Hi Ruairi,
as usual I replied much too quickly to this. After a chat with an actual card-carrying spectroscopist (name withheld since I might still mess things up), I found that I neglected a possibility that does access the 2Pi_1/2 state without resorting to SO coupling:
your perpendicular transition accessing the 2Pi_3/2:
2SIGMA(M_L=0, M_S = +1/2, M_J=+1/2) to 2Pi (M_L=+1, M_S=+1/2, M_J = +3/2) Delta_Omega=+1
the parallel transition I was thinking of that accesses the 2Pi_1/2 via SO:
2SIGMA(M_L=0, M_S = +1/2, M_J=+1/2) to 2Pi (M_L=+1, M_S=-1/2, M_J = +1/2) Delta_Omega=0
but there is this perpendicular transition that accesses the 2Pi_1/2 and should have the same TDM as the one accessing the 2Pi_3/2:
2SIGMA(M_L=0, M_S = +1/2, M_J=+1/2) to 2Pi (M_L=-1, M_S=+1/2, M_J = -1/2) Delta_Omega=-1
Maybe Dirac ignores this last one since it is the same as the first and then only shows the parallel transition?
regards, -Kirk