Pressure-Induced Phase Transformations of Quasi-2D Sr(3)Hf(2)O(7)

[Image: see text] We present an abinitio study of the quasi-2D layered perovskite Sr(3)Hf(2)O(7) compound, performed within the framework of the density functional theory and lattice dynamics analysis. At high temperatures, this compound takes a I4/mmm centrosymmetric structure (S.G. n. 139); as the temperature is lowered, the symmetry is broken into other intermediate polymorphs before reaching the ground-state structure, which is the Cmc2(1) ferroelectric phase (S.G. n. 36). One of these intermediate polymorphs is the Ccce structural phase (S.G. n. 68). Additionally, we have probed the C2/c system (S.G n. 15), which was obtained by following the atomic displacements corresponding to the eigenvectors of the imaginary frequency mode localized at the Γ-point of the Ccce phase. By observing the enthalpies at low pressures, we found that the Cmc2(1) phase is thermodynamically the most stable. Our results show that the I4/mmm and C2/c phases never stabilize in the 0–20 GPa range of pressure values. On the other hand, the Ccce phase becomes energetically more stable at around 17 GPa, surpassing the Cmc2(1) structure. By considering the effect of entropy and the constant-volume free energies, we observe that the Cmc2(1) polymorph is energetically the most stable phase at low temperature; however, at 350 K, the Ccce system becomes the most stable. By probing the volume-dependent free energies at 19 GPa, we see that Ccce is always the most stable phase between the two structures and also throughout the studied temperature range. When analyzing the phonon dispersion frequencies, we conclude that the Ccce system becomes dynamically stable only around 19–20 GPa and that the Cmc2(1) phase is metastable up to 30 GPa.