My definition of a left invariant vector field is one for which the equation $dL_xX = X$ is satisfied, where $X$ is the differentiable vector field and $x \in G$ where G is a Lie group.
Consider the two sides of the equation:
$L_y \circ x_t (p) = L_y(x_t(p)) = yx_t(p)$
$x_t \circ L_y (p) = x_t(L_y(p)) = x_t(yp))$
Why are these equal?