I encountered the concept of "dynamic mass moment" also called "the boost angular momentum" and I am looking for a simple example.
I take as definition (p.18) $$ \vec{N} = (ct)\vec{p} -(E/c)\vec{x}. $$
Is it allowed to just consider the ground state electron in the Bohr model?
$ \vec{x} = (r \cos{\omega t}, r \sin{\omega t}, 0) $
$ ct\vec{p} = ( -mvct \sin{\omega t}, mvct \cos{\omega t}, 0) $
$v=\alpha c \quad (\alpha\approx 1/137)$
$p=mv=m\alpha c$
$E/c = \sqrt{m^2c^4 + p^2c^2} /c = mc\sqrt{1+\alpha^2}$
The result is $$\vec{N}= mc \\ (-\alpha ct \sin{\omega t - r \sqrt{1+\alpha^2} \cos{\omega t}}, \\ \quad \quad \alpha ct \cos{\omega t - r \sqrt{1+\alpha^2} \sin{\omega t}}, 0). $$
I have no idea what, in this simple example, $\vec{N}$ should mean, esp. the variable $t$ which will just grow to infinity?
In the end it will become just $(ct)\vec{p}$ with an infitely large modulus?
In contrast the angular momentum $L=\vec{r}\times\vec{p} = (0,0, m\alpha c r (\cos{}^2+\sin{}^2)) = (0,0,\hbar)$ is straightforward.