The lowest-lying X
1
+, a
3![](/images/gifchars/Phi.gif)
, b
3![](/images/gifchars/Pi.gif)
, c
5![](/images/gifchars/Delta.gif)
, A
1![](/images/gifchars/Phi.gif)
, and B
1![](/images/gifchars/Pi.gif)
electronic states of CoN have been investigated at the
ab initio MRCI and MS-CASPT2 levels, with extended atomic basis sets and inclusion of scalar relativisticeffects. Among the singlet states, the A
1![](/images/gifchars/Phi.gif)
and B
1![](/images/gifchars/Pi.gif)
states have been described for the first time. Potentialenergy curves, excitation energies, spectroscopic constants, and bonding character for all states are reported.Comparison with other early transition-metal nitrides (ScN, TiN, VN, and CrN), isoelectronic (NiC) andisovalent (RhN and IrN) species has been made, besides analyzing the B
1
![](/images/entities/harr.gif)
X
1
+ electronic transition interms of Franck-Condon factors, Einstein coefficients, and radiative lifetimes. At both levels of theory, thefollowing energetic order has been obtained: X
1
+, a
3![](/images/gifchars/Phi.gif)
, b
3![](/images/gifchars/Pi.gif)
, c
5![](/images/gifchars/Delta.gif)
, A
1![](/images/gifchars/Phi.gif)
, and B
1![](/images/gifchars/Pi.gif)
, with good agreementwith experimental results. In contrast, previous DFT and MRCI calculations predicted the ground state to bethe
5![](/images/gifchars/Delta.gif)
state.