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软共振 X 射线衍射观测到 HoB2C2 中的高阶 Ho 多极子。

High-order Ho multipoles in HoB2C2 observed with soft resonant x-ray diffraction.

机构信息

School of PEMS, UNSW, Canberra, ACT, 2600, Australia.

出版信息

J Phys Condens Matter. 2012 Feb 22;24(7):075602. doi: 10.1088/0953-8984/24/7/075602.

Abstract

Soft resonant x-ray Bragg diffraction (SRXD) at the Ho M4,5 edges has been used to study Ho 4f multipoles in the combined magnetic and orbitally ordered phase of HoB2C2. A full description of the energy dependence for both σ and π incident x-rays at two different azimuthal angles, as well as the ratio I(σ)/I(π) as a function of azimuthal angle for a selection of energies, allows a determination of the higher order multipole moments of rank 1 (dipole) to 6 (hexacontatetrapole). The Ho 4f multipole moments have been estimated, indicating a dominant hexadecapole (rank 4) order with an almost negligible influence from either the dipole or the octupole magnetic terms. The analysis incorporates both the intra-atomic magnetic and quadrupolar interactions between the 3d core and 4f valence shells as well as the interference of contributions to the scattering that behave differently under time reversal. Comparison of SRXD, neutron diffraction and non-resonant x-ray diffraction shows that the magnetic and quadrupolar order parameters are distinct. The (00½) component of the magnetic order exhibits a Brillouin type increase below the orbital ordering temperature T(Q), while the quadrupolar order increases more sharply. We conclude that the quadrupolar interaction is strong, but quadrupolar order only occurs when the magnetic order gives rise to a quasi-doublet ground state, which results in a lock-in of the orbitals at T(Q).

摘要

Ho M4,5 边缘的软共振 X 射线布拉格衍射(SRXD)已被用于研究 HoB2C2 中磁有序和轨道有序相中的 Ho 4f 多极矩。两种不同方位角的 σ 和 π 入射 X 射线的能量依赖性以及在一系列能量下作为方位角函数的 I(σ)/I(π)的比值的完整描述允许确定秩 1(偶极子)到 6(六重偶极矩)的更高阶多极矩。已经估计了 Ho 4f 多极矩,表明主导的六重极矩(秩 4)具有几乎可以忽略不计的偶极子或八极子磁项的影响。该分析包括 3d 核和 4f 价壳层之间的原子内磁相互作用和四极相互作用以及散射贡献在时间反转下表现不同的干扰。SRXD、中子衍射和非共振 X 射线衍射的比较表明,磁和四极有序参数是不同的。轨道有序温度 T(Q)以下,磁有序的(00½)分量表现出布里渊型增加,而四极有序增加更急剧。我们得出的结论是,四极相互作用很强,但只有当磁有序导致准双重基态时才会出现四极有序,这导致轨道在 T(Q)处锁定。

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