-1/2 Tr F_{\mu\nu} F^{\mu\nu}
for a suitably defined F. Or further abbreviated to something like L_g.
It just depends on how much detail you need to expose.
-1/2 Tr F_{\mu\nu} F^{\mu\nu}
for a suitably defined F. Or further abbreviated to something like L_g.
It just depends on how much detail you need to expose.