2008/07/10 by L. L. Salcedo · 1 citation
Physics and Astronomy · #Black Holes and Theoretical Physics #Particle physics theoretical and experimental studies #Quantum Chromodynamics and Particle Interactions #hep-th
paper · pdf · doi:10.1140/epjc/s10052-008-0782-4
published as Eur.Phys.J.C58:423-435,2008 · 15 pages
arxiv created 2008/07/10 · openalex publication_date 2008/10/25 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/29
The coupling of spin 0 and spin 1 external fields to Dirac fermions defines a theory which displays gauge chiral symmetry. Quantum mechanically, functional integration of the fermions yields the determinant of the Dirac operator, known as the chiral determinant. Its modulus is chiral invariant but not so its phase, which carries the chiral anomaly through the Wess-Zumino-Witten term. Here we find the remarkable result that, upon removal from the chiral determinant of this known anomalous part, the remaining chiral invariant factor is just the square root of the determinant of a local covariant operator of the Klein-Gordon type. This procedure bypasses the integrability obstruction allowing to write down a functional that correctly reproduces both the modulus and the phase of the chiral determinant. The technique is illustrated by computing the effective action in two dimensions at leading order in the derivative expansion. The results previously obtained by indirect methods are indeed reproduced.