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M-matrix inverse problem for Sturm-Liouville equations on graphs Sonja Currie School of Mathematics University of the Witwatersrand Johannesburg South Africa Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs The

  1. M-matrix inverse problem for Sturm-Liouville equations on graphs Sonja Currie School of Mathematics University of the Witwatersrand Johannesburg South Africa Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  2. The inverse problem Consider a Sturm-Liouville boundary value problem on a graph with formally self-adjoint boundary conditions at the nodes. From the M-matrix associated with such a problem we recover, up to a unitary equivalence, the boundary conditions and the potential. Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  3. Procedure Find asymptotics for the M-matrix as the eigenparameter tends to negative infinity. Recover the boundary conditions up to a unitary equivalence from the M-matrix. Show the M-matrix is a Herglotz function. Prove that the poles of the M-matrix are at the eigenvalues of the associated BVP simple located on the real axis and the residue at a pole is a negative semi-definite matrix of rank equal to the multiplicity of the eigenvalue. Recover the potential. Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  4. Procedure Find asymptotics for the M-matrix as the eigenparameter tends to negative infinity. Recover the boundary conditions up to a unitary equivalence from the M-matrix. Show the M-matrix is a Herglotz function. Prove that the poles of the M-matrix are at the eigenvalues of the associated BVP simple located on the real axis and the residue at a pole is a negative semi-definite matrix of rank equal to the multiplicity of the eigenvalue. Recover the potential. Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  5. Procedure Find asymptotics for the M-matrix as the eigenparameter tends to negative infinity. Recover the boundary conditions up to a unitary equivalence from the M-matrix. Show the M-matrix is a Herglotz function. Prove that the poles of the M-matrix are at the eigenvalues of the associated BVP simple located on the real axis and the residue at a pole is a negative semi-definite matrix of rank equal to the multiplicity of the eigenvalue. Recover the potential. Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  6. Procedure Find asymptotics for the M-matrix as the eigenparameter tends to negative infinity. Recover the boundary conditions up to a unitary equivalence from the M-matrix. Show the M-matrix is a Herglotz function. Prove that the poles of the M-matrix are at the eigenvalues of the associated BVP simple located on the real axis and the residue at a pole is a negative semi-definite matrix of rank equal to the multiplicity of the eigenvalue. Recover the potential. Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  7. Procedure Find asymptotics for the M-matrix as the eigenparameter tends to negative infinity. Recover the boundary conditions up to a unitary equivalence from the M-matrix. Show the M-matrix is a Herglotz function. Prove that the poles of the M-matrix are at the eigenvalues of the associated BVP simple located on the real axis and the residue at a pole is a negative semi-definite matrix of rank equal to the multiplicity of the eigenvalue. Recover the potential. Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  8. Procedure Find asymptotics for the M-matrix as the eigenparameter tends to negative infinity. Recover the boundary conditions up to a unitary equivalence from the M-matrix. Show the M-matrix is a Herglotz function. Prove that the poles of the M-matrix are at the eigenvalues of the associated BVP simple located on the real axis and the residue at a pole is a negative semi-definite matrix of rank equal to the multiplicity of the eigenvalue. Recover the potential. Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  9. Procedure Find asymptotics for the M-matrix as the eigenparameter tends to negative infinity. Recover the boundary conditions up to a unitary equivalence from the M-matrix. Show the M-matrix is a Herglotz function. Prove that the poles of the M-matrix are at the eigenvalues of the associated BVP simple located on the real axis and the residue at a pole is a negative semi-definite matrix of rank equal to the multiplicity of the eigenvalue. Recover the potential. Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  10. Procedure Find asymptotics for the M-matrix as the eigenparameter tends to negative infinity. Recover the boundary conditions up to a unitary equivalence from the M-matrix. Show the M-matrix is a Herglotz function. Prove that the poles of the M-matrix are at the eigenvalues of the associated BVP simple located on the real axis and the residue at a pole is a negative semi-definite matrix of rank equal to the multiplicity of the eigenvalue. Recover the potential. Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  11. Procedure Find asymptotics for the M-matrix as the eigenparameter tends to negative infinity. Recover the boundary conditions up to a unitary equivalence from the M-matrix. Show the M-matrix is a Herglotz function. Prove that the poles of the M-matrix are at the eigenvalues of the associated BVP simple located on the real axis and the residue at a pole is a negative semi-definite matrix of rank equal to the multiplicity of the eigenvalue. Recover the potential. Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  12. History The first graph model was used in chemistry - 1930’s by L. Pauling. Development of the theory of differential operators on graphs is recent with most of the research in this area having been done in the last couple of decades. Multi-point boundary value problems and differential systems were studied far earlier then this. Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  13. History The first graph model was used in chemistry - 1930’s by L. Pauling. Development of the theory of differential operators on graphs is recent with most of the research in this area having been done in the last couple of decades. Multi-point boundary value problems and differential systems were studied far earlier then this. Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  14. History The first graph model was used in chemistry - 1930’s by L. Pauling. Development of the theory of differential operators on graphs is recent with most of the research in this area having been done in the last couple of decades. Multi-point boundary value problems and differential systems were studied far earlier then this. Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  15. Applications Many applications in physics, engineering and chemistry. Eg. scattering theory, quantum wires and quantum chaos, heat flows in a mesh, photonic crystals. For a survey of the physical systems giving rise to boundary value problems on graphs see P . Kuchment, Graph models for waves in thin structures, Waves in Random Media, 12 (2002) R1 -R24 and the bibliography thereof. Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  16. Applications Many applications in physics, engineering and chemistry. Eg. scattering theory, quantum wires and quantum chaos, heat flows in a mesh, photonic crystals. For a survey of the physical systems giving rise to boundary value problems on graphs see P . Kuchment, Graph models for waves in thin structures, Waves in Random Media, 12 (2002) R1 -R24 and the bibliography thereof. Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  17. Applications Many applications in physics, engineering and chemistry. Eg. scattering theory, quantum wires and quantum chaos, heat flows in a mesh, photonic crystals. For a survey of the physical systems giving rise to boundary value problems on graphs see P . Kuchment, Graph models for waves in thin structures, Waves in Random Media, 12 (2002) R1 -R24 and the bibliography thereof. Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  18. Graphs G denotes a directed graph with a finite number of edges, say K, each of finite length and having the path length metric. Each edge e i of length l i can thus be considered as the interval [ 0 , l i ] . Eg. 0 r ❅ e 3 ❅ ❅ ❘ ❅ ✛ ✘ ❅ r r l 1 ❅ ✛ l 4 e 4 l 3 ✻ � 0 ✚ ✙ e 2 e 1 0 � ✠ � r � � l 2 Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

  19. The differential equation With the above identification we can now consider ly := − d 2 y dx 2 + q ( x ) y = λ y , (1) where q is real valued and essentially bounded on the graph G , to be the system of differential equations − d 2 y i dx 2 + q i ( x ) y i = λ y i (2) for x ∈ [ 0 , l i ] and i = 1 , . . . , K . Here q i and y i are q and y restricted to e i . Sonja Currie M-matrix inverse problem for Sturm-Liouville equations on graphs

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