Premium
Kirchhoff's Rule for Quantum Wires. II: The Inverse Problem with Possible Applications to Quantum Computers
Author(s) -
Kostrykin V.,
Schrader R.
Publication year - 2000
Publication title -
fortschritte der physik
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.469
H-Index - 71
eISSN - 1521-3978
pISSN - 0015-8208
DOI - 10.1002/1521-3978(200008)48:8<703::aid-prop703>3.0.co;2-o
Subject(s) - unitarity , mathematics , hamiltonian (control theory) , quantum graph , boundary value problem , s matrix , unitary state , quantum , quantum mechanics , pure mathematics , mathematical analysis , physics , scattering , mathematical optimization , political science , law
In this article we continue our investigations of one particle quantum scattering theory for Schrödinger operators on a set of connected (idealized one‐dimensional) wires forming a graph with an arbitrary number of open ends. The Hamiltonian is given as minus the Laplace operator with suitable linear boundary conditions at the vertices (the local Kirchhoff law). In “Kirchhoff's rule for quantum wires” [J. Phys. A: Math. Gen. 32 , 595–630 (1999)] we provided an explicit algebraic expression for the resulting (on‐shell) S‐matrix in terms of the boundary conditions and the lengths of the internal lines and we also proved its unitarity. Here we address the inverse problem in the simplest context with one vertex only but with an arbitrary number of open ends. We provide an explicit formula for the boundary conditions in terms of the S‐matrix at a fixed, prescribed energy. We show that any unitary n × n matrix may be realized as the S‐matrix at a given energy by choosing appropriate (unique) boundary conditions. This might possibly be used for the design of elementary gates in quantum computing. As an illustration we calculate the boundary conditions associated to the unitary operators of some elementary gates for quantum computers and raise the issue whether in general the unitary operators associated to quantum gates should rather be viewed as scattering operators instead of time evolution operators for a given time associated to a quantum mechanical Hamiltonian. We also suggest an approach by which the S‐matrix in our context may be obtained from “scattering experiments”, another aspect of the inverse problem. Finally we extend our previous discussion, how our approach is related to von Neumann's theory of selfadjoint extensions.