Department of Materials Science and Technology, Tokyo University of Science, Niijuku, Tokyo 125-8585, Japan.
J Phys Condens Matter. 2013 Oct 23;25(42):426004. doi: 10.1088/0953-8984/25/42/426004. Epub 2013 Sep 27.
Magnetic susceptibility and specific heat measurements on quasicrystalline approximants Au-Si-Gd and Au-Ge-Gd reveal that a ferromagnetic (FM) transition occurs at Tc = 22.5(5) K for Au-Si-Gd and at Tc = 13(1) K for Au-Ge-Gd, which are the first examples of ferromagnetism in crystalline approximants. In addition, a re-entrant spin-glass (RSG) transition is observed at TRSG = 3.3 K for Au-Ge-Gd in contrast to Au-Si-Gd. The different behaviors are understood based on the recent structural models reported by Gebresenbut et al (2013 J. Phys.: Condens. Matter 25 135402). The RSG transition in Au-Ge-Gd is attributed to a random occupation of the center of the Gd12 icosahedron by Gd atoms; a central Gd spin hinders the long-range FM order.
对准晶近晶合金 Au-Si-Gd 和 Au-Ge-Gd 的磁化率和比热测量表明,Au-Si-Gd 中的铁磁共振 (FM) 转变发生在 Tc = 22.5(5) K,而 Au-Ge-Gd 中的铁磁共振转变发生在 Tc = 13(1) K,这是晶体近晶合金中首次出现铁磁性。此外,在 Au-Ge-Gd 中观察到再入 spin-glass (RSG) 转变,而在 Au-Si-Gd 中则没有。根据 Gebresenbut 等人(2013 J. Phys.:Condens. Matter 25 135402)最近报道的结构模型,可以理解这些不同的行为。Au-Ge-Gd 中的 RSG 转变归因于 Gd 原子随机占据 Gd12 二十面体的中心;中心 Gd 自旋阻碍了长程 FM 有序。