Supercharge Operator of Hidden Symmetry in the Dirac Equation

dc.creatorKhachidze, Tamari~T.
dc.creatorKhelashvili, Anzor~A.
dc.date2006-02-18
dc.date.accessioned2026-07-07T12:30:39Z
dc.date.available2026-07-07T12:30:39Z
dc.descriptionAs is known, the so-called Dirac $K$-operator commutes with the Dirac Hamiltonian for arbitrary central potential $V(r)$. Therefore the spectrum is degenerate with respect to two signs of its eigenvalues. This degeneracy may be described by some operator, which anticommutes with $K$. If this operator commutes with the Dirac Hamiltonian at the same time, then it establishes new symmetry, which is Witten's supersymmetry. We construct the general anticommuting with $K$ operator, which under the requirement of this symmetry unambiguously select the Coulomb potential. In this particular case our operator coincides with that, introduced by Johnson and Lippmann many years ago.
dc.description3 pages
dc.identifierhttps://arxiv.org/abs/hep-th/0602181
dc.identifierhttp://arxiv.org/abs/hep-th/0602181
dc.identifierGESJ Phys.1:88-97,2006; AIP Conf.Proc.881:279-284,2007
dc.identifierdoi:10.1063/1.2435304
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/216196
dc.subjectHigh Energy Physics - Theory
dc.titleSupercharge Operator of Hidden Symmetry in the Dirac Equation
dc.typetext

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