Relativistic Transport Theory for Systems Containing Bound States

dc.creatorRehberg, P.
dc.date1998-03-04
dc.date.accessioned2026-07-07T11:09:45Z
dc.date.available2026-07-07T11:09:45Z
dc.descriptionUsing a Lagrangian which contains quarks as elementary degrees of freedom and mesons as bound states, a transport formalism is developed, which allows for a dynamical transition from a quark plasma to a state, where quarks are bound into hadrons. Simultaneous transport equations for both particle species are derived in a systematic and consistent fashion. For the mesons a formalism is used which introduces off-shell corrections to the off-diagonal Green functions. It is shown that these off-shell corrections lead to the appearance of elastic quark scattering processes in the collision integral. The interference of the processes $q\bar q\toπ$ and $q\bar q\toπ\to q\bar q$ leads to a modification of the $s$-channel amplitude of quark-antiquark scattering.
dc.identifierhttps://arxiv.org/abs/hep-ph/9803239
dc.identifierhttp://arxiv.org/abs/hep-ph/9803239
dc.identifierPhys.Rev.C57:3299-3313,1998
dc.identifierdoi:10.1103/PhysRevC.57.3299
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/190578
dc.subjectHigh Energy Physics - Phenomenology
dc.titleRelativistic Transport Theory for Systems Containing Bound States
dc.typetext

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