Journal of Inequalities in Pure and Applied Mathematics COERCIVENESS INEQUALITY FOR NONLOCAL BOUNDARY VALUE PROBLEMS FOR SECOND ORDER ABSTRACT ELLIPTIC DIFFERENTIAL EQUATIONS volume 4, issue 2, article 43, 2003. AISSA AIBECHE Department of Mathematics, Faculty of Sciences University Ferhat Abbas, Route de Scipion, 19000, Setif, Algeria. EMail: aibeche@wissal.dz Received 09 December, 2002; accepted 17 March, 2003. Communicated by: Z. Nashed Abstract Contents JJ J II I Home Page Go Back Close c 2000 Victoria University ISSN (electronic): 1443-5756 036-03 Quit Abstract In this paper we give conditions which assure the coercive solvability of an abstract differential equation of elliptic type with an operator in the boundary conditions, and the completeness of generalized eigenfunctions. We apply the abstract result to show that a non regular boundary value problem for a second order partial differential equation of an elliptic type in a cylindrical domain is coercive solvable. Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations 2000 Mathematics Subject Classification: 35J05, 35P20, 34L10, 47E05. Key words: Ellipticity, Abstract Differential Equation, Coerciveness, Non Regular Elliptic Problems. Aissa Aibeche Contents 1 2 3 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Notations and Definitions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Solvability of the Principal Problem . . . . . . . . . . . . . . . . . . . . . 3.1 Homogeneous Problem . . . . . . . . . . . . . . . . . . . . . . . . . 3.2 Non Homogeneous Problem . . . . . . . . . . . . . . . . . . . . . 4 Solvability of the General Problem . . . . . . . . . . . . . . . . . . . . . . 5 Completeness of Root Functions . . . . . . . . . . . . . . . . . . . . . . . . 6 Application . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . References 3 4 7 7 13 18 21 24 Title Page Contents JJ J II I Go Back Close Quit Page 2 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 1. Introduction Many works are devoted to the study of hyperbolic or parabolic abstract equations [16, 18, 9]. In [16, 20] regular boundary value problems for elliptic abstract equations are considered. A few works are concerned with non regular problems. In this paper we establish conditions guaranteeing that non local boundary value problem for elliptic abstract differential equation of the second order in an interval is coercive solvable in the Hilbert space L2 (0, 1; H). A coercive estimates, when the problem is regular, was proved in [1, 3]. The considered problem is not regular, since the boundary conditions are non local, similar problems have been considered in [4, 5, 7, 22]. Moreover, we prove the completeness of root functions. The completeness of root functions for regular boundary value problems are proved in [1, 6, 10, 14] and in the book [22]. The obtained results are then applied to study a non local boundary value problem for the Laplace equation in a cylinder. Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations Aissa Aibeche Title Page Contents JJ J II I Go Back Close Quit Page 3 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 2. Notations and Definitions Let H be a Hilbert space, A a linear closed operator in H and D(A) its domain. We denote by L(H) the space of bounded linear operators acting on H, with the usual operator norm, and by Lp (0, 1; H) the space of strongly measurable functions x → u(x) : [0, 1] → H, whose pth −power are summable, with the norm Z 1 p p kuk0,p = kukLp (0,1;H) = ku(x)kpH dx < ∞, p ∈ [1, ∞] . 0 Now, introduce the Lp (0, 1; H) vector-valued Sobolev spaces Wp2 (0, 1; H1 , H), where H1 , H are Hilbert spaces such that H1 ⊂ H with continuous embedding Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations Wp2 (0, 1; H1 , H) = {u : u00 ∈ Lp (0, 1; H) and u ∈ Lp (0, 1; H1 )} Aissa Aibeche kukWp2 (0,1;H1 ,H) = kukLp (0,1;H1 ) + ku00 kLp (0,1;H) < ∞. Title Page and Let E0 , E1 be two Banach spaces, which are continuously injected in the Banach space E, the pair {E0 , E1 } is said to be an interpolation couple. Consider the Banach space E0 + E1 = {u : u ∈ E, ∃uj ∈ Ej , j = 0, 1, with u = u0 + u1 } , kukE0 +E1 = inf ku0 kE0 + ku1 kE1 , u=u0 +u1 ;uj ∈Ej JJ J II I Go Back Close Quit and the functional K(t, u) = Contents inf u=u0 +u1 ;uj ∈Ej ku0 kE0 + t ku1 kE1 . Page 4 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 The interpolation space for the couple {E0 , E1 } is defined, by the K-method, as follows ( ) Z ∞ p1 (E0 , E1 )θ,p = u : u ∈ E0 + E1 , kukθ,p = t−1−θp K p (t, u)dt <∞ , 0 0 < θ < 1, 1 ≤ p ≤ ∞. ( (E0 , E1 )θ,∞ = ) u : u ∈ E0 + E1 , kukθ,∞ = sup t−θ K(t, u)dt < ∞ , t∈(0,∞) 0 < θ < 1. Let A be a closed operator in H. H(A) is the domain of A provided with the Hilbertian graph norm kuk2H(A) = kAuk2 + kuk2 , u ∈ D(A). kukpθ,p Z = Aissa Aibeche Title Page If −A is the infinitesimal generator of the semigroup exp(−xA) which is analytic for x > 0, decreasing at infinity and strongly continuous for x ≥ 0, then the following holds [19, p. 96]: n o (H, H(An ))θ,p = u : u ∈ H, kukpθ,p < ∞ , where Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations Contents JJ J II I Go Back Close ∞ −n(1−θ)p−1 t n p p kA exp(−tA)uk dt + kuk , Quit 0 0 < θ < 1, n ∈ N, 1 ≤ p < ∞ and kukθ,p its norm. Page 5 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 Let H and H1 be Hilbert spaces such that the imbedding H1 ⊂ H is continuous and H1 = H. Then (H, H1 )θ,2 , is a Hilbert space, we denote it by (H, H1 )θ . It is known that (H, H1 )θ = H(S θ ), where S is a self-adjoint positive-definite operator in H [17]. +∞ 1 R Let F f (σ) = (2π)− 2 exp(iσx)f (x)dx be the Fourier transform of the −∞ function f. Lemma 2.1. [22, p. 300] Let A be a self adjoint and positive definite operator in H. Then i h i h 1 1 1. ∃ω > 0, Aα exp −x (A + λI) 2 ≤ C exp −ωx |λ| 2 for all α ∈ R, x ≥ x0 > 0, |arg λ| ≤ ϕ < π, where C does not depend on x and λ. i h R1 1 α− 14 2 α 2α− 12 2 2 2. 0 (A + λI) exp −x (A + λI) u ≤ C A u + |λ| kuk 1 for all α ≥ 14 , |arg λ| ≤ ϕ < π, and u ∈ D Aα− 4 , where C does not depend on u and λ. α −β 3. A (A + λI) ≤ C (1 + |λ|)α−β , for all 0 ≤ α ≤ β, |arg λ| ≤ ϕ < π, where C does not depend on λ. Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations Aissa Aibeche Title Page Contents JJ J II I Go Back Close Quit Page 6 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 3. 3.1. Solvability of the Principal Problem Homogeneous Problem Consider in the Hilbert space H the boundary value problem for the second order abstract differential equation (3.1) L(D)u = −u00 (x) + Au(x) + A(x)u(x) = f (x) L1 u = δu(0) (3.2) x ∈ (0, 1), Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations = f1 , L2 u = u0 (1) + Bu(0) = f2 , Aissa Aibeche A, A(x), B are linear operators and δ is a complex number. Looking to the principal part of the problem (3.1), (3.2) with a parameter (3.3) 00 L(D)u = −u (x) + (A + λI)u(x) = 0 L1 u = δu(0) (3.4) x ∈ (0, 1), = f1 , L2 u = u0 (1) + Bu(0) = f2 . Theorem 3.1. Assume that the following conditions are satisfied Title Page Contents JJ J II I Go Back Close Quit 1. A is a self-adjoint and positive-definite operator in H. Page 7 of 29 2. δ 6= 0. J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 3. B is continuous from H(A1/2 ) in H(A) and from H in H(A1/2 ). Then the problem (3.3), (3.4) for f1 ∈ (H, H(A)) 1 , f2 ∈ (H, H(A)) 3 and 4 4 for λ such that |arg λ| ≤ φ < π, |λ| −→ ∞, has a unique solution in the space W22 (0, 1; H(A), H), and for the solution of the problem (3.3), (3.4) the following coercive estimate holds (3.5) ku00 kL2 (0,1;H) + kAukL2 (0,1;H) + |λ| kukL2 (0,1;H) 3 3 ≤ C A 4 f1 + |λ| 4 kf1 kH H 1 1 + A 4 f2 + |λ| 4 kf2 kH , H Aissa Aibeche where C does not depend on λ. Proof. The solution u, belonging to W22 (0, 1; H(A), H), of the equation (3.3) is in the form 1 (3.6) Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations −xAλ2 u(x) = e Contents 1 −(1−x)Aλ2 g1 + e Title Page g2 with Aλ = A + λI and g1 , g2 ∈ (H, H(A)) 3 . 4 Indeed, let u ∈ W22 (0, 1; H(A), H) be a solution of (3.3). Then we have 1 1 D − Aλ2 D + Aλ2 u(x) = 0. JJ J II I Go Back Close Quit Note by 1 v(x) = D + Aλ2 u(x). Page 8 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 1 From [22, p. 168] v ∈ W21 (0, 1; H(A 2 ), H) and 1 2 (3.7) D − Aλ v(x) = 0. So 1 2 v(x) = e−(1−x)Aλ v(1), (3.8) where, according to [19, p. 44], 1 1 v(1) ∈ H(A 2 ), H 1 = H, H(A 2 ) 1 . Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations 2 2 From (3.7) , (3.8) we have 1 −xAλ2 Aissa Aibeche Z x 1 2 1 2 e−(x−y)Aλ e−(1−y)Aλ v(1)dy 0 1 1 1 1 1 2 − 12 −xAλ2 −Aλ2 −xAλ −(1−x)Aλ2 −e e v(1), u(0) + Aλ e =e 2 u(x) = e u(0) + where u(0) ∈ (H(A), H) 1 [19, p. 44]. Now, 2 1 1 A 2 : (H, H(A)) 3 → (H, H(A)) 1 = H, H(A 2 ) 1 4 4 2 is an isomorphism. Consequently the last inequality is in the form (3.6). Let us show the reverse, i.e. the function u in the form (3.6) with g1 and g2 in (H, H(A)) 3 , belongs to W22 (0, 1; H(A), H). From interpolation spaces Title Page Contents JJ J II I Go Back Close Quit Page 9 of 29 4 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 properties see [15], [19, p. 96] and the expression (3.6) of the function u we have kukW 2 (0,1;H(A),H) 2 +1 ≤ AA−1 λ 2 ! 21 Z 1 1 Aλ e−xAλ2 g1 dx × + Z 0 1 0 2 ! 12 1 Aλ e−(1−x)Aλ2 g2 dx Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations ≤ C kg1 k(H,H(Aλ )) 3 + kg2 k(H,H(Aλ )) 3 4 4 (3.9) ≤ C(λ) kg1 k(H,H(A)) 3 + kg2 k(H,H(A)) 3 . 4 Aissa Aibeche 4 The function u satisfies the boundary conditions (3.4) if 1 δg1 + δe−Aλ2 g2 = f1 , 1 2 1 −Aλ2 −Aλ e Contents JJ J 1 1 2 g1 + Bg1 + Aλ g2 + Be which we can write in matrix form as: δI 0 0 + (3.10) 1 1 1 2 B Aλ2 −Aλ2 e−Aλ Title Page −Aλ2 g2 = f2 , II I Go Back 1 −Aλ2 δe Be 1 −Aλ2 g1 ! f1 = g2 Close ! . f2 Quit Page 10 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 The first matrix of operators is invertible, its inverse is 1 I 0 δ . (3.11) 1 − 12 1 −2 − δ Aλ B Aλ Multiplying the two members of (3.10) by the matrix inverse (3.11), we get the following system: 1 g1 + e−Aλ2 g2 = 1δ f1 1 −Aλ2 e g1 + g2 = −1 − 1δ Aλ 2 Bf1 + −1 Aλ 2 f2 we can solve it by Cramer’s method, because the coefficients of the linear sys1 2 tem are bounded linear operators. The determinant is givenby I + e−2Aλ which −2A 21 is invertible as a little perturbation of unity, in fact e λ ≤ q < 1. Hence the solution is written as g1 = 1δ f1 + R11 (λ)f1 + R12 (λ)f2 , (3.12) g = − 1 (I + T (λ)) A− 12 Bf + (I + T (λ)) A− 12 f + R (λ)f , 2 1 2 21 1 λ λ δ where Rij (λ) are given by 1 1 − 12 −A 2 1 1 −2Aλ2 λ B, R (λ) = − (I + T (λ)) e + (I + T (λ)) A e 11 λ δ δ 1 1 − 2 R12 (λ) = − (I + T (λ)) Aλ 2 e−Aλ , 1 R (λ) = 1 (I + T (λ)) e−Aλ2 , 21 δ Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations Aissa Aibeche Title Page Contents JJ J II I Go Back Close Quit Page 11 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 and satisfy kRij (λ)k → 0 when |λ| → ∞. (I + T (λ)) is the inverse of I + 1 2 e−2Aλ obtained from the corresponding Neumann series. Finally the solution u is given by 1 −xAλ2 u(x) = e 1 f1 + R11 (λ)f1 + R12 (λ)f2 δ 1 1 −1 −(1−x)Aλ2 +e − (I + T (λ)) Aλ 2 Bf1 δ + (I + −1 T (λ)) Aλ 2 f2 + R21 (λ)f1 . From the assumptions of Theorem 3.1 and the properties of interpolation spaces, the following applications are continuous, −1 (I + T (λ)) Aλ 2 B : (H, H(A)) 3 7−→ (H, H(A)) 3 , 4 4 Aissa Aibeche Title Page Contents −1 (I + T (λ)) Aλ 2 : (H, H(A)) 1 7−→ (H, H(A)) 3 . 4 4 Then we have the estimates − 21 (I + T (λ)) Aλ Bf1 (H,H(A)) 3 ≤ C kf1 k(H,H(A)) 3 −1 (I + T (λ)) Aλ 2 f2 (H,H(A)) 3 4 JJ J II I Go Back 4 4 and Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations Close ≤ C kf2 k(H,H(A)) 1 . 4 Quit Page 12 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 Set u(x) = u1 (x) + u2 (x) + u3 (x), where 1 1 2 u1 (x) = e−xAλ f1 , δ 1 −(1−x)A 12 −1 λ (I + T (λ)) Aλ 2 Bf1 , u2 (x) = − e δ 1 − 12 −(1−x)Aλ2 u2 (x) = e (I + T (λ)) Aλ f2 . Then ku1 kW 2 (0,1;H(A),H) 2 1 −xA 12 1 1 2 −xA Ae λ f1 Aλ e λ f1 . + = |δ| |δ| L2 (0,1;H) L2 (0,1;H) Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations Aissa Aibeche However, from Lemma 2.1, we have 3 1 3 4 Aλ e−xAλ2 f1 4 kf k ≤ C A f + |λ| 1 1 H . L2 (0,1;H) H Non Homogeneous Problem L0 (λ, D)u = −u00 (x) + Aλ u(x) = f (x) II I Go Back Consider, now, the principal problem for the non homogeneous equation with a parameter (3.13) Contents JJ J Similarly we obtain bounds for u2 and u3 . 3.2. Title Page x ∈ (0, 1), Close Quit Page 13 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 L10 u = δu(0) (3.14) = f1 , L20 u = u0 (1) + Bu(0) = f2 . We have the result. Theorem 3.2. Suppose the following conditions satisfied Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations 1. A is a self-adjoint and positive-definite operator in H. 2. B is continuous from H(A1/2 ) in H(A) and from H in H(A1/2 ). 3. δ 6= 0. Aissa Aibeche Then the problem (3.13), (3.14), for f, f1 and f2 in L2 (0, 1; H), (H, H(A)) 3 4 and (H, H(A)) 1 respectively, and for λ such that |arg λ| ≤ φ < π, |λ| −→ 4 ∞, has a unique solution belonging to the space (1, ∞), and the following coercive estimate holds (3.15) Wp2 (0, 1; H(A), H), for p ∈ ku00 kL2 (0,1;H) + kAukL2 (0,1;H) + |λ| kukL2 (0,1;H) 3 ≤ C kf kL2 (0,1;H) + A 4 f1 H1 3 1 4 4 4 + |λ| kf1 kH + A f2 + |λ| kf2 kH , H where C does not depend on λ. Title Page Contents JJ J II I Go Back Close Quit Page 14 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 Proof. In Theorem 3.1, we proved the uniqueness. Let us now show that the solution of the problem (3.13), (3.14) belonging to Wp2 (0, 1; H(A), H) can be written in the form u(x) = u1 (x) + u2 (x), u1 (x) is the restriction to [0, 1] of u e1 (x), where u e1 (x) is the solution of the equation (3.16) L0 (λ, D)e u1 (x) = fe(x), x ∈ R, with fe(x) = f (x) if x ∈ [0, 1] and fe(x) = 0 otherwise. u2 (x) is the solution of the problem (3.17) L0 (λ, D)u2 = 0, L10 u2 = f1 − L10 u1 , L20 u2 = f2 − L20 u1 . The solution of the equation (3.16) is given by the formula Z 1 b (3.18) u b1 (x) = √ eiµx L0 (λ, iµ)−1 fe(µ)dµ 2π R b where fe is the Fourier transform of the function fe(x), L0 (λ, s) is the characteristic pencil of the equation (3.16) i.e. L0 (λ, s) = −s2 I + A + λI. From (3.18) and Plancherel equality it follows that: |λ| ku1 kL2 (0,1;H) + ku001 kL2 (0,1;H) + kAu1 kL2 (0,1;H) (3.19) ≤ |λ| kb u1 kL2 (R;H(A)) + kb u001 kL2 (R;H) + kAb u1 kL2 (R;H) ≤ |λ| F −1 L0 (λ, iµ)−1 F fe(µ) L2 (R;H) −1 2 −1 e + F (iµ) L0 (λ, iµ) F f (µ) L2 (R;H) −1 −1 e , + F AL0 (λ, iµ) F f (µ) Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations Aissa Aibeche Title Page Contents JJ J II I Go Back Close Quit Page 15 of 29 L2 (R;H) J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 where F is the Fourier transform. From condition (1) of Theorem 3.2, for |arg λ| ≤ ϕ < π and |λ| sufficiently large, we have L0 (λ, iµ)−1 = (A + λI + µ2 I)−1 (3.20) ≤ C(1 + λ + µ2 )−1 ≤ C |µ|−2 (3.21) AL0 (λ, iµ)−1 = A(A + λI + µ2 I)−1 ≤ C (3.22) |λ| L0 (λ, iµ)−1 = |λ| (A + λI + µ2 I)−1 ≤ C |λ| (1 + λ + µ2 )−1 ≤ C. Aissa Aibeche Title Page Then it follows that |λ| ku1 kL2 (0,1;H) + ku001 kL2 (0,1;H) + kAu1 kL2 (0,1;H) ≤ C kf kL2 (0,1;H) . Since u1 ∈ Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations W22 (0, 1; H(A), H) and from [19, p. 44] we have u01 (0) ∈ (H(A), H) 3 = (H, H(A)) 1 , 4 JJ J II I Go Back 4 Close u1 (0) ∈ (H, H(A)) 3 . 4 Quit Therefore L10 u1 ∈ (H, H(A)) 3 and L20 u1 ∈ (H, H(A)) 1 . 4 Contents 4 Page 16 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 From Theorem 3.1, the problem (3.17) , when |arg λ| ≤ φ < π, |λ| → ∞, has a solution u2 (x) which is in W22 (0, 1; H(A), H). Now, we have to find bounds for the following terms 3 3 4 4 A L10 u1 = A u1 (0) , H H 3 3 |λ| 4 kL10 u1 kH = |λ| 4 ku1 (0)kH , 1 1 1 4 A L20 u1 ≤ A 4 u01 (1) + A 4 Bu1 (0) H and 1 H 1 H 1 |λ| 4 kL20 u1 kH ≤ |λ| 4 ku01 (1)kH + |λ| 4 kBu1 (0)kH . Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations Aissa Aibeche For example, we have 3 |λ| 4 ku1 (0)kH ≤ C ku1 kW 2 (0,1;H(A),H) + |λ| ku1 kL2 (0,1;H) 2 ≤ C kf kL2 (0,1;H) . Similarly, we get the other bounds and by the same way the coerciveness estimate. Title Page Contents JJ J II I Go Back Close Quit Page 17 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 4. Solvability of the General Problem Consider, now, the general problem with a parameter (4.1) L0 (λ, D)u = λu(x)−u00 (x)+Au(x)+A(x)u(x) = f (x) L10 u = δu(0) (4.2) x ∈ (0, 1), = f1 , Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations L20 u = u0 (1) + Bu(0) = f2 . We have the result. Theorem 4.1. Suppose the following conditions satisfied Aissa Aibeche 1. A is a self-adjoint and positive-definite operator in H. Title Page 2. The imbedding H(A) ⊂ H is compact. 3. B is continuous from H(A 1/2 ) in H(A) and from H in H(A Contents 1/2 ). 4. δ 6= 0. 5. kA(.)ukL2 (0,1;H) ≤ kAukL2 (0,1;H) + C() kukL2 (0,1;H) . Then the problem (4.1), (4.2), for f, f1 and f2 in L2 (0, 1; H), (H, H(A)) 3 4 and (H, H(A)) 1 respectively, and for λ such that |arg λ| ≤ φ < π, |λ| −→ 4 JJ J II I Go Back Close Quit Page 18 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 ∞, has a unique solution belonging to the space Wp2 (0, 1; H(A), H), for p ∈ (1, ∞), and the following coercive estimate holds (4.3) ku00 kL2 (0,1;H) + kAukL2 (0,1;H) + |λ| kukL2 (0,1;H) 3 ≤ C kf kL2 (0,1;H) + A 4 f1 H1 3 1 + |λ| 4 kf1 kH + A 4 f2 + |λ| 4 kf2 kH . H where C does not depend on u, f, f1, f2, and λ. Proof. Let u be a solution of (4.1), (4.2) belonging to W22 (0, 1; H(A), H). Then u is a solution of the problem x ∈ (0, 1), L0 (λ, D)u = f (x) − A(x)u(x) L u = δu(0) = f1 10 (P0 ) L20 u = u0 (1) + Bu(0) = f2 . From Theorem 3.2, we get the estimate ku00 kL2 (0,1;H) + kAukL2 (0,1;H) + |λ| kukL2 (0,1;H) 3 ≤ C kf − A(.)ukL2 (0,1;H) + A 4 f1 1 H 3 1 + |λ| 4 kf1 kH + A 4 f2 + |λ| 4 kf2 kH . H Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations Aissa Aibeche Title Page Contents JJ J II I Go Back Close Quit Page 19 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 Using condition (5) of Theorem 3.2, we get ku00 kL2 (0,1;H) + (1 − C) kAukL2 (0,1;H) + (|λ| − C.C()) kukL2 (0,1;H) 3 ≤ C kf kL2 (0,1;H) + A 4 f1 H1 3 1 4 4 4 + |λ| kf1 kH + A f2 + |λ| kf2 kH . H Choosing such that C · < 1, the coerciveness estimates follows easily. Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations Aissa Aibeche Title Page Contents JJ J II I Go Back Close Quit Page 20 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 5. Completeness of Root Functions Let us define the operator L by Lu ≡ −u00 + Au, D (L) = W22 (0, 1; H(A), H, Lk u = 0, k = 0, 1) . Lemma 5.1. Suppose that sj (I, H(A), H) ' Cj −q then sj I, W22 − 11 (0, 1; H(A), H) , L2 (0, 1; H) ' Cj 2 +q . I (resp. I) is the imbedding of H(A) in H (resp. of W22 (0, 1; H(A), H) in L2 (0, 1; H)) and sj (I, H(A), H) are the s-numbers of the operator I from H(A) to H. Proof. Let S1 be the operator defined in L2 (0, 1) such that S1 = S1∗ ≥ γ 2 I, D(S1 ) = H(S1 ) = W22 (0, 1). From [17], we know that if H1 ⊂ H and H1 is dense in H then there exists an operator S1 such that S1 = S1∗ and D(S1 ) = H. Otherwise, let S2 be the operator defined by S2 = S2∗ ≥ γ 2 I, D(S2 ) = H(A). If we define the operator S on L2 (0, 1)⊗H = L2 (0, 1; H) by S = S1 ⊗I2 +I1 ⊗S2 , where I1 (resp. I2 ) is the identity operator in L2 (0, 1) (resp. H). We have sj S1−1 , L2 (0, 1), L2 (0, 1) ' sj (I, H(S1 ), L2 (0, 1)) ' Cj −2 , sj S2−1 , H, H ' sj (I, H(A), H) ' Cj −q . Hence, from [11], we obtain sj (S −1 , L2 (0, 1; H), L2 (0, 1; H)) ' Cj − 1 1 +q 2 . Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations Aissa Aibeche Title Page Contents JJ J II I Go Back Close Quit Page 21 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 Theorem 5.2. Let the conditions of Theorem 3.2 hold along with A−1 ∈ σq (H) , q > 0. Then, the system of root functions of the operator L is complete in L2 (0, 1; H). Proof. From Theorem 4.1, we have kR(λ, L)k ≤ C |λ|−1 for |arg λ| ≤ ϕ < π and |λ| sufficiently large. Using Lemma 5.1, we have R(λ, L) ∈ σp (L2 (0, 1; H)) for p > 12 + 1q , so, for the operator L, all the conditions of [8, Theorem 126, 2.3, p. 50], are fulfilled. This achieves the proof of the theorem. Theorem 5.3. Suppose that the conditions of Theorem 5.2 are satisfied as well as the condition D(A(x)) ⊂ D(A) and ∀ > 0, kA(·)ukH ≤ kAukH + C() kukH . u ∈ D(A). Let A be the operator defined by (Au) (x) = A(x)u(x), D (A) = L2 (0, 1; H). Then the system of root functions of L + A is complete in L2 (0, 1; H). Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations Aissa Aibeche Proof. It is clear that Title Page kAukL2 (0,1;H) ≤ kAukL2 (0,1;H) + C() kukL2 (0,1;H) . Since by Theorem 4.1, we have kAukL2 (0,1;H) ≤ C kf kL2 (0,1;H) = C k(L − λI) ukL2 (0,1;H) , Contents JJ J II I Go Back hence kAukL2 (0,1;H) ≤ k(L − λI) ukL2 (0,1;H) + C() kukL2 (0,1;H) and so, for |λ| sufficiently large and |arg λ| ≤ ϕ < π, Close Quit Page 22 of 29 R(λ, L + A) ∈ σp (L2 (0, 1; H)) , J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 and from Theorem 4.1 we have kR(λ, L + A)k ≤ C |λ|−1 for |λ| sufficiently large and |arg λ| ≤ ϕ < π. Then the system of root functions is complete in L2 (0, 1; H). Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations Aissa Aibeche Title Page Contents JJ J II I Go Back Close Quit Page 23 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 6. Application Let us consider, in the cylindrical domain Ω = [0, 1]×G the non local boundary value problem for the Laplace equation with a parameter L(λ)u = λu(x, y) − ∆u(x, y) + b(x, y)u(x, y) = f (x, y), (x, y) ∈ Ω; y ∈ G; (6.1) (P ) L1 u = δu(0, y) = f1 (y), ∂ L2 u = ∂x u(1, y) + Bu(0, y) = f2 (y), y ∈ G; P u = u(x, y 0 ) = 0, (x, y 0 ) ∈ Γ, where Γ = [0, 1] × ∂G and ∂G is the boundary of G. A number λ0 is called an eigenvalue of (P ) if the problem L(λ0 )u = 0, (x, y) ∈ Ω; L1 u = 0, y ∈ G; 0 (6.2) (P ) L2 u = 0, y ∈ G; P u = 0, (x, y 0 ) ∈ Γ, has a non trivial solution that belongs to W22 (Ω). The non trivial solution u0 of (P 0 ) that belongs to W22 (Ω) is called the eigenfunction of (P ) corresponding to Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations Aissa Aibeche Title Page Contents JJ J II I Go Back Close Quit Page 24 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 the eigenvalue λ0. Solutions uk of L(λ0 )uk + uk−1 = 0, L1 uk = 0, 00 (6.3) (P ) L2 uk = 0, P uk = 0, (x, y) ∈ Ω; y ∈ G; y ∈ G; (x, y 0 ) ∈ Γ, belonging to W22 (Ω) are associated functions of the k−th rank to the eigenvalue u0 of (P ) . Eigenfunctions and associated functions of (P ) are gathered under the general name of root functions of (P ) . 0,1 Theorem 6.1. Let b(x, y) ∈ W∞ (Ω), δ 6= 0, ∂G ∈ C 2 then − W2 mk 2 Aissa Aibeche + 34 (G, P u = 0) and for λ 1. (P ) , for f ∈ W20,1 (Ω, P u = 0), fk ∈ such that |λ| sufficiently large and |arg λ| ≤ ϕ < π, has a unique solution that belongs to the space W22 (Ω), and for this solution we have the coercive estimate 2 ≤C kf kL2 (Ω) + k=1 Title Page Contents JJ J |λ| ku00 kL2 (Ω) + kukW 2 (Ω) 2 X Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations kfk k II I Go Back m − 2k + 3 4 (G,P u=0) W2 + 2 X k=1 m − 2k |λ| Close ! + 34 kfk kH , Quit Page 25 of 29 where C does not depend on u and λ. J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 2. Root functions of (P ) are complete in L2 (Ω). Proof. Consider in H = L2 (Ω) the operators A and A(x) defined by Au = −∆u(y) + λ0 u(y), A (x) u = b(x, y)u(y) − λ0 u(y), D(A) = W22 (G, P u = 0) D(A (x)) = W21 (G, P u = 0, m = 0). Then the problem (P ) can be written in the form λu(x) − u00 (x) + Au(x) + A(x)u(x) = 0 x ∈ (0, 1), δu(0) = f1 u0 (1) + Bu(0) = f2 . We have the compact imbedding W22 (Ω) ⊂ L2 (Ω). On the other hand 2 sj I, W22 (Ω), L2 (Ω) ' j − r+1 . By virtue of Lemma 3.1 in [21, p. 60] we have sj (I, H(A), L2 (Ω)) ' sj A−1 , L2 (Ω), L2 (Ω) . W22 (Ω), −1 −1 Since H(A) ⊂ then it follows that A ∈ σp (L2 (Ω), L2 (Ω)) , then kR(λ, A)k ≤ C |λ| for |arg λ| ≤ ϕ < π and |λ| sufficiently large. Hence, all conditions of Theorem 5.3 has been checked. Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations Aissa Aibeche Title Page Contents JJ J II I Go Back Close Quit Page 26 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003 References [1] S. AGMON, On the eigenfunctions and eigenvalues of general boundary value problems, Comm. Pure Appl. Math. 15(1962), 119–147. [2] S. AGMON AND L. NIRENBERG, Properties of solutions of ordinary differential equation in Banach spaces, Comm. Pure Appl. Math., 16 (1963), 121–239. [3] M.S. 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Coerciveness Inequality for Nonlocal Boundary value Problems for Second Order Abstract Elliptic Differential Equations Aissa Aibeche Title Page Contents JJ J II I Go Back Close Quit Page 29 of 29 J. Ineq. Pure and Appl. Math. 4(2) Art. 43, 2003