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Homework Statement
Given the gauge invariant Dirac equation(i\hbar \gamma^\mu D_{\mu} - mc)\psi(x, A) = 0Show that the following holds: \psi(x, A - \frac{\hbar}{e} \partial\alpha) = e^{i\alpha}\psi(x, A)
Homework Equations
The covariant derivative is D_\mu = \partial_{\mu} + i\frac{e}{\hbar} A And the Dirac equation expanded gives (i\hbar \gamma^\mu \partial_{\mu} - mc)\psi(x, A) = e\gamma^\mu A_{\mu}(x)\psi(x, A)
The free field Feynman propagator S_{F}(x-x') satisfies (i\hbar \gamma^\mu \partial_{\mu} - mc)S_{F}(x-x') = i\hbar\delta^{(4)}(x - x')
The Attempt at a Solution
So i separate the hamiltonian density of the system into the unperturbed and the interaction terms \mathcal{H} = \mathcal{H}_{0} + \mathcal{H}_{interaction}
giving \mathcal{H}_{0} = c\overline{\psi}(-i\hbar \gamma^\mu \partial_{\mu} + mc)\psi
and \mathcal{H}_{int} = e\overline{\psi}(\gamma^\mu A_{\mu})\psi
All i can quess now is that the interaction term should give a contribution to a perturbative series, but i fail to see and accomplish this. Also, where does the free field Feynman propagator come into play?