Consider the non-relativistic limit of the matrix element (2.356) for an e− in a static external field.
(a) Compute the limit to linear order in the momenta. Hint: use the explicit forms for the spinors in the Pauli-Dirac representation. It simplifies the calculation to rewrite uˉ2Γμu1 using the Gordon decomposition.
(b) Suppose that Γμ(p2,p1) in (2.352) contained a term 2miσμνqνγ5G2(q2). This violates P and T but in principle could be generated by a new interaction. Show how G2(0) is related to the electric dipole moment de of the electron, which is defined by the non-relativistic interaction HEDM=−de⋅E(x), where E is an external electric field. Note that the Hermiticity condition (2.354) requires that G2 is pure imaginary.