2002
DOI: 10.1017/s1446181100008014
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Inverse scattering for the matrix Schrödinger operator and Schrödinger operator on graphs with general self-adjoint boundary conditions

Abstract: Using a parameterisation of general self-adjoint boundary conditions in terms of Lagrange planes we propose a scheme for factorising the matrix Schrodinger operator and hence construct a Darboux transformation, an interesting feature of which is that the matrix potential and boundary conditions are altered under the transformation. We present a solution of the inverse problem in the case of general boundary conditions using a Marchenko equation and discuss the specialisation to the case of a graph with trivial… Show more

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Cited by 51 publications
(72 citation statements)
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“…It is convenient to consider the Schrödinger operator on the graph with n rays as a matrix operator, with diagonal potential, see [8,9]. Let us consider the matrix of n solutions of Schrödinger equation LΞ = λΞ on the graph satisfying the following boundary conditions at the origin…”
Section: The Schrödinger Operator On the Graph With Trivial Compact Partmentioning
confidence: 99%
“…It is convenient to consider the Schrödinger operator on the graph with n rays as a matrix operator, with diagonal potential, see [8,9]. Let us consider the matrix of n solutions of Schrödinger equation LΞ = λΞ on the graph satisfying the following boundary conditions at the origin…”
Section: The Schrödinger Operator On the Graph With Trivial Compact Partmentioning
confidence: 99%
“…Results of [1] are extended by Harmer [9] to arbitrary selfadjoint boundary conditions at origin, and then it becomes possible to treat the operator on noncompact star graphs as a specialization to the case of operator with diagonal matrix potential.…”
Section: Introductionmentioning
confidence: 99%
“…The article [17] considers a star-shaped graph consisting of N infinite branches and solves the inverse scattering problem assuming the measurement of N − 1 reflection coefficients. Next, in [18], Harmer provides an extension of the previous result with general self-adjoint boundary conditions at the central node.…”
Section: Introductionmentioning
confidence: 99%