I have never learned well Fem, but I wanted to do spacetime finite elements for the Klein-Gordon equation : ##\frac{\partial^2\psi}{\partial x^2}-\frac{\partial^2\psi}{c^2\partial t^2}=\lambda\psi##.
Then I wanted to make the change of coordinates ##x'=ct-x,y'=x+ct## transforming the LHS in ##4\frac{\partial^2\psi'}{\partial x'\partial y'}=\lambda\psi'## ? if I'm not mistaken
Next step was to choose linear basis functions on squares such that their non zero value lie in ##x',y'\in[0,2ct] ## to respect the limit speed of ##c##. (I think now I should treat this with polar coordinates to be correct)
The usual integration by part to get the stiffness matrix is done and
Strangely it seems to give an eigenvalue problem and the eigenvalue ##\lambda=-\frac{m_0c^2}{\hbar^2}## gives a quantized mass ?
Also there is no initial state to give which seems strange to me.
But I don't know how to code this but rather compute the limit of the steps ##\Delta x'=\Delta y'\rightarrow 0## analytically.
I don't even know if it is a well posed problem nor if it converges.