The Lorentz groups act on the scalar fields as: $\phi'(x)=\phi(\Lambda^{-1} x)$
The conditions for an action of a group on a set are that the identity does nothing and that $(g_1g_2)s=g_1(g_2s)$. This second condition is not fulfilled because of the inverse on $\Lambda$. What is then the action of the Lorentz group on the scalar fields?
This post imported from StackExchange Physics at 2014-03-22 17:31 (UCT), posted by SE-user inquisitor