundary conditions contain pseudodifferential operators whose symbols are defined and continuous in a certain domai...

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Дата:2005
Автори: Kengne, E., Кенне, Е.
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Мова:Англійська
Опубліковано: Institute of Mathematics, NAS of Ukraine 2005
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Ukrains’kyi Matematychnyi Zhurnal
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author Kengne, E.
Кенне, Е.
author_facet Kengne, E.
Кенне, Е.
author_sort Kengne, E.
baseUrl_str https://umj.imath.kiev.ua/index.php/umj/oai
collection OJS
datestamp_date 2020-03-18T20:01:36Z
description We investigate the problem of the well-posedness of a boundary-value problem for a system of pseudodifferential equations of arbitrary order with nonlocal conditions. The equation and boundary conditions contain pseudodifferential operators whose symbols are defined and continuous in a certain domain $H ⊂ ℝ_{σ}^m$. A criterion for the existence and uniqueness of solutions and for the continuous dependence of the solution on the boundary function is established.
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fulltext UDC 517.9 E. Kengne (Univ. Dschang, Cameroon) ON THE PROPER POSEDNESS OF TWO-POINT BOUNDARY-VALUE PROBLEM FOR SYSTEM WITH PSEUDODIFFERENTIAL OPERATORS PRO KOREKTNIST| DVOTOÇKOVO} KRAJOVO} ZADAÇI DLQ SYSTEM IZ PSEVDODYFERENCIAL|NYMY OPERATORAMY The question on the proper posedness of boundary-value problem with nonlocal condition for a system of pseudodifferential equations of an arbitrary order is investigated. The equation and the boundary conditions contain the pseudodifferential operators which symbols are defined and continuous in some domain H ⊂ Rσ m . The criterion of the existence, uniqueness of solutions and of the continuously dependence of the solution on the boundary function is established. Rozhlqnuto pytannq pro korektnist\ krajovo] zadaçi z nelokal\nog umovog dlq systemy psevdodyferencial\nyx rivnqn\ dovil\noho porqdku. Rivnqnnq ta hranyçni umovy mistqt\ psev- dodyferencial\ni operatory iz symvolamy, wo vyznaçeni ta neperervni u deqkij oblasti H ⊂ ⊂ Rσ m . Vstanovleno kryterij isnuvannq ta [dynosti rozv’qzkiv, a takoΩ neperervno] zaleΩnosti rozv’qzku vid hranyçno] funkci]. 1. Introduction. The present paper generalizes and evolves the results of works [1, 2]. It investigates the question of the proper posedness of nonlocal boundary-value problem for system of equations, containing the pseudodifferential operators that symbols are defined and continuous in some domain H ⊂ R m . The solution of the problem is sought in functional spaces. Consider in the infinite layer Π = R m × 0, T[ ] the following two-point boundary problem L t i x u x t u t P i x u∂ ∂ − ∂ ∂     = ∂ ∂ + − ∂ ∂     =, ( , ) 0 , (1) M i x u x t A i x u x B i x u x T x− ∂ ∂     = − ∂ ∂     + − ∂ ∂     =( , ) ( , ) ( , ) ( )0 ϕ (2) where ∂ ∂ = ∂ ∂ ∂ ∂ … ∂ ∂    x x x xm1 2 , , , , u u u um= …( )col 1 2, , , , ϕ ϕ ϕ ϕ( ) ( ), ( ), , ( )x x x xm= …( )col 1 2 ; P i x P i xjk j k l − ∂ ∂     = − ∂ ∂     =, ,1 , A i x A i xjk j k l − ∂ ∂     = − ∂ ∂     =, ,1 , B i x B i xjk j k l − ∂ ∂     = − ∂ ∂     =, ,1 matrices that elements are pseudodifferential operators with symbols P( )σ , A( )σ , and B( )σ , respectively, continuous in some domain H ⊂ Rσ m . Generally speaking, problem (1), (2) is improperly posed, even if Pjk ( )σ , Ajk ( )σ , and Bjk ( )σ are polynomials [3 – 6]. We shall be concerned with the question of the existence and uniqueness of solution © E. KENGNE, 2005 ISSN 1027-3190. Ukr. mat. Ωurn., 2005, t. 57, # 8 1131 1132 E. KENGNE of problem (1), (2), and the question of the continuously dependence of this solution on the boundary function ϕ( )x . 2. Notations and definitions. For the description of the spaces of solutions, we introduce the following notation: WΩ ∞ is the space of vector-functions u x( ) = ( u x1( ) , u x2( ), … , u xl( )), u xj ( ) ∈ ∈ L m 2 R( ), such that the Fourier transform ˆ ( )uj σ is compactly supported in Ω ⊂ ⊂ Rσ ∞ ; the space WΩ ∞ is invariant relatively to the pseudodifferential operator à x − ∂ ∂     ˜ ( ) ( ) ˜( ) ˆ( ) exp , ( )A i x u x A u ix d u x Wm− ∂ ∂     = ( ) ∈     − ∞∫2π σ σ σ σ Ω Ω with the matrix ˆ( )A σ continuous in Ω, moreover, à i x − ∂ ∂     : WΩ ∞ → WΩ ∞ is a continuous application; WΩ ∞( )′ is the space of generalized vector-functions on WΩ ∞ ; this space is invariant relatively to  i x ∂ ∂     ; WΩ +∞ = WΩ ∞( )′ , WΩ −∞ = W− ∞( )′Ω , where – Ω = { σ ∈ R m : – σ ∈ Ω }; Ck ( 0, T[ ], WΩ ±∞) are spaces of vector-functions that for every t ∈ 0, T[ ] are functions of space WΩ ±∞ respectively and continuously depend on t together with the derivatives up to order k. According to I. G. Petrovski [7], introduce the following definition: Definition. We say that problem (1), (2) is properly posed in Cn( 0, T[ ], WΩ ±∞) if, for every boundary function ϕ( )x ∈ WΩ ±∞ , problem (1), (2) should have in Cn( 0, T[ ], WΩ ±∞) one and only one solution u x t( , ) , continuously depending on ϕ( )x . We shall not be concerned with Cauchy problem (the proper posedness of the Cauchy problem for equation (1) is studied in [7]). 3. On the proper posedness of problem (1), (2). It is easily seen that the following two applications for every domain Ω ⊂ H are continuous: L t i x ∂ ∂ − ∂ ∂     , : Cn( 0, T[ ], WΩ ±∞) → C0( 0, T[ ], WΩ ±∞), u � ∂ ∂ u x t t ( , ) + P i x − ∂ ∂     u x t( , ) and M i x − ∂ ∂     : Cn( 0, T[ ], WΩ ±∞) → C0( 0, T[ ], WΩ ±∞), u � A i x − ∂ ∂     u x( , )0 + B i x u x T− ∂ ∂     ( , ). Let us prove the inverse. If we denote by ˆ( , )u tσ and ˆ ( )ϕ σ the x-Fourier transforms of the solution u x t( , ) of problem (1), (2) and the boundary function ϕ( )x , respectively, it is easily seen that ISSN 1027-3190. Ukr. mat. Ωurn., 2005, t. 57, # 8 ON THE PROPER POSEDNESS OF TWO-POINT BOUNDARY-VALUE PROBLEM … 1133 ˆ( , )u tσ is a solution of the following boundary-value problem: L d dt u t du t dt P u t, ˆ( , ) ˆ( , ) ( ) ˆ( , )σ σ σ σ σ    = + , (3) M u t( ) ˆ( , )σ σ = A u B u T( ) ˆ( , ) ( ) ˆ( , )σ σ σ σ0 + = ˆ ( )ϕ σ . (4) Let us find the fundamental matrix of solutions F t( , )σ of system (3). Because P( )σ is a matrix continuous in H, the roots of characteristic equation det ( )I Pλ σ+ = 0 are continuous functions of parameter σ. We denote by χ j = χ σj ( ) the multiplicity of the root λ j = λ σj ( ), j = 1, ν , ν = ν σ( ) . According to the theory of matrices [8], there exist two polynomial matrices M( , )λ σ and N( , )λ σ = Njk j k l ( , ) , , λ σ =1 such that M( , )λ σ × L( , )λ σ × N( , )λ σ ≡ Q( , )λ σ ≡ hj jk j k l ( , ) , , λ σ δ =1 , det ( , )N λ σ ≡ ≡ N( )σ ≠ 0, where hj ( , )λ σ = k =∏ 1 ν (λ – λ σ k q jk) ( ) , j = 1, l , where j l jkq=∑ 1 ( )σ = = χ σk ( ) , k = 1, l , and δ jk are the Kronecker symbols. It follows from the equality M( , )λ σ × L( , )λ σ × N( , )λ σ ≡ Q( , )λ σ and condition det ( , )N λ σ ≡ N( )σ ≠ 0 that M( , )λ σ × L( , )λ σ ≡ Q( , )λ σ × N−1( , )λ σ , and after using the transformation y t( , )σ = N d dt u t−     1 , ˆ( , )σ σ , system (3) takes the form Q d dt y t, ( , )σ σ    = 0, that is, h d dt y tj j, ( , )σ σ    = 0, j = 1, l . (5) The fundamental system of solutions of each of equations (5) reads as y t d d tj k k , ( , ) exp( )α α λ λ σ λ λ=     − = 1 , α σ= 1, ( )qjk , k = 1, ν . Therefore, the fundamental matrix of solutions of system (3) reads as F t( , )σ = exp( ) ( )! ! ! ( , ) , , , , , , , λ α ρ λ λ σ α β λ λ β α ν ρ α β k s s p j j l q k s t t s d d N k k × − ×    = − = = = = = − − ∑1 1 0 1 1 1 1 1 . Using the theorem of dependence of solutions on the parameter [9], we conclude that F t( , )σ is continuous with respect to σ. Therefore, the solution of system (3) reads as ˆ( , )u tσ = F t C( , )σ , where C = = col (C1, C2 , … , Cl ). Using the boundary condition (4), we find that C is a solution of the following linear algebraic system A F B F T C( ) ( , ) ( ) ( , ) ˆ ( )σ σ σ σ ϕ σ0 +( ) = , whose determinant is ∆( ) det ( ) det ( ) ( , ) ( ) ( , )σ σ σ σ σ σ= = +D A F B F T0 , where ISSN 1027-3190. Ukr. mat. Ωurn., 2005, t. 57, # 8 1134 E. KENGNE D A F B F T( ) ( ) ( , ) ( ) ( , )σ σ σ σ σ= +0 . Let Ω = H N\ ∆ , N∆ = {σ ∈ R m : ∆( )σ = 0}. For every σ ∈ Ω , C = C( )σ = = D−1( )σ × ˆ ( )ϕ σ and the solution of problem (3), (4) reads as ˆ( , )u tσ = F t( , )σ × × D−1( )σ ˆ ( )ϕ σ ∀ ∈( )σ Ω . Let W t( , )σ = F t( , )σ × D−1( )σ . Associate with matrix W t( , )σ the pseudodifferential operator W i x t− ∂ ∂     , that acts continuously from WΩ ±∞ respectively to Cn( 0, T[ ], WΩ ±∞), that is, W i x t− ∂ ∂     , : WΩ ±∞ → Cn( 0, T[ ], WΩ ±∞), u x( ) � W i x t− ∂ ∂     , u x( ) is a continuous application on WΩ ±∞ . Theorem. In order that problem (1), (2) should be properly posed in Cn( 0, T[ ], WΩ ±∞), it is necessary and sufficient that Ω = H N\ ∆ . Proof. It is clear that Ω ⊂ H . We prove the theorem in the case of Cn( 0, T[ ], WΩ +∞) (the case of Cn( 0, T[ ], WΩ −∞) can be done by analogy with [8]). Necessity. If σ0 ∈ Ω ∩ N∆ , the homogeneous problem L d dt u t, ˆ( , )σ σ0 0 0     = , M u t A u B u T( ) ˆ( , ) ( ) ˆ( , ) ( ) ˆ( , )σ σ σ σ σ σ0 0 0 0 0 00 0= + = possesses more than one solution. Consequently, the solution (if it exists) of the homogeneous problem L t i x u x t∂ ∂ − ∂ ∂     =, ( , ) 0, M i x u x t A i x u x B i x u x T− ∂ ∂     = − ∂ ∂     + − ∂ ∂     =( , ) ( , ) ( , )0 0 is not unique in Cn( 0, T[ ], WΩ +∞), and this implies the nonuniqueness of solutions of problem (1), (2) in Cn( 0, T[ ], WΩ +∞). The ill-posedness of problem (1), (2) in Cn( 0, T[ ], WΩ +∞) follows from the nonuniqueness of its solution in Cn( 0, T[ ], WΩ +∞). Sufficiency. Let Ω = H N\ ∆ . For every ϕ( )x ∈ WΩ +∞ , u x t( , ) = W i x t− ∂ ∂     , ϕ( )x is a solution of problem (1), (2) in Cn( 0, T[ ], WΩ +∞) and continuously depends on ϕ( )x , which implies the existence of solution of problem (1), (2) in Cn( 0, T[ ], WΩ +∞) that continuously depends on ϕ( )x . In order to prove the uniqueness of solution of problem (1), (2), let us notice that if u x t( , ) ∈ Cn( 0, T[ ], WΩ +∞), its x-Fourier transform ˆ( , )u tσ will be a solution of problem (3), (4). Under the condition of the theorem, this problem (3), (4) possesses one and only one solution for every σ ∈ Ω . If σ ∈ R m \ Ω , then ˜( , )u tσ ≡ 0. This implies the uniqueness of solution of problem (1), (2) in Cn( 0, T[ ], WΩ +∞), and the theorem is proved. 4. Application. Consider an infinite set of point-like particles, disposed on a string ISSN 1027-3190. Ukr. mat. Ωurn., 2005, t. 57, # 8 ON THE PROPER POSEDNESS OF TWO-POINT BOUNDARY-VALUE PROBLEM … 1135 at the same distances l from each other; the mass of each particle is m, while F is the tension of the string. The values of F and m are supposed to be constant every- where and independent of time. Particles are supposed to have only one degree of freedom. At each given time t, the motion of the j-th particle is completely defined in terms of the position of its adjacent particles, i.e., the ( j – 1)-th and ( j + 1)-th ones ( j = 0, ± 1, ± 2, … ). Thus, the fundamental law of dynamics is given by ˙̇ ( ) ( ) ( ) ( )v v v vn n n nt a t t t= + −( )+ − 2 1 14 2 , n = 0, ± 1, ± 2, … , (6) being a = 2 F ml . We associate with (6) the boundary conditions v vn n nT( ) ( )0 + = ϕ , (7) ˙ ( ) ˙ ( )v vn n nT0 + = ψ . Consider the differentiable function v( , )x t that takes the values of vj at the nodes of the lattice, i.e., v( , )jl t = vj t( ) . Therefore, system (6) acquires the form of the difference-differential equation ∂ ∂ = + − + −[ ] 2 2 2 4 2 v v v v ( , ) ( , ) ( , ) ( , ) x t t a x l t x t x l t , 0 < t < T. (8) After using the equality e x t i i x − ∂ ∂    2 v( , ) = v( , )x l t+ , equation (8) takes the form of the pseudodifferential equation: ∂ ∂ + − ∂ ∂     = 2 2 2 2 0v v t a i x sin , 0 < t < T. (9) By setting u = col (u1, u2 ) with u1 = v and u2 = ∂ ∂ v t , equation (9) and the boundary conditions (7) become ∂ ∂ + − ∂ ∂     =u t P i x u 0 , (10) u x u x T x1 1 10( , ) ( , ) ( )+ = θ , (11) u x u x T x2 2 20( , ) ( , ) ( )+ = θ , respectively, where P i x a i x − ∂ ∂     = − − ∂ ∂           0 1 02 2sin and θ1( )x and θ2( )x are two differentiable functions that take the values of ϕn and ψn , respectively, at the nodes of the lattice. For this example, F t( , )σ reads as F t( , )σ = cos sin sin sin sin sin sin sin cos sin at at a at a at σ σ σ σ σ σ ( ) − ( ) − ( ) − ( )     and ∆( ) sin cos sinσ σ σ= − + ( )[ ]2 1a aT . Therefore, ISSN 1027-3190. Ukr. mat. Ωurn., 2005, t. 57, # 8 1136 E. KENGNE N k k aT aT k aT kk∆ = { } + − + ≤ ≤ + ∈     ∈π π π π π πZ Z∪ arcsin ( ) , , 2 1 2 2 . If we take H = R, we conclude from the above theorem that problem (10), (11) is properly posed in Cn( 0, T[ ], WΩ ±∞) with Ω = R \ N∆ . 1. Borok V. M., Fardigola L. V. Nonlocal properly posed boundary problem in the layer // Math. Note Acad. Sci. USSR. – 1990. – 48. – P. 20 – 25. 2. Kengne E. Criterion of the regularity of boundary problems with an integral in the boundary condition. – Moscow: VINITI, 1992. – Vol. 92. – 20 p. 3. Antepko I. I. On the boundary problem in an infinite layer for system of linear partial differential equations // News Kharkov Univ. – 1971. – Issue 67 (36). – P. 62 – 72. 4. Borok V. M., Antepko I. I. Criterion of the proper posedness of boundary problem in the layer // Teor. functs., Funkts. Analys i Pril. – 1976. – 26. – P. 3 – 9. 5. Kengne E., Pelap F. B. Regularity of two-point boundary-value problem // Afr. Math. – 2001. – 12, # 3. – P. 61 – 70. 6. Kengne E. Properly posed and regular nonlocal boundary-value problems for partial differential equations // Ukr. Math. J. – 2002. – 54, # 8. – P. 1135 – 1142. 7. Petrovskii I. G. On the Cauchy problem for system of linear partial differential equations in the domain on nonanalytical functions // Bull. Moscow State Univ. Sect. A. – 1938. – 1. – P. 1 – 72. 8. Gantmakher F. R. Theory of matrices. – Moscow: Nauka, 1988. – 552 p. 9. Petrovskii I. G. Lecture on the theory of ordinary differential equations. – Moscow: Nauka, 1970. – 279 p. Received 22.01.2004 ISSN 1027-3190. Ukr. mat. Ωurn., 2005, t. 57, # 8
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spelling umjimathkievua-article-36712020-03-18T20:01:36Z On the Well-Posedness of a Two-Point Boundary-Value Problem for a System with Pseudodifferential Operators Про коректність двоточкової крайової задачі для систем із псевдодиференціальними операторами Kengne, E. Кенне, Е. We investigate the problem of the well-posedness of a boundary-value problem for a system of pseudodifferential equations of arbitrary order with nonlocal conditions. The equation and boundary conditions contain pseudodifferential operators whose symbols are defined and continuous in a certain domain $H ⊂ ℝ_{σ}^m$. A criterion for the existence and uniqueness of solutions and for the continuous dependence of the solution on the boundary function is established. Розглянуто питання про коректність крайової задачі з нелокальною умовою для системи псевдодиференціальних рівнянь довільного порядку. Рівняння та граничні умови містять псевдодиференціальні оператори із символами, що визначені та неперервні у деякій області $H \subset \mathbb{R}^m_{\sigma}$. Встановлено критерій існування та єдиності розв&#039;язків, а також неперервної залежності розв&#039;язку від граничної функції. Institute of Mathematics, NAS of Ukraine 2005-08-25 Article Article application/pdf https://umj.imath.kiev.ua/index.php/umj/article/view/3671 Ukrains’kyi Matematychnyi Zhurnal; Vol. 57 No. 8 (2005); 1131 – 1136 Український математичний журнал; Том 57 № 8 (2005); 1131 – 1136 1027-3190 en https://umj.imath.kiev.ua/index.php/umj/article/view/3671/4070 https://umj.imath.kiev.ua/index.php/umj/article/view/3671/4071 Copyright (c) 2005 Kengne E.
spellingShingle Kengne, E.
Кенне, Е.
On the Well-Posedness of a Two-Point Boundary-Value Problem for a System with Pseudodifferential Operators
title On the Well-Posedness of a Two-Point Boundary-Value Problem for a System with Pseudodifferential Operators
title_alt Про коректність двоточкової крайової задачі для систем із псевдодиференціальними операторами
title_full On the Well-Posedness of a Two-Point Boundary-Value Problem for a System with Pseudodifferential Operators
title_fullStr On the Well-Posedness of a Two-Point Boundary-Value Problem for a System with Pseudodifferential Operators
title_full_unstemmed On the Well-Posedness of a Two-Point Boundary-Value Problem for a System with Pseudodifferential Operators
title_short On the Well-Posedness of a Two-Point Boundary-Value Problem for a System with Pseudodifferential Operators
title_sort on the well-posedness of a two-point boundary-value problem for a system with pseudodifferential operators
url https://umj.imath.kiev.ua/index.php/umj/article/view/3671
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