Lattice dynamics of layered transition-metal dihalides

Abstract
We present an extended-shell-model (ESM) calculation of the dispersion relations and of the phonon density of crystals with either CdI2 or CdCl2 structure, namely, of V, Mn, Fe, Co, and Ni dichlorides and dibromides. The dynamical matrix, including the Coulomb and short-range contributions originating from the anion static dipoles, is constructed from model interionic potentials. While anion-anion Born-Mayer repulsion and van der Waals interactions are taken as in alkali halides, the parameters of metal-halogen short-range potential are obtained from equilibrium nearest-neighbor distance and cohesive energy. To this purpose we have derived an expression for the cohesive energy suitable to crystals with reduced ionicity and open d-shell configurations. A transverse metal-metal force constant and a correction to the transverse anion-anion interlayer force constant are added in order to fulfill the rotational invariance conditions. The three electrostatic parameters, net charge Z, anion shell charge Y, and anion shell-core displacement w0, are adjustable and are best-fitted to the experimental Raman and far-infrared data. A reliable scale of ionicities ranging from Z=0.71 of NiBr2 to 0.91 of MnCl2 is obtained, and the theoretical dynamical charges and elastic constants are reported. The calculated dispersion curves are in good agreement with the few available neutron data. For MnCl2, where a complete comparison with neutron data is possible, we show how the various ESM contributions influence the dynamical anisotropy and the lattice stability. Finally, we discuss the role of central metal-metal interaction, three-body forces, monopolar and quadrupolar metal-ion breathing (all neglected in the calculations) in order to explain the residual discrepancies.