I have the Lagrangian L=−∂μϕI∂μϕI/2−m2ϕIϕI/2
where I=1,2,3 and I want to find 3 independent infinitesimal transformations that leave the action invariant. One of them is a SO(3) infinitesimal rotation by δθ,ϕ−>ϕ′=ϕ+δθϵabcnbϕc. Also, the lagrangian is invariant when I change the sign of the fields but I suppose that it is not an infinitesimal transformation. If I had compex fields I would have a U(1) symmetry but this doesn't work here. Any help or hint?