eBook ISBN:  9781470403683 
Product Code:  MEMO/162/770.E 
List Price:  $61.00 
MAA Member Price:  $54.90 
AMS Member Price:  $36.60 
eBook ISBN:  9781470403683 
Product Code:  MEMO/162/770.E 
List Price:  $61.00 
MAA Member Price:  $54.90 
AMS Member Price:  $36.60 

Book DetailsMemoirs of the American Mathematical SocietyVolume: 162; 2003; 111 ppMSC: Primary 35; 51; Secondary 47
This investigation introduces a new description and classification for the set of all selfadjoint operators (not just those defined by differential boundary conditions) which are generated by a linear elliptic partial differential expression \[A(\mathbf{x},D)=\sum_{0\,\leq\,\left s\right \,\leq\,2m}a_{s} (\mathbf{x})D^{s}\text{ for all }\mathbf{x}\in\Omega\] in a region \(\Omega\), with compact closure \(\overline{\Omega}\) and \(C^{\infty }\)smooth boundary \(\partial\Omega\), in Euclidean space \(\mathbb{E}^{r}\) \((r\geq2).\) The order \(2m\geq2\) and the spatial dimension \(r\geq2\) are arbitrary. We assume that the coefficients \(a_{s}\in C^{\infty}(\overline {\Omega})\) are complexvalued, except real for the highest order terms (where \(\left s\right =2m\)) which satisfy the uniform ellipticity condition in \(\overline{\Omega}\). In addition, \(A(\cdot,D)\) is Lagrange symmetric so that the corresponding linear operator \(A\), on its classical domain \(D(A):=C_{0}^{\infty}(\Omega)\subset L_{2}(\Omega)\), is symmetric; for example the familiar Laplacian \(\Delta\) and the higher order polyharmonic operators \(\Delta^{m}\).
Through the methods of complex symplectic algebra, which the authors have previously developed for ordinary differential operators, the Stonevon Neumann theory of symmetric linear operators in Hilbert space is reformulated and adapted to the determination of all selfadjoint extensions of \(A\) on \(D(A)\), by means of an abstract generalization of the GlazmanKreinNaimark (GKN) Theorem. In particular the authors construct a natural bijective correspondence between the set \(\{T\}\) of all such selfadjoint operators on domains \(D(T)\supset D(A)\), and the set \(\{\mathsf{L}\}\) of all complete Lagrangian subspaces of the boundary complex symplectic space \(\mathsf{S}=D(T_{1})\,/\,D(T_{0})\), where \(T_{0}\) on \(D(T_{0})\) and \(T_{1}\) on \(D(T_{1})\) are the minimal and maximal operators, respectively, determined by \(A\) on \(D(A)\subset L_{2}(\Omega)\). In the case of the elliptic partial differential operator \(A\), we verify \(D(T_{0})=\overset{\text{o}}{W}{}^{2m}(\Omega)\) and provide a novel definition and structural analysis for \(D(T_{1})=\overset{A}{W}{}^{2m}(\Omega)\), which extends the GKNtheory from ordinary differential operators to a certain class of elliptic partial differential operators. Thus the boundary complex symplectic space \(\mathsf{S}= \overset{A}{W}{}^{2m}(\Omega)\,/\,\overset{\text{o}}{W}{}^{2m}(\Omega)\) effects a classification of all selfadjoint extensions of \(A\) on \(D(A)\), including those operators that are not specified by differential boundary conditions, but instead by global (i.e. nonlocal) generalized boundary conditions. The scope of the theory is illustrated by several familiar, and other quite unusual, selfadjoint operators described in special examples.
An Appendix is attached to present the basic definitions and concepts of differential topology and functional analysis on differentiable manifolds. In this Appendix care is taken to list and explain all special mathematical terms and symbols  in particular, the notations for Sobolev Hilbert spaces and the appropriate trace theorems.
An Acknowledgment and subject Index complete this Memoir.
ReadershipGraduate students and research mathematicians interested in partial differential equations and geometry.

Table of Contents

Chapters

1. Introduction: organization of results

2. Review of Hilbert and symplectic space theory

3. GKNtheory for elliptic differential operators

4. Examples of the general theory

5. Global boundary conditions: modified Laplace operators


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This investigation introduces a new description and classification for the set of all selfadjoint operators (not just those defined by differential boundary conditions) which are generated by a linear elliptic partial differential expression \[A(\mathbf{x},D)=\sum_{0\,\leq\,\left s\right \,\leq\,2m}a_{s} (\mathbf{x})D^{s}\text{ for all }\mathbf{x}\in\Omega\] in a region \(\Omega\), with compact closure \(\overline{\Omega}\) and \(C^{\infty }\)smooth boundary \(\partial\Omega\), in Euclidean space \(\mathbb{E}^{r}\) \((r\geq2).\) The order \(2m\geq2\) and the spatial dimension \(r\geq2\) are arbitrary. We assume that the coefficients \(a_{s}\in C^{\infty}(\overline {\Omega})\) are complexvalued, except real for the highest order terms (where \(\left s\right =2m\)) which satisfy the uniform ellipticity condition in \(\overline{\Omega}\). In addition, \(A(\cdot,D)\) is Lagrange symmetric so that the corresponding linear operator \(A\), on its classical domain \(D(A):=C_{0}^{\infty}(\Omega)\subset L_{2}(\Omega)\), is symmetric; for example the familiar Laplacian \(\Delta\) and the higher order polyharmonic operators \(\Delta^{m}\).
Through the methods of complex symplectic algebra, which the authors have previously developed for ordinary differential operators, the Stonevon Neumann theory of symmetric linear operators in Hilbert space is reformulated and adapted to the determination of all selfadjoint extensions of \(A\) on \(D(A)\), by means of an abstract generalization of the GlazmanKreinNaimark (GKN) Theorem. In particular the authors construct a natural bijective correspondence between the set \(\{T\}\) of all such selfadjoint operators on domains \(D(T)\supset D(A)\), and the set \(\{\mathsf{L}\}\) of all complete Lagrangian subspaces of the boundary complex symplectic space \(\mathsf{S}=D(T_{1})\,/\,D(T_{0})\), where \(T_{0}\) on \(D(T_{0})\) and \(T_{1}\) on \(D(T_{1})\) are the minimal and maximal operators, respectively, determined by \(A\) on \(D(A)\subset L_{2}(\Omega)\). In the case of the elliptic partial differential operator \(A\), we verify \(D(T_{0})=\overset{\text{o}}{W}{}^{2m}(\Omega)\) and provide a novel definition and structural analysis for \(D(T_{1})=\overset{A}{W}{}^{2m}(\Omega)\), which extends the GKNtheory from ordinary differential operators to a certain class of elliptic partial differential operators. Thus the boundary complex symplectic space \(\mathsf{S}= \overset{A}{W}{}^{2m}(\Omega)\,/\,\overset{\text{o}}{W}{}^{2m}(\Omega)\) effects a classification of all selfadjoint extensions of \(A\) on \(D(A)\), including those operators that are not specified by differential boundary conditions, but instead by global (i.e. nonlocal) generalized boundary conditions. The scope of the theory is illustrated by several familiar, and other quite unusual, selfadjoint operators described in special examples.
An Appendix is attached to present the basic definitions and concepts of differential topology and functional analysis on differentiable manifolds. In this Appendix care is taken to list and explain all special mathematical terms and symbols  in particular, the notations for Sobolev Hilbert spaces and the appropriate trace theorems.
An Acknowledgment and subject Index complete this Memoir.
Graduate students and research mathematicians interested in partial differential equations and geometry.

Chapters

1. Introduction: organization of results

2. Review of Hilbert and symplectic space theory

3. GKNtheory for elliptic differential operators

4. Examples of the general theory

5. Global boundary conditions: modified Laplace operators