Green's function for adjoint Dirac Equation If $S_F(x-y)$ is the Green's function for the Dirac operator $(i\gamma^\mu\partial_\mu-m)$, that is, I assume the following matrix equation holds: $$ (i\gamma^\mu\partial_\mu-m)S_F(x-y)=i\delta(x-y) $$
The adjoint dirac equation is:
$$ -i\partial_\mu\bar{\psi}\gamma^\mu -m\bar\psi=0 $$
I am looking for the Green's function of the above equation, in terms of $S_F(x-y)$, that is, if $F[S]$ is some function of $S$ (may include complex conjugation, transposing, etc), then I am looking for such an $F[S]$ such that this equation holds:
$$ -i\partial_\mu F[S]\gamma^\mu -mF[S]=i\delta(x-y) $$
What I have done so far:


*

*Dagger this equation: $(i\gamma^\mu\partial_\mu-m)S_F(x-y)=i\delta(x-y)$ and get $$(-i\partial_\mu S_F(x-y)^\dagger \gamma^{\mu\dagger} - S_F(x-y)^\dagger m)=-i\delta(x-y)$$

*Multiply by $\gamma^0$ on the right to get: $$ (-i\partial_\mu [-\bar{S_F}(x-y)] \gamma^{\mu} - [-\bar{S_F}(x-y)] m)=i\delta(x-y)\gamma^0 $$

*So $[-\bar{S_F}(x-y)]$ almost solves this equation, except you get a factor of $\gamma^0$ on the right which I am not sure how to handle.

 A: The solution to the problem can be found in the nature of the propagator of the Dirac equation: it is a matrix with two spinor indices, i.e. 
$$S_F(x-y)=S_F(x-y)_{\alpha\beta}.$$
In step 2, you have treated the propagator as if it was a spinor with a single index, which is not correct. Avoiding this, but multiplying the equation by $\gamma^0$ from the left leaves you with the result 
$$F(S)=\gamma^0 S^\dagger \gamma^0=\bar{S}.$$
The last equality sign is consistent with the reference given in one of the comments and with the definition of the adjoint of a matrix discussed in this question. 
A: After thinking for a while I think it's easiest to treat this problem in momentum space. Then $$S(p) = \frac{p\!\!\!/ + m}{p^2 - m^2 + i\varepsilon}$$
and satisfies
$$(p\!\!\!/ - m)S(p) = 1.$$
Note that $S$ carries spinor indices.
Then from dagger on the above equation, $$S(p)^\dagger (p\!\!\!/ - m)^\dagger =1.$$
Now, $p\!\!\!/ = p_\mu \gamma^\mu$ and $p_\mu$is real, so $$p\!\!\!/^\dagger = p_\mu (\gamma^\mu)^\dagger = p_\mu \gamma^0 \gamma^\mu \gamma^0 = \gamma^0 p\!\!\!/ \gamma^0.$$
Therefore, $$S(p)^\dagger(\gamma^0 p\!\!\!/ \gamma^0 - m) = S(p)^\dagger \gamma^0(p\!\!\!/ +m)\gamma^0 = 1$$
so $S(p)^\dagger\gamma^0$ solves the adjoint Dirac equation with unit source.
A: Can we just multiply from the left with $\gamma^{0}$ then we would get ,
\begin{equation}
\left[-\gamma^{0}S_{F}(x-y)\gamma^{0}\right]\left(-i\partial_{\mu}\gamma^{\mu}-m\right)=i\delta(x-y)
\end{equation}
