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Siddhartha S. Nathan

Publications and source records attributed to Siddhartha S. Nathan.

2 recordsLinked to original sources

Anion correlation induced nonrelativistic spin splitting in rutile antiferromagnets

Many studies of non-relativistic spin-splitting (NRSS), or altermagnetism, have focused on idealized, perfectly ordered crystals, relying on symmetry-based approaches to identify candidate materials. Here, we theoretically investigate how local short-range ordering (SRO) influences NRSS of energy bands in partially ordered collinear antiferromagnetic iron oxyfluoride (FeOF). Using the cluster expansion method, we identify four nearly degenerate structures (energy difference $\leq 8$ meV per formula unit) that represent distinct snapshots of local plane-to-plane O/F correlations. Our density functional theory (DFT) results show robust NRSS along the $Γ$-M direction in all four structures, despite the absence of long-range order. The magnitude and character of the splitting depend sensitively on the specific direction of anion correlations, effects that are not fully captured in high-symmetry average structures. Notably, two configurations ($Pmc2_1$ and $Pm$) exhibit $Γ$-point spin splitting absent in ordered FeF$_2$ and a virtual crystal approximation model of FeOF. We further predict distinct magneto-optical Kerr effect (MOKE) signatures, enabling experimental detection of SRO-driven electronic structure changes. These results highlight heteroanionic compounds as a promising design space for NRSS antiferromagnets, with experimentally synthesized FeOF already exhibiting a substantially higher Néel temperature (315\,K) than FeF$_2$ (79\,K).

cond-mat.mtrl-sci↗

Peierls-like distortion drives anion ordering in rutile TiOF

We use first principles density functional theory calculations to examine the effect of multiple anions on the Peierls distortion in the rutile oxyfluoride TiOF. By using a structure enumeration approach, we obtain the ground state atomic structure for TiOF and identify the driving forces behind the experimentally observed two-dimensional anion ordering along rutile (110) planes. We find that adjacent edge-connected octahedra comprise like atoms with an --O-O/F-F/O-O/F-F-- pattern along the rutile [001] direction. This anion pattern coexists with a Peierls-like distortion leading to the formation of a singlet state between neighboring Ti$^{3+}$ cations. We show that the anion ordering arises from competition between electrostatic interactions, owing to the Ti-F cation-anion pairs, and the tendency of the $d^1$ Ti$^{3+}$ cation to form Ti-Ti dimers, characterized by increased metal-metal bonding. We find that the addition of strong on-site Coulombic interactions to the Ti $d$ manifold suppresses the formation of the singlet state. By increasing the correlation strength, we uncover two first-order phase transitions: first, from a nonmagnetic insulator to a ferromagnetic half-metal, and then second to a ferromagnetic insulator. Last, we show that the electronic configuration of the transition metal cation in rutile oxyfluorides is responsible for the observed anion order, enabling design of ordered heteroanionic materials exhibiting collective phenomena through cation sublattice control.

cond-mat.mtrl-sci↗