“…As expected for such a spin‐only system, fitting the data with CONDON 2.0 resulted in very similar parameters for J 1–3 , though the multiparameter fitting implementation in CONDON allows for a further refinement leading to a slight improvement in the quality of the fit, measured as ${SQ = \sqrt {\sum\nolimits_{i = 1}^n {([\chi _{obs} (i) - \chi _{calc} (i)]/\chi _{obs} (i))^2 } } }$ . Using standard values for the spin‐orbit coupling constant and the Racah parameters (ζ=347 cm −1 , B =960 cm −1 , C =3325 cm −1 ) for all three compounds, fitting to all data sets (Figure 9) yields for 8 : J 1 = J 2 =−1.17 cm −1 , J 3 =+0.13 cm −1 (SQ decreases from 2.2 % for the published fitted data43 to 1.7 %); for 9 : J 1 =−1.39 cm −1 , J 2 =−0.066 cm −1 , J 3 =+0.19 cm −1 (SQ decreases from 2.1 % to 0.8 %); for 10 : J 1 = J 2 =−0.32 cm −1 , J 3 =+0.045 cm −1 (SQ decreases from 1.5 % to 1.2 %). Similar measurements on Co II analogues of 8–10 are currently underway.…”