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More on Chiral Anomaly

  • Mira Dey
  • Jishnu Dey
Part of the Springer Series in Nuclear and Particle Physics book series (SSNUCLEAR)

Abstract

Start with the Dirac-Maxwell Lagrangian density. Let us consider
$$ \begin{gathered} \mathcal{L}{\text{ = }}\left( {1/4{{\text{e}}^2}} \right){F_{\mu \upsilon }}{F^{\mu \upsilon }} + \overline \psi i{\gamma _\mu }{D^\mu }\psi - m\overline \psi \psi \hfill \\{D^\mu } = {\partial _\mu } + {A_\mu } \hfill \\\end{gathered} $$
(4.1.1)

Keywords

Gauge Field Ward Identity Vector Current Grassmann Variable Chiral Anomaly 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

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Copyright information

© Springer-Verlag Berlin Heidelberg 1994

Authors and Affiliations

  • Mira Dey
    • 1
  • Jishnu Dey
    • 2
  1. 1.Lady Brabourne CollegeCalcuttaIndia
  2. 2.IFT-UNESPSão PauloBrasil

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