Abstract

We recalculate the chiral anomaly in the Abelian gauge model in which a spin-$\frac{1}{2}$ field is directly coupled to a Rarita-Schwinger spin-$\frac{3}{2}$ field, using the extended theory in which there is an exact fermionic gauge invariance. Since the standard gauge fixing and ghost analysis applies to this theory, the ghost contribution to the chiral anomaly is $-1$ times the standard chiral anomaly for spin-$\frac{1}{2}$. Calculation of the fermion loop Feynman diagrams contributing to the coupled model anomaly gives a result of $6$ times the standard anomaly, so the total anomaly is $5$ times the standard anomaly. This agrees with the result obtained from the unextended model taking the ghost contribution there as $0$, corresponding to a non-propagating ghost arising from exponentiating the second class constraint determinant, together with the fermion loop anomaly contribution in the unextended model of $5$ times the standard anomaly.

Highlights

  • In this paper we continue an ongoing investigation of whether3 2 theory can be consistently gauged when not coupled to supergravity

  • We find that the one Feynman diagram in the extended model that is analogous to the anomalous triangle in the unextended model has an anomaly of times the standard spin

  • 1 2 field to which the Rarita-Schwinger field is coupled with coupling mass m, and Λ is the auxiliary field introduced in [1] that restores exact fermionic gauge invariance

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Summary

INTRODUCTION

3 2 theory can be consistently gauged when not coupled to supergravity. For the minimal gauged spin-. 1 2 fermion field, in which the weak field singularity is removed, and a perturbation theory calculation of the chiral anomaly is possible For this coupled model, the chiral anomaly arising from fermion triangle diagrams was found to be times the standard spin-. Our metric and gamma matrix conventions, and some useful identities, are given in the Appendix

COVARIANT AND LEFT CHIRAL ACTIONS
PATH INTEGRAL
FEYNMAN RULES FOR PROPAGATORS AND VERTICES
ENUMERATION OF DIAGRAMS
ANOMALY ARISING FROM THE LEADING ORDER NOETHER CURRENT TRIANGLE
The anomaly arising from diagram IA
ANOMALY CONTRIBUTIONS ARISING FROM THE REMAINING DIAGRAMS
VIII. DISCUSSION
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