On the quark propagator singularity

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dc.creatorSauli, V.
dc.date2007-04-19
dc.date2007-10-31
dc.date.accessioned2026-07-07T08:39:21Z
dc.date.available2026-07-07T08:39:21Z
dc.descriptionUsing the method of Fukuda and Kugo \cite{FUKKUG} the continuation of Euclidean solution is performed to the timelike axis of fourmomenta. It is shown that assumed presence of the real simple pole in quark propagator is not in agreement with the solution. The simple pole disappears because of the discontinuity in the resulting quark mass function.
dc.description4pp, 4 fig
dc.identifierhttps://arxiv.org/abs/0704.2566
dc.identifierhttp://arxiv.org/abs/0704.2566
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/141042
dc.subjectHigh Energy Physics - Phenomenology
dc.titleOn the quark propagator singularity
dc.typetext

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