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Homework Statement
Given the Lagrangian
[tex]
L = -\frac{1}{2}\partial_{\alpha}A_{\beta}\partial^{\alpha}A^{\beta} + \frac{1}{2}\partial_{\alpha}A^{\alpha}\partial_{\beta}A^{\beta} + \frac{\mu^2}{2}A_{\beta}A^{\beta}[/tex]
show that A satisfies the Lorentz condition [itex]\partial_{\alpha}A^{\alpha} = 0[/itex].
Homework Equations
The Attempt at a Solution
I want to say we can treat [itex]\partial_{\alpha}A^{\alpha}[/itex] as an independent field, and find the appropriate field equations for it, but I'm not sure if that makes sense. Any thoughts?