Pressure effects on 3dⁿ (n = 4, 9) insulating compounds: Long axis switch in Na₃MnF₆ not due to the Jahn‐Teller effect

The pressure-induced switch of the long axis of MnF₆^3- units in the monoclinic Na₃MnF₆ compound and Mn³⁺-doped Na₃FeF₆ is explored with the help of first principles calculations. Although the switch phenomenon is usually related to the Jahn-Teller effect, we show that, due to symmetry reasons, it can hardly take place in 3dⁿ (n=4,9) systems displaying a static Jahn-Teller effect. By contrast , we prove that in Na₃MnF₆ the switch arises from the anisotropic response of the low symmetry lattice to hydrostatic pressure. Indeed, while the long axis of a MnF₆^3- unit at ambient pressure corresponds to the Mn³⁺-F₃^- direction , close to the crystal c axis, at 2.79 GPa the c axis is reduced by 0.29 Å while b is unmodified. This fact is shown to force a change of the HOMO wavefunction favoring that the long axis becomes the Mn³⁺-F₂^- direction, not far from crystal b axis, after the subsequent relaxation process. The origin of the different d-d transitions observed for Na₃MnF₆ and CrF₂ at ambient pressure is also discussed together with changes induced by pressure in Na₃MnF₆. The present work opens a window for understanding the pressure effects upon low symmetry insulating compounds containing d⁴ or d⁹ ions.