论文标题

铀层和锯齿链链的磁晶对竞争的竞争$ _ {0.34} $ ge $ _2 $单晶

Competition of Magnetocrystalline Anisotropy of Uranium Layers and Zig-Zag Chains in UNi$_{0.34}$Ge$_2$ Single Crystals

论文作者

Pikul, Adam P., Szlawska, Maria, Ding, Xiaxin, Sznajd, Józef, Ohashi, Masashi, Kowalska, Dorota A., Pasturel, Mathieu, Gofryk, Krzysztof

论文摘要

单晶Uni $ _ {1-x} $ ge $ _2 $带有$ x $ \,= \,0.66的结构和热力学特性,通过测量磁化,比热和热膨胀在广泛的温度和磁场范围内进行了研究。测量结果揭示了在n {e}温度下方的铀磁矩下方的远程防铁磁序的出现。沿这两个晶体学方向应用的磁场在系统中诱导了一阶元磁相变(从抗磁磁性到野极化的磁磁性),并且与该过渡相关的磁性磁滞后宽度在最低温度下达到高达40 koe。从实验数据开发的磁相图表明,与该磁性磁滞相关的亚稳态形成了一个漏斗,该漏斗向零磁场中的n {é} El点变窄。四层ISING模型已成功预测了Uni $ _ {0.34} $ GE $ _2 $(从早期报告中知道),其磁相图以及其磁化强度的温度和场变化中的共线抗磁磁结构。此外,这表明一阶相变延伸至零磁场,尽管在低磁场中进行的实验几乎无法检测到。根据该模型,二阶相变仅在零场中的化合物中发生。

Structural and thermodynamic properties of single-crystalline UNi$_{1-x}$Ge$_2$ with $x$\,=\,0.66 have been investigated by measuring magnetization, specific heat, and thermal expansion over a wide range of temperatures and magnetic fields. The measurements revealed the emergence of a long-range antiferromagnetic ordering of uranium magnetic moments below the N{é}el temperature $T_{\rm N}$\,=\,45.5\,K and the existence of two easy axes in the studied compound, namely $b$ and $c$, which correspond to the planes of the uranium zig-zag chains. Magnetic field applied along these two crystallographic directions induces in the system a first-order metamagnetic phase transition (from antiferromagnetism to field-polarized paramagnetism), and the width of the magnetic hysteresis associated with that transition reaches as much as 40 kOe at the lowest temperatures. A magnetic phase diagram developed from the experimental data showed that the metastable region associated with that magnetic hysteresis forms a funnel that narrows toward the N{é}el point in zero magnetic field. The four-layer Ising model has successfully predicted the collinear antiferromagnetic structure in UNi$_{0.34}$Ge$_2$ (known from earlier reports), its magnetic phase diagram, and temperature and field variations of its magnetization. Moreover, it suggests that the first-order phase transition extends down to zero magnetic field, although it is barely detectable in the experiments performed in low magnetic fields. According to this model, the second-order phase transition occurs in the compound only in zero field.

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