Covariant derivatives commutator - field strength tensor

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The discussion focuses on deriving the field strength tensor using the covariant derivatives' commutator. The participants analyze the expression [D_{\mu},D_{\nu}] and its components, noting that the terms involving partial derivatives and gauge fields do not cancel completely. The key result is that the remaining terms simplify to the expression for the field strength tensor, specifically showing that the derivatives act on the gauge fields A_{\mu} and A_{\nu}. The conclusion emphasizes that the non-canceling terms ultimately lead to the desired formulation of the field strength tensor. This analysis is crucial for understanding gauge theories in physics.
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Homework Statement


So I've been trying to derive field strength tensor. What to do with the last 2 parts ? They obviously don't cancel (or do they?)

Homework Equations

The Attempt at a Solution


[D_{\mu},D_{\nu}] = (\partial_{\mu} + A_{\mu})(\partial_{\nu} + A_{\nu}) - (\mu <-> \nu) = [\partial_{\mu},\partial_{\nu}] + [\partial_{\mu},A_{\nu}]+[A_{\mu},\partial_{\nu}] +[A_{\mu}, A_{\nu}] =
\partial_{\mu}A_{\nu} - \partial_{\nu} A_{\mu} + [A_{\mu},A_{\nu}] -A_{\nu} \partial_{\mu} + A_{\mu} \partial_{\nu}
 
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They are canceled by the first two terms when the derivative acts on whatever function the entire operator is acting on. What remains is just the derivative acting on the A fields.
 
Thank you
 

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