Understanding the local structure, magnetism and optical properties in layered compounds with d9 ions: Insight into silver fluorides and K2CuF4

TL;DR

This study uses first-principles DFT calculations to explore how crystal structure, magnetism, and optical properties vary in layered fluoride compounds with d9 ions, revealing new insights into their structural stability and magnetic ordering.

Contribution

The paper demonstrates that the orthorhombic structure of Cs2AgF4 and K2CuF4 is stabilized by electrostatic effects rather than Jahn-Teller distortions, providing a new understanding of their structural and magnetic properties.

Findings

Cs2AgF4 and K2CuF4 have orthorhombic structures with weak ferromagnetism.

Their structure is stabilized by electrostatic effects, not Jahn-Teller distortions.

The I4/mmm phase is unstable and evolves into the orthorhombic Cmca structure with ferromagnetic order.

Abstract

Using first-principles DFT calculations, we analyze the origin of the different crystal structures, optical and magnetic properties of two basic families of layered fluoride materials with formula A2MF4 (M = Ag, Cu, Ni, Mn; A = K, Cs, Rb). On one hand, Cs2AgF4 and K2CuF4 compounds (both with d9 metal cations) crystallize in an orthorhombic structure with Cmca space group and MA - F - MB bridge angle of 180, and they exhibit a weak ferromagnetism (FM) in the layer plane. On the other hand, K2NiF4 or K2MnF4 compounds (with d8 and d5 metal cations, respectively) have a tetragonal I4/mmm space group with 180 bridge angle and exhibit antiferromagnetism (AFM) in the layer plane. Firstly, we show that, contrary to what is claimed in the literature, the Cmca structure of Cs2AgF4 and K2CuF4 is not related to a cooperative Jahn-Teller effect among elongated MF64- units. Instead, first-principles calculations carried out in the I4/mmm parent phase of these two compounds show that MF64- units are axially compressed because the electrostatic potential from the rest of lattice ions force the hole to lie in the 3z2 - r2 molecular orbital (z being perpendicular to the layer plane). This fact increases the metal-ligand distance in the layer plane and makes that covalency in the bridging ligand has a residual character (clearly smaller than in K2NiF4 or KNiF3) stabilizing for only a few meV (7.9 meV for Cs2AgF4) an AFM order. However, this I4/mmm parent phase of Cs2AgF4 is unstable thus evolving towards the experimental Cmca structure with an energy gain of 140 meV, FM ordering and orthorhombic MF64- units.