More on Chiral Anomaly

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


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


Gauge Field Ward Identity Vector Current Grassmann Variable Chiral Anomaly 
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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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