The implementation of the MCD B term for non-degenerate cases and of the derivative transition moments for RI-CC2 in TURBOMOLE have been reported in Refs. 10 and 46, respectively. This has now been generalized for degenerate states by adding the ω m j [ Mj (ω j )t µ (-ω j )] contribution to B(0 → j) for j ∈ D j , and by keeping the magnetic field-derivatives of the eigenvector of state j orthogonal to the entire set D j according to Eq (18).