2000
DOI: 10.1088/0305-4470/33/49/302
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Hermitian symplectic geometry and the factorization of the scattering matrix on graphs

Abstract: Hermitian symplectic spaces provide a natural framework for the extension theory of symmetric operators. Here we show that hermitian symplectic spaces may also be used to describe the solution to the factorisation problem for the scattering matrix on a graph, ie. we derive a formula for the scattering matrix of a graph in terms of the scattering matrices of its subgraphs. The solution of this problem is shown to be given by the intersection of a Lagrange plane and a coisotropic subspace which, in an appropriat… Show more

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Cited by 44 publications
(77 citation statements)
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“…For more on this classical theory, see for example [32,33,41,55,66,67] and for its use to analyze second order regular singular operators, see [10, 11, 38-40, 49, 54, 56], and see Gil and Mendoza [24] and Lesch [44] for the analysis of more general Fuchs type or cone operators in the sense of Schulze [59,60]; finally, see [16] for applications of self-adjoint extensions to quantum physics.…”
Section: Hermitian Symplectic Formalism Of Self-adjoint Extensionsmentioning
confidence: 99%
“…For more on this classical theory, see for example [32,33,41,55,66,67] and for its use to analyze second order regular singular operators, see [10, 11, 38-40, 49, 54, 56], and see Gil and Mendoza [24] and Lesch [44] for the analysis of more general Fuchs type or cone operators in the sense of Schulze [59,60]; finally, see [16] for applications of self-adjoint extensions to quantum physics.…”
Section: Hermitian Symplectic Formalism Of Self-adjoint Extensionsmentioning
confidence: 99%
“…This correspondence is a direct consequence of von Neumann's classical theory of self-adjoint extensions; a partial list of relevant references is [33,34,35,65,81,86,80,69,70,72,77,78,79,80,90,93,104,105]. …”
Section: The Hermitian Symplectic Theory Of Self-adjoint Extensionsmentioning
confidence: 99%
“…However eigenvalues ±1 which coincide with the eigenvalues ±1 of S do not depend on k. All other eigenvalues tend to 1 as k → ∞. The high energy limit of S V (k) exists [4,5,8] and is given by…”
Section: Vertex Scattering Matricesmentioning
confidence: 97%