A relativistic variant of the Wigner function

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dc.creatorMorgan, Peter
dc.date2003-04-28
dc.date2003-12-17
dc.date.accessioned2026-07-07T06:06:38Z
dc.date.available2026-07-07T06:06:38Z
dc.descriptionThe conventional Wigner function is inappropriate in a quantum field theory setting because, as a quasiprobability density over phase space, it is not manifestly Lorentz covariant. A manifestly relativistic variant is constructed as a quasiprobability density over trajectories instead of over phase space.
dc.descriptionv3: as accepted by Phys. Lett. A
dc.identifierhttps://arxiv.org/abs/quant-ph/0304171
dc.identifierhttp://arxiv.org/abs/quant-ph/0304171
dc.identifierPhys.Lett. A321 (2004) 216-224
dc.identifierdoi:10.1016/j.physleta.2003.12.029
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/91048
dc.subjectQuantum Physics
dc.subjectHigh Energy Physics - Theory
dc.titleA relativistic variant of the Wigner function
dc.typetext

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