I'm trying to prove that for any harmonic function $u$, we have :
let $ \Omega \subset \mathbb{R}^2$ and $ \overline B(0,R) \subset \Omega $
$$ u \colon \Omega \to \mathbb R $$
$$\forall z \in B(0,R) : u(z) = \Re \ \ \frac 1 {2 \pi i}\int_{ |\zeta| = R } \frac{ \zeta+z}{ \zeta ( \zeta -z)} u( \zeta ) d\zeta $$
I've tried a few things:
I've shown that $$ \int_{|\zeta| = R } \frac{ \zeta+z}{ \zeta ( \zeta -z)} u( \zeta ) d\zeta = 2 \int_{|\zeta| = R } \frac{ u( \zeta ) }{ ( \zeta -z)} d\zeta - \int_{|\zeta| = R } \frac{ u( \zeta ) }{ \zeta} d\zeta $$
Which ( I'm not sure about this point... but in complex analysis I think it would have made sense ) is proportional to
$$ 2 \operatorname{Res}_z(u) - \operatorname{Res}_0(u) $$
But I don't think I'm going anywhere ...
So I started again and I studied the function :
$$L_f(z) = \frac 1 {2 \pi i}\int_{ \mathbb{T} } \frac{ \zeta+z}{ \zeta ( \zeta -z)} f( \zeta ) d\zeta$$
I would still need to prove that this is holomorphic, but the derivative is given by :
$$L'_f(z) = \frac 1 { \pi i}\int_{ \mathbb{T} } \frac{ f( \zeta ) }{ ( \zeta -z)^2 }d\zeta$$
I was very surprised because the RHS is exactly the expression of $ 2 f'(z) $ according to Cauchy Integral Formula. So I was believing that $L_f \equiv f$. But in order to prove the equality, I would still need to prove that :
$$- \int_{ \mathbb{T} } \frac{ f( \zeta ) }{ \zeta} d\zeta = \frac 1 { \pi i}\int_{ \mathbb{T} } \frac{ f( \zeta ) }{ \zeta -z }d\zeta $$
So could you please tell me if my reasoning is true/ going somewhere, if I'm allowed to talk about residues for harmonic functions... Or if you have another solution for the main problem, I would also be very grateful to read it :)