Describing relativistic fermions with two-component field

dc.creatorChen, YU-Qi
dc.date2004-09-03
dc.date.accessioned2026-07-07T03:53:20Z
dc.date.available2026-07-07T03:53:20Z
dc.descriptionWith a non-unitary transformation, the Lagrangian of a Dirac fermion is decomposed into two decoupled sectors. We propose to describe massive relativistic fermions in gauge theories in a two-component form. All relations between the Green's functions in this form and those in the conventional four-component form are derived. It is shown that the S-matrix elements in both forms are exactly the same. The description of the fermion in the new form simplifies significantly the gamma-matrix algebra in the four-component form. In particular, in perturbative calculations the propagator of the fermion is a scalar function. The advantages of the two-component form make it very useful in practical applications.
dc.description9 pages
dc.identifierhttps://arxiv.org/abs/hep-ph/0409027
dc.identifierhttp://arxiv.org/abs/hep-ph/0409027
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/43797
dc.subjectHigh Energy Physics - Phenomenology
dc.subjectHigh Energy Physics - Theory
dc.subjectNuclear Theory
dc.titleDescribing relativistic fermions with two-component field
dc.typetext

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