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The interplay of long-range magnetic order and single-ion anisotropy in rare earth nickel germanides

机译:稀土镍锗化物中长距离磁阶与单离子各向异性的相互作用

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摘要

This dissertation is concerned with the interplay of long-range order and anisotropy in the tetragonal RNi2Ge2 (R = rare earth) family of compounds. Microscopic magnetic structures were studied using both neutron and x-ray resonant exchange scattering (XRES) techniques;The magnetic structures of Tb, Dy, Eu and Gd members have been determined using high-quality single-crystal samples. TbNi2Ge2 and DyNi2Ge2 order in an amplitude modulated structure below TN, with propagation vectors (0 0 ∼ 0.758) and (0 0 ∼ 0.75), respectively. Below Tt \u3c TN, the structures are equal moment commensurate , described by three modulations, (0 0 ¾) and its third harmonic (0 0 ¼), (½ ½ 0) and (½ ½ ½), respectively. Whereas the Tb compound is uniaxial with moments along the c\u26d4; axis in both phases, its Dy neighbor has an ordered in-plane component. XRES is the probe of choice for the study of neutron-opaque Eu and Gd members. While EuNi2Ge2 has a simple antiferromagnetic state, (0 0 1), with moments in the basal plane, GdNi2Ge 2 orders with an incommensurate modulation, (0 0 ∼ 0.793) at TN. There is an ordered component along c\u26d4; in the Gd compound below TN but above Tt. Below Tt, Gd moment is locked to the basal plane;This work has correlated a strong Fermi surface nesting to the magnetic ordering in the RNi2Ge2 compounds. Generalized susceptibility, c0 (q), calculations found nesting to be responsible for both incommensurate ordering wave vector in GdNi2Ge 2, and the commensurate structure in EuNi2Ge 2. A continuous transition from incommensurate to commensurate magnetic structures via band filling is predicted. The surprisingly higher TN in EuNi2Ge2 than that in GdNi 2Ge2 is also explained;Next, all the metamagnetic phases in TbNi2Ge2 with an applied field along the c\u26d4; axis have been characterized with neutron diffraction measurements. A \u22mixed phase\u22 model for the first metamagnetic structure consisting of fully-saturated as well as reduced-moment Tb ions is presented. The moment reduction may be due to moment instability which is possible if the exchange is comparable to the low-lying CEF level splitting and the ground state is a singlet. In such a case, certain Tb sites may experience a local field below the critical value needed to reach saturation.
机译:本文涉及四方RNi2Ge2(R =稀土)化合物家族中的长程有序和各向异性的相互作用。使用中子和X射线共振交换散射(XRES)技术研究了微观磁性结构;使用高质量的单晶样品确定了Tb,Dy,Eu和Gd成员的磁性结构。 TbNi2Ge2和DyNi2Ge2在TN以下的调幅结构中有序,分别具有传播矢量(0 0〜0.758)和(0 0〜0.75)。在T t TN之下,这些结构是相等的力矩对应的,分别由三个调制(0 0¾)及其三次谐波(0 0¼),(1/2½0)和(1/2½½)来描述。 Tb化合物是沿c \ u26d4的矩是单轴的;在两个阶段的轴中,其Dy邻居具有一个有序的平面内分量。 XRES是研究中子不透明Eu和Gd成员的首选探针。 EuNi2Ge2具有简单的反铁磁态(0 0 1),在基面上有矩,而GdNi2Ge 2在TN处的调制不当,为(0 0〜0.793)。 c \ u26d4处有一个有序组件;在低于TN但高于Tt的Gd化合物中。在Tt以下,Gd矩被锁定在基面上;这项工作将强大的费米表面嵌套与RNi2Ge2化合物中的磁有序联系起来。广义磁化率c0(q)计算发现,嵌套是造成GdNi2Ge 2中不相称的有序波矢量和EuNi2Ge 2中相称的结构的原因。预计会通过带填充从不相称磁结构过渡到相称磁结构。还解释了EuNi2Ge2中比GdNi 2Ge2中更高的TN。接下来,TbNi2Ge2中的所有亚磁相都沿着c \ u26d4施加了磁场。轴已经用中子衍射测量来表征。提出了由完全饱和的以及还原矩的Tb离子组成的第一个超磁结构的混合相模型。力矩减小可能是由于力矩不稳定性所致,如果交换与低洼的CEF电平拆分相当,并且基态是单线态,则力矩不稳定是可能的。在这种情况下,某些Tb部位可能会遇到低于达到饱和所需的临界值的局部场。

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    Islam, Zahirul;

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  • 年度 1999
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  • 原文格式 PDF
  • 正文语种 en
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