How to get from representations to finite or infinitesimal transformations?

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SUMMARY

This discussion focuses on deriving infinitesimal transformations from the representation of a Lie algebra related to symmetry groups in theoretical physics. The user seeks to calculate Noether currents using the fields in their Lagrangian, specifically transitioning from finite transformations to infinitesimal ones. Key steps involve identifying the generators of the algebra, represented as matrices, and utilizing the formula g[q] = exp(iqaTa) to express group-valued transformations. The conversation emphasizes the importance of understanding both the finite and infinitesimal forms of these transformations.

PREREQUISITES
  • Understanding of Lie algebra representations
  • Familiarity with Noether's theorem and currents
  • Knowledge of group theory and transformations
  • Basic concepts of quantum field theory and Lagrangians
NEXT STEPS
  • Study the derivation of Noether currents from Lagrangian symmetries
  • Learn about the matrix representation of Lie algebras
  • Explore the relationship between finite and infinitesimal transformations
  • Investigate specific examples of symmetry groups in quantum field theory
USEFUL FOR

The discussion is beneficial for theoretical physicists, particularly those working with quantum field theory, as well as graduate students studying advanced topics in symmetry and group theory.

confusio
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Hi all. I have here a reference with a representation of the Lie algebra of my symmetry group in terms the fields in my Lagrangian. In order to calculate Noether currents, I would like to use this representation to derive formulae for the infinitesimal forms of the symmetry transformations described by the elements of the Lie algebra. I know how to get from the finite forms of the transformations to the infinitesimal ones, so those would be great too. Does anybody know how to get from the representation of the algebra to the actual transformations?

Thanks so much for reading.
 
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confusio said:
... with a representation of the Lie algebra of my symmetry group in terms the fields in my Lagrangian. ... Does anybody know how to get from the representation of the algebra to the actual transformations?
As far as I understand it you have fields like Aa(x) where a is the algebra-index. Now you want to find the transformation from A(x) to A'(x), correct?

So what you need is the finite transformation. They can be represented via the matrix representation. So you have to find generators of you algebra, i.e. matrices Ta which form a basis of the algebra in some representation (fermions usually in the fundamental rep., bosons like photons, gluons, ... usually in the adjoint rep.). The group-valued transformations are generated as

g[q] = exp iqaTa with qa=qa(x)
 

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