If a group G is acting over a manifold M, every vector V∈g gives rise to a vector field V♯ in M in the following way: for every p∈M we consider the curve αpV(t)=p⋅etV. And we take V♯(p)=ddt(p⋅etV)|t=0. It is called the fundamental vector field.
They reflects the Lie algebra action.
When M is G itself, the fundamental vector field generated by V is the right invariant vector field RV. It is the same as the left invariant vector field generated by Adg−1V where Ad is the adjoint representation. See also Maurer-Cartan form#MC form and left and right actions.