论文标题

对伪hexagonal cerh $ _3 $ si $ _2 $ si $ _2 $ si $ _2 $ si $ _2 $ si $ _2 $ si $ _2 $调查

Investigation of metamagnetism and crystal-field splitting in pseudo-hexagonal CeRh$_3$Si$_2$

论文作者

Amorese, Andrea, Khalyavin, Dmitry, Kummer, Kurt, Brookes, Nicholas B., Ritter, Clemens, Zaharko, Oksana, Larsen, Camilla Buhl, Pavlosiuk, Orest, Pikul, Adam P., Kaczorowski, Dariusz, Gutmann, Matthias, Boothroyd, Andrew T., Severing, Andrea, Adroja, Devashibhai T.

论文摘要

CERH $ _3 $ SI $ _2 $据报道显示出低于5〜K的元磁过渡,一种巨大的晶体场分裂,以及来自单晶磁化和热容量测量的各向异性磁性特性。在这里,我们报告了磁性结构和晶体场激发的中子和X射线散射研究的结果,以进一步了解该化合物的磁性。当考虑质量轴的晶体学$ A方向时,无弹性中子散射(INS)和共振非弹性X射线散射(RIX)揭示了CE的$ J_z $ \,= \,1/2的地面标准。此外,我们发现$ j $ \,= \,5/2倍数的78 \,MEV的总分裂。零场中的中子衍射研究表明,从顺磁状态冷却后,系统首先以$ t _ {\ text {n} _1} = 4.7 $ \,k在纵向旋转密度波动中,沿着$ b $ axis(I.E. $ \ textbf {k} =(0,0.43,0 $)。下面的低温过渡$ t _ {\ text {n} _2} = 4.48 $ \,k,传播矢量锁到相应值$ \ textbf {k} =(0,0.5,0)$,带有所谓的锁定锁定过渡。我们在应用磁场中的中子衍射研究$ h \ \ parallel b $轴显示了相应的传播矢量的变化,并且在$ h = 3 $ \,koe时的铁磁成分的开发发生了变化,然后是一系列过渡,然后在完全现场诱导的铁磁阶段到达$ h = 7 $ \ $ \,kee。这解释了先前报道的磁化测量测量的步骤的性质。对于$ h \ parallel $ [0 1 1]晶体方向也观察到非常相似的行为。

CeRh$_3$Si$_2$ has been reported to exhibit metamagnetic transitions below 5~K, a giant crystal field splitting, and anisotropic magnetic properties from single crystal magnetization and heat capacity measurements. Here we report results of neutron and x-ray scattering studies of the magnetic structure and crystal-field excitations to further understand the magnetism of this compound. Inelastic neutron scattering (INS) and resonant inelastic x-ray scattering (RIXS) reveal a $J_z$\,=\,1/2 groundstate for Ce when considering the crystallographic $a$ direction as quantization axis, thus explaining the anisotropy of the static susceptibility. Furthermore, we find a total splitting of 78\,meV for the $J$\,=\,5/2 multiplet. The neutron diffraction study in zero field reveals that on cooling from the paramagnetic state, the system first orders at $T_{\text{N}_1}=4.7$\,K in a longitudinal spin density wave with ordered Ce moments along the $b$-axis (i.e. the [0 1 0] crystal direction) and an incommensurate propagation vector $\textbf{k}=(0,0.43,0$). Below the lower-temperature transition $T_{\text{N}_2}=4.48$\,K, the propagation vector locks to the commensurate value $\textbf{k}=(0,0.5,0)$, with a so-called lock-in transition. Our neutron diffraction study in applied magnetic field $H\parallel b$-axis shows a change in the commensurate propagation vector and development of a ferromagnetic component at $H=3$\,kOe, followed by a series of transitions before the fully field-induced ferromagnetic phase is reached at $H = 7$\,kOe. This explains the nature of the steps previously reported in field-dependent magnetization measurements. A very similar behaviour is also observed for the $H\parallel$ [0 1 1] crystal direction.

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