In contrast to well established experimental results of vibronic coupling effects in octahedral dn complexes with Eg ground states (Cu2+, Ag2+; Cr2+, Mn3+ etc.), not much useful material is available for the Jahn–Teller (JT) effect in orbital triplet ground states. The present study is concerned with this deficiency, providing data for octahedral halide model complexes with 3dn cations – in particular for TiIII, VIII and high-spin CoIII, NiIII with T2g and T1g ground states, which involve, to first-order, solely splitting of the π-antibonding t2g MOs. Besides experimental results – structural and spectroscopic, mainly from d–d spectra – data from computations are needed for a quantitative treatment of the Tg ⊗ (ɛg + τ2g) vibronic interaction as well as in the Eg ⊗ ɛg coupling case (MnIII, low-spin NiIII); DFT was the method of choice, if only critically selected outcomes are utilised. The theoretical bases of the treatment are the dn ligand field matrices in Oh, extended by the inclusion of lower-symmetry distortion parameters, and the conventional theory of vibronic coupling. Caution is needed when classifying the effects of interelectronic repulsion; DFT does not reproduce the magnitudes of the Racah parameters B, C, as deduced from the d–d spectra, properly – the presumed reasons are analysed. DFT even allows one to deduce reliable vibronic coupling constants via the analysis of orbitally degenerate excited states (CrIII, 4A2g ground state). The group-theoretical analysis of the interaction with the JT-active ɛg and τ2g modes yields D4h, D3d and D2h as the possible distortion symmetries in the case of a Tg ground state. The DFT-calculations give clear evidence, that the D4h stationary points represent the absolute minima in the Tg ⊗ (ɛg + τ2g) potential surface – in agreement with experiment, where available. For the first time, vibronic coupling constants, characterising JT splitting of ground and excited Tg states, can be presented for trivalent 3dn cations in octahedral halide ligand fields. They turn out to be smaller by a factor of almost 3 in comparison to those, which determine the coupling in σ-antibonding eg MOs.The tetragonal splitting of Tg states is typically only small, around 0.1 eV, and suggests that strain influences from a specific ligand arrangement and/or the presence of different ligands may modify the potential surface considerably. We have studied such effects via compounds AIMIIIF4, where an elastic strain induced by the host structure, and a binding strain, due to the simultaneous existence of (largely) terminal and of bridging ligands, are active. A novel strain model, in its interplay with JT coupling, is proposed and applied – using energies from the d–d spectra, structural results and data from DFT.Chloride complexes are only known for TiIII to FeIII; the rather small electronegativity already of CoIII suggests a reducing ligand-to-metal (3dn) electron transfer for n ≥ 6. Similarly, the low-lying ligand-to-metal charge transfer bands in the d–d spectra of the CuIIIF63− complex and the reduced Tg ⊗ ɛg coupling strength suggest a pronounced covalency of the CuIII–F, and, even more distinctly, of the CuIII–O bond, which is of interest for superconductivity. The NiIIIF63− polyhedron possesses a low-spin configuration in the elpasolite structure. The spectroscopic evidence and the DFT data indicate, that the minimum positions of the alternative a2A1g(a2Eg) and a4A2g (a4T1g) potential curves are only ≤0.02 eV apart, giving rise to interesting high-spin/low-spin phenomena. It is the strong Eg ⊗ ɛg as compared to the T1g ⊗ ɛg coupling, which finally stabilises a spin-doublet ground state in D4h.We think, that the selected class of solids is unique particularly for the study of Jahn–Teller coupling in T ground states, with model character for other systems. In our overview a procedure is sketched, which uses reliable computational results (here from DFT) for supplementing incomplete experimental data, and presents – on a semiquantitative scale – convincing statements, consistent with chemical intuition. It is also a pleading for ligand field theory, which rationalises d-d spectra in terms of chemical bonding; though the latter spectra provide frequently only rather coarse information, their assistance in the energy analysis is crucial.

We have investigated MIIIX63- polyhedra [MIII: T, V, Co; X: Cl, F] with π-antibonding T ground states by optical spectroscopy and by DFT calculations, which supply reliable structural and energetic informations, as long as the ligands can be considered to be approximately terminal as in the chosen A2′AMIIIX6 [A′, A: K+, Rb+, Cs+] solids of elpasolite structure. While in the case of TiIII and CoIII distinct splittings of the excited Eg state are observed, indicating that a T ⊗ ε-type Jahn–Teller distortion of the respective polyhedra is present, the d–d spectra are of cubic appearence in the case of VIII. Here, it is most likely the t2g2-t2g1eg1 configuration interaction via the two 3A2g states in D4h, which suppresses the T ⊗ ε vibronic coupling. Assuming a purely tetragonal Jahn–Teller interaction the linear coupling constant is consistently found to be of the magnitude Vε ≈ 0.8 (1) [F−] and 0.25 (5) [Cl−] eV Å−1, leading to only very small Jahn–Teller splittings of the T ground states, with dynamic polyhedron distortions at 298 K in the case of TiIII and CoIII. In comparison, the vibronic coupling in the excited Eg states is much more pronounced (A1 ≈ 2.0 (2) [F−]; 1.05 (5) [Cl−] eV Å−1). The Jahn–Teller splittings are considerably enhanced, if terminal and bridging ligands are simultaneously present in the polyhedron, as in solids AMIIIF4. The different covalent binding properties of the two types of ligands can be shown to be responsible for these effects.