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Relativistic two-body system in (1 + 1) dimensions

Norman Dombey1 and Fuad M Saradzhev2

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The relativistic two-body system in (1+1)-dimensional quantum electrodynamics is studied. It is proved that the eigenvalue problem for the two-body Hamiltonian without the self-interaction terms reduces to the problem of solving a one-dimensional stationary Schrödinger-type equation with an energy-dependent effective potential which includes the δ-functional and inverted oscillator parts. The conditions determining the metastable energy spectrum are derived, and the energies and widths of the metastable levels are estimated in the limit of large particle masses. The effects of the self-interaction are discussed.


PACS

03.65.Pm Relativistic wave equations

02.30.Sa Functional analysis

02.30.Em Potential theory

03.65.Ge Solutions of wave equations: bound states

MSC

34L40 Particular operators (Dirac, one-dimensional Schrödinger, etc.)

81V10 Electromagnetic interaction; quantum electrodynamics

81V70 Many-body theory; quantum Hall effect

Subjects

Mathematical physics

Quantum information and quantum mechanics

Dates

Issue 24 (23 June 2000)

Received 12 October 1999, in final form 25 April 2000



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    Norman Dombey and Fuad M Saradzhev 2000 J. Phys. A: Math. Gen. 33 4491

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