Quantization of Gauge theories ?

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SUMMARY

The discussion focuses on the quantization of gauge theories, specifically addressing the Hamiltonian formulation when the Lagrangian is defined as tr[F^{ab}F_{ab}]. It outlines two primary approaches for quantization: the sum over histories method, which relies solely on the Lagrangian, and the canonical approach that treats the potential A as the position coordinate to derive the Hamiltonian using the Legendre transform. Key references include "Quantization of Fields with Constraints" by D. M. Gitman and I.V. Tyutin, and "Quantization of Gauge Systems" by Henneaux and Teitelboim, which provide foundational insights into gauge quantization techniques.

PREREQUISITES
  • Understanding of gauge theories and their mathematical formalism
  • Familiarity with Lagrangian and Hamiltonian mechanics
  • Knowledge of Lie groups and their generators
  • Experience with differential forms and the Hodge Star operator
NEXT STEPS
  • Study the Legendre transform in the context of field theory
  • Explore the sum over histories approach in quantum mechanics
  • Review Dirac's method of quantization with constraints
  • Examine chapter 15 of "The Quantum Theory of Fields" by Steven Weinberg
USEFUL FOR

The discussion is beneficial for theoretical physicists, graduate students in quantum field theory, and researchers interested in the mathematical foundations of gauge theories and their quantization methods.

mhill
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Quantization of Gauge theories ??

Hi , i am trying to learn the math formalism of Gauge Theories

as far as i know they begin with the 1-form

A= \sum_{i} T^{i}A_{\mu}^{i}

where 'T_i ' are the generators of the Lie Group

then we define the 2-form F= dA + (1/2)[A,A]

and the equation of motion are dF =0 (exterior derivative of F ) and *d *F = J

with J being an external source and *F_{ij}=e_{ijkl}F^{kl} Hodge Star operator

QUESTION:
=========

How can you define a Hamiltonian of Your Gauge theory if the Lagrangian is equal to tr[F^{ab}F_{ab}]

how can you apply the Quantization to these theories ??
 
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mhill said:
How can you define a Hamiltonian of Your Gauge theory if the Lagrangian is equal to tr[F^{ab}F_{ab}]

how can you apply the Quantization to these theories ??
Two ways: one is the sum over histories approach which requires knowledge only of the Lagrangian.

The other is to treat the potential A as the "position" coordinate, so we can find the canonically conjugate momenta

\pi = \frac{\partial L}{\partial \dot{A}}

and then use the Legendre transform to get the Hamiltonian

H = \pi\partial_{0}A - L.

NOTE NOTE NOTE these are Lagrangian, Hamiltonian, and momentum DENSITIES and if you want to get the Lagrangian, Hamiltonian, or momentum you merely integrate the corresponding density over the spatial volume.

Usually you end up with constraints in the canonical approach and you either quantize then constrain (Dirac's approach) or constrain then quantize (reduced phase space approach). It's a whole problem...

A good book or two to refer to would be Quantization of Fields with Constraints by D. M. Gitman and I.V. Tyutin (the latter was the "T" in the BRST technique of gauge quantization), or Quantization of Gauge Systems by Henneaux and Teitelboim. The latter is a more difficult read (my notes consist of elucidating what they say, and providing more detailed proofs; it's very elegant but also very short and kinda choppy in the beginning in my opinion...).
 


Look at chapter 15 in Weinberg or Dirac's little primer "Lectures in quantum mechanics".
 

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