Problem
1) Prove that if the real and imaginary part of a holomorphic function are of class $C^2$, then they are harmonic.
2)Deduce from 1) that if $u(x,y) \in C^2$ is a function that admits a harmonic conjugate, then $u$ is harmonic.
My attempt
I could prove part 1) using the Cauchy-Riemann equations. I am having problems with 2): I am not suppose to use that holomorphic functions are analytic (which also means $u,v \in C^{\infty}$).
I want to show that $u_{xx}+u_{yy}=0.$
By hypothesis, $u$ is the real part of a holomorphic function $f(x+iy)=u(x,y)+iv(x,y).$
Using the Cauchy-Riemann equations, I have $$u_{xx}=v_{xy} \space;\space u_{yy}=-v_{yx}$$
I don't know how one can deduce from here that $\Delta u=0$. I would appreciate some help.
The Laplace operator $\nabla^2$ or $\Delta$ is simply $$ \nabla^2 = \Delta = \frac{\partial^2}{\partial x^2} + \frac{\partial^2}{\partial y^2} $$ so we want to show that $\Delta u = u_{xx} + u_{yy} = 0$. From your identities shown, $u_{xx} = v_{xy}$ and $u_{yy} = -v_{yx}$, we have $$ \Delta u = u_{xx} + u_{yy} = v_{xy} - v_{yx}. $$ Since $u\in C^2$, $v_{xy}$ and $-v_{yx}$ exist and are continuous. Schwarz's Theorem states that
Now the complex plane can be viewed as the two-dimensional Euclidean space $\mathbb{R}^2$. Therefore, $$ \Delta u = u_{xx} + u_{yy} = v_{xy} - v_{yx} = v_{xy} - v_{xy} = 0. $$