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在脉冲高磁场下通过中子衍射确定 U(Ru(0.96)Rh(0.04))2Si2 中相 II 的磁结构。

Magnetic structure of phase II in U(Ru(0.96)Rh(0.04))2Si2 determined by neutron diffraction under pulsed high magnetic fields.

机构信息

Institute of Applied Beam Science, Ibaraki University, Mito 310-8512, Japan.

出版信息

Phys Rev Lett. 2013 May 24;110(21):216406. doi: 10.1103/PhysRevLett.110.216406. Epub 2013 May 23.

Abstract

We report neutron diffraction measurements on U(Ru(0.96)Rh(0.04))(2)Si(2) single crystal under pulsed high magnetic fields up to 30 T applied along the tetragonal c axis. The high-field experiments revealed that the field-induced phase II above 26 T corresponds to a commensurate up-up-down ferrimagnetic structure characterized by the wave vector q=(2/3,0,0) with the magnetic moments parallel to the c axis, which naturally explains the one-third magnetization plateau and the substantially changed Fermi surface in phase II. This a-axis modulated magnetic structure indicates that the phase II near the hidden order phase is closely related to the characteristic incommensurate magnetic fluctuations at Q(1)=(0.6,0,0) in the pure system URu(2)Si(2), in contrast to the pressure-induced antiferromagnetic order at Q(0)=(1,0,0).

摘要

我们报道了在脉冲高磁场下对 U(Ru(0.96)Rh(0.04))(2)Si(2) 单晶进行的中子衍射测量,磁场高达 30 T,沿四方 c 轴施加。高场实验表明,在 26 T 以上的场诱导相 II 对应于一个共格的 up-up-down 铁磁共振结构,其波矢 q=(2/3,0,0),磁矩平行于 c 轴,这自然解释了三分之一的磁化平台和相 II 中明显变化的费米面。这种 a 轴调制的磁结构表明,在近隐藏序相的相 II 与纯系统 URu(2)Si(2)中在 Q(1)=(0.6,0,0)处的特征非共格磁涨落密切相关,而与压力诱导的在 Q(0)=(1,0,0)处的反铁磁有序相反。

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