Phonon dynamics in the layered negative thermal expansion compounds Cu${}_x$Ni${}_{2-x}$(CN)${}_4$

Abstract

This study explores the relationship between phonon dynamics and negative thermal expansion (NTE) in Cu${}_x$Ni${}_{2-x}$(CN)${}_4$. The partial replacement of nickel (II) by copper (II) in Ni(CN)${}_2$ leads to a line phase, CuNi(CN)${}_4$ (x = 1), and a solid solution, Cu${}_x$Ni${}_{2-x}$(CN)${}_4$ (0 $\le$ x $\le$ 0.5). CuNi(CN)${}_4$ adopts a layered structure related to that of Ni(CN)${}_2$ (x = 0), and interestingly exhibits 2D NTE which is about 1.5 times larger. Inelastic neutron scattering (INS) measurements combined with first principles lattice dynamical calculations provide insights into the effect of Cu${}^{2+}$ on the underlying mechanisms behind the anomalous thermal behavior in all the Cu${}_x$Ni${}_{2-x}$(CN)${}_4$ compounds. The solid solutions are presently reported to also show 2D NTE. The INS results highlight that as the Cu${}^{2+}$ content increases in Cu${}_x$Ni${}_{2-x}$(CN)${}_4$, large shifts to lower energies are observed in modes consisting of localized in- and out-of-plane librational motions of the CN ligand, which contribute to the NTE in CuNi(CN)${}_4$. Mode Grüneisen parameters calculated for CuNi(CN)${}_4$ show that acoustic and low-energy optic modes contribute the most to the NTE, as previously shown in Ni(CN)${}_2$. However, mode eigenvectors reveal a large deformation of the [CuN4] units compared to the [NiC4] units, resulting in phonon modes not found in Ni(CN)${}_2$, whose NTE-driving phonons consist predominately of rigid-unit modes. The deformations in CuNi(CN)${}_4$ arise because the d${}^9$ square-planar center is easier to deform than the d${}^8$ one, resulting in a greater range of out-of-plane motions for the adjoining ligands.