Variation in action for modified EM Field Action

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SUMMARY

The discussion focuses on the variation of the action in Lagrangian Field Theory, specifically examining the action S = \frac{1}{4}\int d^{4}x F_{\mu\nu}F^{\mu\nu}. The user explores the variation of the potential A_{\mu} under a gauge transformation A_{\mu} \rightarrow A_{\mu} + \partial_{\mu}\Phi, concluding that the variation in the action, \delta S, equals zero. This result indicates the invariance of the Lagrangian under gauge transformations, affirming that changes in the potential do not affect the physical fields or particle trajectories.

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  • Understanding of Quantum Field Theory (QFT)
  • Familiarity with Lagrangian Field Theory
  • Knowledge of gauge transformations
  • Basic concepts of tensor calculus in four-dimensional spacetime
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This discussion is beneficial for students and researchers in theoretical physics, particularly those focusing on Quantum Field Theory, Lagrangian mechanics, and gauge theories.

maverick280857
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Hi everyone

I am teaching myself QFT, and am currently learning Lagrangian Field Theory. Here is a question I am trying to solve, and I am not absolutely sure if my solution is correct because I am new to this notation and material. I would be grateful if someone could go over it and let me know if its correct. This isn't homework.

Also, I'd like to know what the significance of this result is, if it is indeed true.

Question: Consider the action [itex]S = \frac{1}{4}\int d^{4}x F_{\mu\nu}F^{\mu\nu}[/itex]. Vary the potential according to [itex]A_{\mu} \rightarrow A_{\mu} + \partial_{\mu}\Phi[/itex] where [itex]\Phi[/itex] is a scalar field. Determine the variation in the action.

Solution:

[tex]\delta S = \frac{1}{4}\int d^{4}x (\delta F_{\mu\nu}F^{\mu\nu} + F_{\mu\nu}\delta F^{\mu\nu})[/tex]

[tex]\delta F_{\mu\nu}F^{\mu\nu} &=& \delta(\partial_{\mu}A_{\nu}-\partial_{\nu}A_{\mu})F^{\mu\nu}[/tex]
[tex]\implies = (\partial_{\mu}\partial_{\nu}\Phi - \partial_{\nu}\partial_{\mu}\Phi)F^{\mu\nu} = 0[/tex]

Similarly [itex]F_{\mu\nu}\delta F^{\mu\nu} = 0[/itex]. Therefore [itex]\delta S = 0[/itex].

I have attached a pdf file, which contains this question and my working.
 

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I did not read your pdf-file, but your conclusion is correct. delta_S is equal to zero. Moreover, F_mu_nu does not vary. It is know as a "gauge" liberty, invariance of transformations. A_mu may be replaced by another A_mu in a certain way, but this does not change fields and particle trajectories. It is similar to the potential energy shifts U -> U+const in CM. The only thing that counts is the exchange, not the absolute value.

Bob.
 
Thanks bob. I see, so this is a gauge transformation under which the Lagrangian is invariant.
 

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