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Canonical expansion of {{\cal P}{\cal T}} -symmetric operators and perturbation theory

E Caliceti1 and S Graffi2

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Let H be any {{\cal P}{\cal T}} -symmetric Schrödinger operator of the type −planck2Δ + (x21 + sdotsdotsdot + x2d) + igW(x1, ..., xd) on L^2({\bb R}^d) , where W is any odd homogeneous polynomial and g\in{\bb R} . It is proved that {\cal P} H is self-adjoint and that its eigenvalues coincide (up to a sign) with the singular values of H, i.e., the eigenvalues of \sqrt{H^\ast H} . Moreover we explicitly construct the canonical expansion of H and determine the singular values μj of H through the Borel summability of their divergent perturbation theory. The singular values yield estimates of the location of the eigenvalues λj of H by Weyl's inequalities.


PACS

03.65.Ge Solutions of wave equations: bound states

03.65.Fd Algebraic methods

02.10.Ud Linear algebra

11.30.Er Charge conjugation, parity, time reversal, and other discrete symmetries

MSC

81Q05 Closed and approximate solutions to the Schrödinger, Dirac, Klein-Gordon and other quantum-mechanical equations

Subjects

Mathematical physics

Particle physics and field theory

Quantum information and quantum mechanics

Dates

Issue 6 (13 February 2004)

Received 8 September 2003

Published 28 January 2004



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