5A redefinition of the form Λ cΛ by a real constant c corresponds to a redefinition of the coupling of the form 1g2 1g2 c where c is another constant, or equivalently g2 g2 + cg4 + . Therefore this is a redefinition starting at the one-loop order, keeping the leading order definition of g2 fixed. In this lecture note, we do not track such finite renormalization of the coupling very carefully.