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Physical unitarity for massive non-abelian gauge theories in the Landau gauge: Stückelberg & Higgs

Ruggero Ferrari1 and Andrea Quadri2

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We discuss the problem of unitarity for Yang-Mills theory in the Landau gauge with a mass term à la Stückelberg. We assume that the theory (non-renormalizable) makes sense in some subtraction scheme (in particular the Slavnov-Taylor identities should be respected!) and we devote the paper to the study of the space of the unphysical modes. We find that the theory is unitary only under the hypothesis that the 1-PI two-point function of the vector mesons has no poles (at p2 = 0). This normalization condition might be rather crucial in the very definition of the theory. With all these provisos the theory is unitary. The proof of unitarity is given both in a form that allows a direct transcription in terms of Feynman amplitudes (cutting rules) and in the operatorial form. The same arguments and conclusions apply verbatim to the case of non-abelian gauge theories where the mass of the vector meson is generated via Higgs mechanism. To the best of our knowledge, there is no mention in the literature on the necessary condition implied by physical unitarity.


Keywords

BRST Quantization

Renormalization Regularization and Renormalons

BRST Symmetry

Gauge Symmetry

PACS

11.15.-q Gauge field theories

11.10.Gh Renormalization

14.40.-n Mesons

Subjects

Particle physics and field theory

Dates

Issue 11 (November 2004)

Received 30 August 2004, accepted for publication 9 November 2004

Published 2 December 2004



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