Effect of spin-orbit coupling on spin and orbital ordering in Sr$_{n+1}$Cr$_n$O$_{3n+1}$, $n=1,2$

Cristian Fanjul; A. A. Aligia

doi:10.1103/wjw9-xylv

paper

Effect of spin-orbit coupling on spin and orbital ordering in Sr $_{n + 1}$ Cr $_{n}$ O $_{3 n + 1}$ , $n = 1, 2$

arXiv:2603.28904 · doi:10.1103/wjw9-xylv

Abstract

We incorporate spin-orbit coupling (SOC) into effective Kugel-Khomskii models for the $n = 1$ and $n = 2$ members of the Ruddlesden-Popper series Sr $_{n + 1}$ Cr $_{n}$ O $_{3 n + 1}$ . These model contain interacting spins 1 and pseudospins 1/2 at each site describing spin and orbitals degrees of freedom respectively. We solve the models at zero temperature using pseudospin bond operators and spin waves. We find that for realistic parameters, SOC dominates the physics of the compound Sr $_{2}$ CrO $_{4}$ with almost decoupled single CrO $_{2}$ planes. The spin ordering is antiferromagnetic, with nearest-neighbor Cr spins aligned antiparallel. The corresponding orbital configuration is $d_{x y ↑}^{1} (d_{x z ↑}^{1} - i d_{y z ↑}^{1})$ or $d_{x y ↓}^{1} (d_{x z ↓}^{1} + i d_{y z ↓}^{1})$ depending on the spin of the site. In contrast, for the bilayer compound Sr $_{3}$ Cr $_{2}$ O $_{7}$ we find that the effect of the SOC is weak and the system prefers to form pseudospin singlets in the $z$ direction perpendicular to the planes. The spin order is antiferromagnetic within each plane and ferromagnetic between planes, in agreement with previous studies.

arXiv comment10 pages, 1 figure

Effect of spin-orbit coupling on spin and orbital ordering in Srn+1​Crn​O3n+1​, n=1,2

Abstract

References in corpus (21)

Effect of spin-orbit coupling on spin and orbital ordering in Sr $_{n + 1}$ Cr $_{n}$ O $_{3 n + 1}$ , $n = 1, 2$