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纳米尺度 MgB2/Fe 层状结构界面的冶金相及其磁性。

Metallurgical phases and their magnetism at the interface of nanoscale MgB2/Fe layered structures.

机构信息

Deutsches Elektronen Synchrotron DESY, Notkestrasse 85, D-22607 Hamburg, Germany.

出版信息

J Phys Condens Matter. 2011 Nov 30;23(47):475702. doi: 10.1088/0953-8984/23/47/475702. Epub 2011 Nov 10.

DOI:10.1088/0953-8984/23/47/475702
PMID:22076071
Abstract

We report on the characterization of metallurgical phases and their magnetism at the interfaces of nanoscale MgB(2)/Fe layered structures. MgB(2)/(57)Fe multilayers with varying layer thicknesses were prepared by vacuum deposition and investigated, before and after annealing by electrical resistance measurements, x-ray diffraction and (57)Fe conversion-electron Mössbauer spectroscopy (CEMS) down to 5 K. Interfacial Fe-B phases, such as Fe(2)B, were identified by CEMS. A superparamagnetic-to-ferromagnetic transition is observed with increasing (57)Fe film thickness. Ultrahigh vacuum annealing at 500 °C of the multilayers leads to strong diffusion of Fe atoms into the boundary regions of the MgB(2) layers. MgB(2) in the as-grown multilayers is non-superconducting. Structural disorder and the effect of Fe interdiffusion contribute to the suppression of superconductivity in the MgB(2) films of all the as-grown multilayers and the thinner annealed multilayers. However, an annealed MgB(2)/(57)Fe/MgB(2) trilayer with thicker (500 Å) MgB(2) layers is observed to be superconducting with an onset temperature of 25 K. At 5 K, the annealed trilayer can be conceived as being strongly chemically modulated, consisting of two partially Fe-doped superconducting MgB(2) layers separated by an interdiffused weakly magnetic Fe-B interlayer, which is characterized by a low hyperfine magnetic field B(hf) of ∼11 T. This chemically modulated layer structure of the trilayer after annealing was verified by Rutherford backscattering.

摘要

我们报告了纳米级 MgB(2)/Fe 层状结构界面处冶金相及其磁性的特征。通过真空沉积制备了具有不同层厚的 MgB(2)/(57)Fe 多层膜,并在退火前后通过电阻测量、X 射线衍射和 (57)Fe 转换电子穆斯堡尔谱 (CEMS) 进行了研究,最低温度可达 5 K。CEMS 鉴定了界面处的 Fe-B 相,如 Fe(2)B。随着 (57)Fe 膜厚度的增加,观察到超顺磁到铁磁转变。对多层膜在 500°C 的超高真空退火导致 Fe 原子强烈扩散到 MgB(2)层的边界区域。在生长的多层膜中,MgB(2)是非超导的。结构无序和 Fe 互扩散的影响导致所有生长的多层膜和较薄的退火多层膜中 MgB(2)薄膜的超导性被抑制。然而,观察到具有较厚 (500 Å) MgB(2)层的退火 MgB(2)/(57)Fe/MgB(2)三层膜具有超导性,起始温度为 25 K。在 5 K 时,退火后的三层膜可以被认为是强烈化学调制的,由两个部分掺杂 Fe 的超导 MgB(2)层组成,它们由互扩散的弱磁性 Fe-B 层隔开,其超精细磁场 B(hf)约为 11 T。退火后三层膜的这种化学调制层结构通过卢瑟福背散射得到了验证。

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