论文标题

基于双层铁的超导体CAK中的首选自旋激发(fe $ _ {0.96} $ ni $ _ {0.04} $)$ _ 4 $ as 4 $ as $ _4 $带有Spin-Vortex Crystal订单

Preferred Spin Excitations in the Bilayer Iron-Based Superconductor CaK(Fe$_{0.96}$Ni$_{0.04}$)$_4$As$_4$ with Spin-Vortex Crystal Order

论文作者

Liu, Chang, Bourges, Philippe, Sidis, Yvan, Xie, Tao, He, Guanghong, Bourdarot, Frederic, Danilkin, Sergey, Ghosh, Haranath, Ghosh, Soumyadeep, Ma, Xiaoyan, Li, Shiliang, Li, Yuan, Luo, Huiqian

论文摘要

自旋轨道耦合(SOC)是了解磁性超导体中磁驱动的超导性的关键,那里存在局部和巡回电子,并且轨道角动量尚未完全消退。在这里,我们报告了一项关于双层化合物CAK的中子散射研究(Fe $ _ {0.96} $ ni $ _ {0.04} $)$ _ 4 $ as 4 $ as $ _4 $,具有超导性的超导性共存,并与非collinearear spin-vortex crystal磁性订单合作,可保留Fe-fe-fe-fe-fe-fe-fe-fe-fe-fe-fe-fe-fe-fe-fe-fe-fe-fe-fe-fe。在超导状态下,由于双层耦合而导致的两种具有奇数甚至$ l $对称性的旋转共振模式类似于$ _4 $的未掺杂化合物Cakfe $ _4 $,但在较低的能量处。极化分析表明,奇数模式为$ c- $轴极化,低能量自旋各向异性可以在高温下持续到顺磁相,在高温下,与其他平面界线和$ c- $ axis双轴磁序相似的其他系统。这些结果为铁刺剂超导体中的SOC效应提供了缺少的难题,并且在$ c- $轴首选磁性激发$ t_c $下方的常见图片中,无论磁性模式或晶格对称性的细节如何。

The spin-orbit coupling (SOC) is a key to understand the magnetically driven superconductivity in iron-based superconductors, where both local and itinerant electrons are present and the orbital angular momentum is not completely quenched. Here, we report a neutron scattering study on the bilayer compound CaK(Fe$_{0.96}$Ni$_{0.04}$)$_4$As$_4$ with superconductivity coexisting with a non-collinear spin-vortex crystal magnetic order that preserves the tetragonal symmetry of Fe-Fe plane. In the superconducting state, two spin resonance modes with odd and even $L$ symmetries due to the bilayer coupling are found similar to the undoped compound CaKFe$_4$As$_4$ but at lower energies. Polarization analysis reveals that the odd mode is $c-$axis polarized, and the low-energy spin anisotropy can persist to the paramagnetic phase at high temperature, which closely resembles other systems with in-plane collinear and $c-$axis biaxial magnetic orders. These results provide the missing piece of the puzzle on the SOC effect in iron-pnictide superconductors, and also establish a common picture of $c-$axis preferred magnetic excitations below $T_c$ regardless of the details of magnetic pattern or lattice symmetry.

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