AdSM, Hiroshima University, Higashi-Hiroshima 739-8530, Japan.
J Phys Condens Matter. 2012 Jul 25;24(29):294207. doi: 10.1088/0953-8984/24/29/294207.
We performed electrical resistivity ρ, magnetic susceptibility χ, specific heat C and electron diffraction measurements on single-crystalline samples of PrT2Zn20 (T = Ru, Rh and Ir). The three compounds show the Van Vleck paramagnetic behavior, indicating the nonmagnetic crystalline electric field (CEF) ground states. A Schottky-type peak appears at around 14 K, irrespective of the T element, which can be moderately reproduced by a doublet–triplet model. For T = Ru, a structural transition occurs at Ts = 138 K, below which no phase transition appears down to 0.04 K. On the other hand, for T = Ir, antiferroquadrupole (AFQ) ordering arising from the nonmagnetic Γ3 doublet takes place at TQ = 0.11 K. For T = Rh, despite a structural transition between 170 and 470 K, the CEF ground state is still the non-Kramers Γ3 doublet. However, no phase transition due to the Γ3 doublet was observed even down to 0.1 K.
我们对 PrT2Zn20(T=Ru、Rh 和 Ir)的单晶样品进行了电阻率 ρ、磁化率 χ、比热 C 和电子衍射测量。这三种化合物均表现出范弗莱克顺磁行为,表明存在非磁性晶场(CEF)基态。在大约 14 K 处出现肖特基型峰值,与 T 元素无关,该峰值可以通过双峰-三重态模型适度重现。对于 T=Ru,在 Ts=138 K 处发生结构转变,在 0.04 K 以下没有出现相变。另一方面,对于 T=Ir,来自非磁性 Γ3 二重态的反铁四极(AFQ)有序在 TQ=0.11 K 处发生。对于 T=Rh,尽管在 170 到 470 K 之间存在结构转变,但 CEF 基态仍然是非克喇末 Γ3 二重态。然而,即使在 0.1 K 以下,也没有观察到由于 Γ3 二重态引起的相变。