Variation in action for modified EM Field Action

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The discussion centers on the variation of the action in Lagrangian Field Theory, specifically examining the action S = (1/4)∫ d^4x FμνFμν. The participant is exploring the variation of the potential Aμ under a gauge transformation Aμ → Aμ + ∂μΦ, where Φ is a scalar field. The conclusion reached is that the variation in the action, δS, equals zero, indicating that the field strength tensor Fμν remains invariant under this transformation. This invariance is recognized as a gauge freedom, similar to potential energy shifts in classical mechanics, emphasizing that the physical outcomes are unaffected by such transformations. The discussion highlights the importance of gauge invariance in field theories.
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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 S = \frac{1}{4}\int d^{4}x F_{\mu\nu}F^{\mu\nu}. Vary the potential according to A_{\mu} \rightarrow A_{\mu} + \partial_{\mu}\Phi where \Phi is a scalar field. Determine the variation in the action.

Solution:

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

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

Similarly F_{\mu\nu}\delta F^{\mu\nu} = 0. Therefore \delta S = 0.

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.
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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