Given the following Lagrangian of a scalar field $$ L = +i \psi^*\partial_t\psi - \frac{1}{2m} \nabla \psi^* \cdot \nabla \psi, $$ I want to compute the equation(s) of motion. First by varying wrt $\psi^*$ and then wrt $\psi$.
First I say $$\frac{\partial L}{\partial \psi^{*}} = + i\partial_t\psi$$ and $$\partial_{\mu} (\frac{\partial L}{\partial (\partial_{\mu} \psi^*)}) = \partial_{t} (\frac{\partial L}{\partial (\partial_{t} \psi^*)}) + \nabla(\frac{\partial L}{\partial (\nabla \psi^*)}) = 0 - \frac{1}{2m}\nabla^2 \psi. $$ By Euler -Lagrange I get
$$ i \frac{\partial \psi}{\partial t} = - \frac{1}{2m} \nabla^2 \psi. $$
Now if I do the same but vary to $\psi$ instead of $\psi^*$, I get $$ i \psi^* = +\frac{1}{2m} \nabla^2 \psi^{*}, $$ as equation of motion. The only main difference is that $$\frac{\partial L}{\partial \psi} = 0.$$
Could someone verify if the answers are correct please?
The last equation is not a typo.But something feels weird, therefore I'd appreciate a verification. '
EDIT: Solved, my mistake was that I only considered $(\frac{\partial L}{\partial (\partial_{t} \psi)}) = i \psi^*$, instead of $\partial_{t} (\frac{\partial L}{\partial (\partial_{t} \psi)}) = i \frac{\partial \psi^{*}}{\partial t}$.