The many body problem in relativistic quantum mechanics

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dc.creatorMoshinsky, Marcos
dc.creatorNikitin, Anatoly
dc.date2005-02-03
dc.date.accessioned2026-07-07T11:04:43Z
dc.date.available2026-07-07T11:04:43Z
dc.descriptionWe discusse a relativistic Hamiltonian for an n-body problem in which all the masses are equal and all spins take value 1/2. In the frame of reference in which the total momentum $vP=0$, the Foldy-Wouthuysen transformation is applies and the positive energy part of the Hamiltonian is separated. The Hamiltonian with unharmonic oscillator potential is applied to describe mass differences for charmonium and bottonium states.
dc.identifierhttps://arxiv.org/abs/hep-ph/0502028
dc.identifierhttp://arxiv.org/abs/hep-ph/0502028
dc.identifierRev.Mex.Fis.50:66-73,2005
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/188985
dc.subjectHigh Energy Physics - Phenomenology
dc.subjectHigh Energy Physics - Theory
dc.titleThe many body problem in relativistic quantum mechanics
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