Lagrangian, scalar or pseudo-scalar?

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SUMMARY

The discussion centers on the nature of the Lagrangian density in quantum field theory (QFT) and whether it can be a pseudo-scalar. It is established that the conventional requirement is for the Lagrangian density to be a scalar under the spacetime symmetry group, specifically the Poincaré group, along with CPT and gauge invariance. The implications of a pseudo-scalar Lagrangian density are explored, particularly its behavior as an eigenfunction of the parity operator. This topic is crucial for understanding the foundational principles of QFT in Minkowski spacetime.

PREREQUISITES
  • Understanding of quantum field theory (QFT)
  • Familiarity with the Poincaré group and its symmetries
  • Knowledge of scalar and pseudo-scalar fields
  • Basic principles of gauge invariance in physics
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  • Research the implications of scalar vs. pseudo-scalar fields in QFT
  • Study the role of the Poincaré group in quantum mechanics
  • Learn about parity transformations and their effects on physical theories
  • Explore gauge invariance and its significance in particle physics
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The discussion is beneficial for theoretical physicists, quantum field theorists, and students studying advanced physics concepts related to symmetries and field theories.

salparadise
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Hi,

My question is. Can in principle, a Lagrangian density for some theory be a pseudo-scalar. Normally people say that the Lagrangian needs to be a scalar, but it case it is a pseudo-scalar it would also be a eigaen function of the parity operator.

This topic could well be on the classical physics section, but as this is more relevant in quantum theory I decided to place it here.

Thanks
 
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The normal requirement is that the fields transform irreducibly under the spacetime symmetry group and that the lagrangian density is a scalar under the spacetime symmetry group. The symmetry requirement for QFT in Minkowski spacetime is restricted Poincare group plus CPT plus gauge invariance. The Lagrangian density should be a scalar wrt to the 3 altogether or each taken separately.
 

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