1995
DOI: 10.1007/bf02070936
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SO(N) invariant Wess-Zumino action and its quantization

Abstract: A consistent quantization procedure of anomalous chiral models is discussed. It is based on the modification of the classical action by adding Wess-Zumino terms. The $SO(3)$ invariant WZ action for the $SO(3)$ model is constructed. Quantization of the corresponding modified theory is considered in details.Comment: 22 pages, LaTe

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Cited by 4 publications
(6 citation statements)
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“…In particular, there is no perturbative anomaly. This provides a cohomological interpretation of the Wess-Zumino anomaly cancellation mechanism [11,12,43]. By enlarging the original field space with the group elements g (if the complete gauge group is broken), the anomaly becomes trivial, i.e.…”
Section: Perturbation Theorymentioning
confidence: 99%
“…In particular, there is no perturbative anomaly. This provides a cohomological interpretation of the Wess-Zumino anomaly cancellation mechanism [11,12,43]. By enlarging the original field space with the group elements g (if the complete gauge group is broken), the anomaly becomes trivial, i.e.…”
Section: Perturbation Theorymentioning
confidence: 99%
“…But as was mentioned in the Introduction for some SU(N) groups this action can have degenerate symplectic form. This means that there are a number of additional primary constraints that can generate for example some secondary constraints and so on [14,15]. In this case one should modify the Faddeev-Shatashvili method to include the whole tower of the constraints.…”
Section: Anomalous Su(n) Yang-mills Modelmentioning
confidence: 99%
“…Due to the fact that WZ action is the first order one in its fields the symplectic form must be degenerate at least for all odd-dimensional groups such as SU(2k), dim SU(2k) = 4k 2 − 1. The particular case of two dimensional SU(2) and four dimensional SU(3)/SO(3) models was considered in [14,15]. In this paper we consider the general case of SU(N) group with degenerate symplectic form in four space-time dimensions.…”
Section: Introductionmentioning
confidence: 99%
“…28) and the corresponding anti-fields. In terms of new variables, all b * terms cancel out and we obtainS = Ŝ + dx [ Θ * {∂ α Θ Cα − ∂ α Cα } + Θ ′ * b ],(3.29)where Ŝ is S in which all fields and anti-fields are replaced by corresponding new ones.…”
mentioning
confidence: 99%
“…For YM type theories this possibility has been studied for example in[16][28] 4. The generalizations to reducible and on-shell theories may be examined by consulting[26].…”
mentioning
confidence: 99%