After beta decay the daughter nucleus is often left in an excited state. This nucleus will then usually de-excite by means of an electromagnetic transition in which a gamma ray is emitted. The theory of such electromagnetic processes is contained in Maxwell's equations. These equations can be expressed in terms of a vector potential (I) and a scalar po tential ((j)). Nuclear states have a definite angular momentum and parity because the nuclear Hamiltonian is invariant under rotations and reflections. Using this fact, it is advisable to carry out a multipole expansion of the vector potential (A). Once this is done it is the multipole potential which