The action principle in quantum theory

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SUMMARY

The discussion centers on the action principle in quantum theory, specifically regarding the deduction of conserved current equations and symmetry transformations from the effective action in the path integral formalism. It is established that the effective action serves as the quantum counterpart to classical Lagrangian mechanics, and that Ward identities are essential for quantized charge conservation. The construction of conserved charges occurs at the classical level prior to quantization, and it is crucial to demonstrate that operator identities persist without anomalies in quantum field theory.

PREREQUISITES
  • Understanding of effective action in quantum field theory
  • Familiarity with path integral formalism
  • Knowledge of Ward identities and their role in charge conservation
  • Basic concepts of classical Lagrangian mechanics
NEXT STEPS
  • Study the derivation of effective action in quantum field theory
  • Learn about the implications of Ward identities in quantum mechanics
  • Explore the relationship between classical and quantum conserved quantities
  • Investigate anomalies in operator identities within quantum field theory
USEFUL FOR

Physicists, particularly those specializing in quantum field theory, theoretical physicists interested in the foundations of quantum mechanics, and students seeking to deepen their understanding of the action principle and its applications in quantum theories.

Dyson
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Hello!

I wonder is there exist a way to deduct the conserved current equation, generator of

the symmetry transformation and so on from a total quantum L with the help of action

principle?

Many books i have seen deduct the physical quantity from the classical L or construct

the quantum generator from the comparasion with classical one.


Thanks for reply!
 
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What you call "quantum L" is called effective action in the path integral formalism. There are so-called Ward-identities corresponding to a "quantized charge conservation". But the construction of the conserved charge is always done before quantization = at the classical level.

Within quantum (field) theory one has to proof that the corresponding operator identities / Ward-identities continue to exist w/o anomaly.

The path integral formalism is rather close to the classical one when it comes to conserved quantities as it is based on an action integral, no operators.
 
tom.stoer said:
What you call "quantum L" is called effective action in the path integral formalism. There are so-called Ward-identities corresponding to a "quantized charge conservation". But the construction of the conserved charge is always done before quantization = at the classical level.

Within quantum (field) theory one has to proof that the corresponding operator identities / Ward-identities continue to exist w/o anomaly.

The path integral formalism is rather close to the classical one when it comes to conserved quantities as it is based on an action integral, no operators.

Thanks! You give me a guide to learn more knowledge on effective action!
 

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