Song Qian, Stavrić Srdjan, Barone Paolo, Droghetti Andrea, Antonenko Daniil S, Venderbos Jörn W F, Occhialini Connor A, Ilyas Batyr, Ergeçen Emre, Gedik Nuh, Cheong Sang-Wook, Fernandes Rafael M, Picozzi Silvia, Comin Riccardo
Department of Physics, Massachusetts Institute of Technology, Cambridge, MA, USA.
Department of Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, MA, USA.
Nature. 2025 May 28. doi: 10.1038/s41586-025-09034-7.
Magnetic states with zero magnetization but non-relativistic spin splitting are outstanding candidates for the next generation of spintronic devices. Their electronvolt (eV)-scale spin splitting, ultrafast spin dynamics and nearly vanishing stray fields make them particularly promising for several applications. A variety of such magnetic states with non-trivial spin textures have been identified recently, including even-parity d-wave, g-wave or i-wave altermagnets and odd-parity p-wave magnets. Achieving voltage-based control of the non-uniform spin polarization of these magnetic states is of great interest for realizing energy-efficient and compact devices for information storage and processing. Spin-spiral type II multiferroics are optimal candidates for such voltage-based control, as they exhibit an inversion-symmetry-breaking magnetic order that directly induces ferroelectric polarization, allowing for symmetry-protected cross-control between spin chirality and polar order. Here we combine photocurrent measurements, first-principles calculations and group-theory analysis to provide direct evidence that the spin polarization of the spin-spiral type II multiferroic NiI exhibits odd-parity character connected to the spiral chirality. The symmetry-protected coupling between chirality and polar order enables electrical control of a primarily non-relativistic spin polarization. Our findings represent an observation of p-wave magnetism in a spin-spiral type II multiferroic, which may lead to the development of voltage-based switching of non-relativistic spin polarization in compensated magnets.
具有零磁化强度但非相对论性自旋分裂的磁态是下一代自旋电子器件的杰出候选者。它们电子伏特(eV)量级的自旋分裂、超快自旋动力学以及几乎可以忽略不计的杂散场,使其在多种应用中特别具有前景。最近已经发现了多种具有非平凡自旋纹理的此类磁态,包括偶宇称d波、g波或i波交替磁体以及奇宇称p波磁体。实现对这些磁态非均匀自旋极化的基于电压的控制,对于实现用于信息存储和处理的高效节能且紧凑的器件具有重要意义。自旋螺旋型II类多铁性材料是这种基于电压控制的最佳候选者,因为它们表现出打破反演对称性的磁序,该磁序直接诱导铁电极化,从而实现自旋手性和极性序之间的对称性保护交叉控制。在这里,我们结合光电流测量、第一性原理计算和群论分析,以提供直接证据表明自旋螺旋型II类多铁性材料NiI的自旋极化表现出与螺旋手性相关的奇宇称特性。手性和极性序之间的对称性保护耦合使得能够对主要是非相对论性的自旋极化进行电控制。我们的发现代表了在自旋螺旋型II类多铁性材料中对p波磁性的观察,这可能会导致在补偿磁体中开发基于电压的非相对论性自旋极化切换。