Pressure-Driven Transitions in La2CoTiO6: Antiferromagnetic Insulator to Nonmagnetic Metal via Antiferromagnetic Metal in a Double Perovskite Oxide

TL;DR

This study investigates pressure-induced phase transitions in La2CoTiO6, revealing a sequence from antiferromagnetic insulator to nonmagnetic metal driven by structural and spin-state changes, using experimental and first-principles calculations.

Contribution

It uncovers the pressure-driven magnetic and electronic phase transitions in La2CoTiO6, highlighting the role of structural distortions and spin-state changes in a double perovskite oxide.

Findings

Transition from AFM insulator to AFM metal at ~42 GPa

Spin state shifts from high-spin to low-spin in Co

Structural distortion influences electronic and magnetic phases

Abstract

In double perovskite oxides (A$_2$BB$^\prime$O$_6$), magnetism often arises from diluted magnetic lattices, created by combining a perovskite structure with localized 3$d$ magnetic elements (B) alongside another perovskite lattice containing nearly nonmagnetic delocalized 4$d$/$5d$ elements (B$^\prime$). Alternatively, the magnetic lattice can consist entirely of 3$d$ elements, with one being completely nonmagnetic with $d^0$ state. La$_2$CoTiO$_6$ (LCTO), a representative double perovskite oxide, contains Ti in a nonmagnetic state with a $d^0$ electron configuration due to its $4^+$ oxidation state. Experimental evidence shows that LCTO possesses a monoclinic structure (space group $P2_1/n$) and behaves as an antiferromagnet with a N\'{e}el temperature of 14.6 K. Through first-principle electronic structure calculations, we uncover that adjusting external hydrostatic pressure induces a sequence of phase transitions: from antiferromagnetic insulator (AFM-I) to antiferromagnetic metal (AFM-M), and ultimately to itinerant nonmagnetic metal (NM-M). The transition from AFM-I to AFM-M at $\sim$ 42 GPa pressure coincides with a shift in spin states, moving from a high-spin (HS) state to a low-spin (LS) state, while Co retains a $d^7$ configuration. Distortion within the monoclinic structure under pressure plays a pivotal role in the spin-state transition. At the AFM-I to AFM-M transition, we observe a sharp decrease in the ratio of the octahedral volumes occupied by Co and Ti. Such change in ratio is linked to variations in octahedral volumes, akin to a breathing mode distortion. We explore the impact of the breathing mode distortion by examining a highly symmetric theoretical structure (space-group $I4/mmm$), achieved by optimizing the structure with all $\angle${Co-O-Ti} angles set to 180$^{\circ}$.