Altermagnets (AMs) represent an emerging magnetic phase that combines compensated antiferromagnetic order with ferromagnet‐like spin‐splitting, offering a new route for efficient spin‐current generation. Here, we experimentally demonstrate spin‐torque generation in epitaxial CrSb and reveal a pronounced crystallographic dependence of the resulting spin‐orbit torques (SOTs) across the ( 11¯00$1\overline{1}00$ ) and ( 112¯0$11\overline{2}0$ ) orientations. Using spin‐torque ferromagnetic resonance, we identify unconventional SOT behavior, including a finite x‐polarized damping‐like torque and reversal of the y‐polarized damping‐like torque between the two crystal planes, features that cannot be explained by conventional spin Hall or Rashba–Edelstein mechanisms. The damping‐like torque efficiencies are comparable to those of heavy metals and exhibit strong in‐plane anisotropy directly linked to crystal symmetry. Symmetry analysis shows that the observed angular dependence originates from a crystallographic torque permitted by the C2v point group, whereas AM‐specific contributions from the magnetic spin Hall and spin‐splitter effects remain negligible due to the multi‐domain state and weak strain‐induced g‐to‐d spin symmetry deformation in CrSb. These findings show that epitaxial CrSb can host strongly anisotropic spin‐torques governed primarily by crystallographic and interfacial symmetry, providing a route toward crystallographically engineered spintronic devices.
Artificially‐designed magnetic hetero‐structures with an antiferromagnetic alignment of magnetization in magnetic layers, which exploit the interlayer exchange coupling (IEC) through a non‐magnetic layer, are called synthetic antiferromagnets (SyAF) and are a treasure trove of functionalities for spintronics applicat...
Xue-Yao Hou, Keita Ito, V. K. Kushwaha et al.· Advanced Electronic Material...· 0 citations
Ferromagnetic 3
d
‐5
d
double perovskites exhibit appealing physical properties due to their unique electronic band structures, which result from the hybridization of 3
d
and 5
d
orbitals. Sr
2
FeReO
6
(SFRO) exhibits half‐metallicity, a high Curie temperature (∼400 K), and spin–orbit–lattice coupling,...
Gahee Noh, Seong-Sik Kim, Hansol Lee et al.· Advanced Functional Material...· 0 citations
Realizing room‐temperature out‐of‐plane spin currents remains a key challenge for low‐power perpendicular spin–orbit torque devices. Oxides with strong spin–orbit coupling are highly desirable spin sources for spintronic applications, and RuO
2
has recently attracted widespread attention owing to its excellent sp...
Jie Zheng, Gui-Bin Lan, He Bai et al.· Advanced Functional Material...· 0 citations
Altermagnets offer a promising route to spintronic devices by combining spin-split electronic states with zero net magnetization, but how reduced dimensionality reshapes their magnetic order remains poorly understood. Here, we grow bilayer-thickness CrSb (0001) films directly on SrTiO3(001) substrates by molecular beam...
Yun-Long Liu, Zi-Xuan Wu, Qin-Xi Liu et al.· Newton· 0 citations
Atomically thin magnets are governed by composition, thickness, stacking, strain, defects, substrates, ferroic order, and interfaces. This Review organizes two‐dimensional (2D) magnetism using net magnetization and momentum‐space spin splitting or spin‐polarization patterns as primary coordinates, supplemented by sub...
Guo-Jian Zhao, Ziang Meng, Li Liu et al.· Advanced Functional Material...· 0 citations
Exchange bias (EB) is a central mechanism in spintronics, enabling unidirectional magnetic anisotropy, enhanced coercivity, and stable pinned magnetic states through interfacial exchange coupling. Two‐dimensional (2D) van der Waals (vdW) magnets offer a new platform for engineering EB at the atomic scale, where sharp...