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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 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&d4; 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&d4; 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&d4; axis have been characterized with neutron diffraction measurements. A “mixed phase” 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 R Ni 2 Ge 2 (R =稀土)族的长程相互作用和各向异性的相互作用。化合物。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。 Tb,Dy,Eu和Gd成员的磁性结构已使用高质量的单晶样品确定。 TbNi 2 Ge 2 和DyNi 2 Ge 2 顺序为调幅结构低于 T N ,具有传播矢量(0́0 0.758)和(0́0 0.75)。在 T t italic> T N 之下,结构为等矩相称,描述如下分别通过(00¾)和三次谐波(00¼),(1 /2½0)和(1 /2½½)三种调制进行调制。而Tb化合物为单轴,且沿 c &d4; / ac> 轴在两个阶段中,其Dy邻居具有有序的平面内分量。 XRES是研究中子不透明Eu和Gd成员的首选探针。 EuNi 2 Ge 2 具有简单的反铁磁状态(0’0 1),矩在基平面上,GdNi 2 Ge 2 阶,具有不相称调制,(0 0 0.793)在 T N c &d4; 有一个有序的分量 T N 以下但在 T t 以上的Gd化合物中。在 T t 以下,Gd矩被锁定到基面。这项工作将强费米表面嵌套与 R Ni 2 Ge 2 化合物中的磁有序联系起来。广义磁化率 c 0 q ),计算发现嵌套是负责任的GdNi 2 Ge 2 中的不等价有序波矢量以及EuNi 2中相称的结构 Ge 2 。预测通过带填充将从不相称的磁性结构连续过渡到相称的磁性结构。 EuNi 2 Ge 2 中的 T N 高于GdNi 2 还解释了Ge 2 。接下来,沿着 c施加磁场的TbNi 2 Ge 2 中的所有亚磁相 &d4; 轴已通过中子衍射测量进行了表征。提出了由完全饱和的以及减矩的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。

著录项

  • 作者

    Islam, Zahirul.;

  • 作者单位

    Iowa State University.;

  • 授予单位 Iowa State University.;
  • 学科 Physics Condensed Matter.; Engineering Materials Science.
  • 学位 Ph.D.
  • 年度 1999
  • 页码 165 p.
  • 总页数 165
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 工程材料学;
  • 关键词

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