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首页> 外文期刊>Journal of materials science >Role of Gd content in Cu(l) and Cu(2) sites on electrical,microstructural, physical, mechanical and superconducting properties of YBa_2Cu_(3-x)Gd_xO_(7-δ) ceramics
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Role of Gd content in Cu(l) and Cu(2) sites on electrical,microstructural, physical, mechanical and superconducting properties of YBa_2Cu_(3-x)Gd_xO_(7-δ) ceramics

机译:Gd含量在YBa_2Cu_(3-x)Gd_xO_(7-δ)陶瓷的电,微结构,物理,机械和超导性能上的Cu(l)和Cu(2)位置中的作用

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摘要

This study deals with the effects of partial Gd~(3+) substitution for the Cu sites on the electrical, microstructural, physical, mechanical and superconducting properties of YBa_2Cu_(3-x)Gd_xO_(7-δ) ceramic superconductors with x = 0, 0.025, 0.050, 0.100 and 0.150 with the aid of dc resistivity, transport critical current density (J_c), X-Ray analysis (XRD), scanning electron microscopy (SEM), electron dispersive X-Ray (EDX), Vickers microhardness (H_v) and density measurements. The samples studied in this work are prepared by the standard solid-state reaction method. The resistivity (at room temperature), critical (onset and offset) temperature, variation of transition temperature, critical current density, hole-carrier concentration, grain size, phase purity, lattice parameter, texturing, surface morphology, element distribution, density, porosity, crystallinity, Vickers microhardness and elastic modulus (E) values of the samples are obtained and compared with each other. The obtained results show that the room temperature resistivity systematically increases with the increment of the Gd content as a result of the hole filling when the onset (T_c~(onset)) and offset (T_c~(offset)) critical temperatures determined from the resistivity curves are found to decrease from 95.2 to 93.6 K and 92.0 to 83.3 K, respectively, showing the presence of impurities and weak links between the superconducting grains. As for the critical current density measurements, the J_c values decrease from 132 to 34 A/cm~2 as the Gd doping increases; The XRD results give that although the Gd~(3+) ions substituted tend to occupy both the Cu(1) and Cu(2) sites, the ions are more favorable for the Cu(2) site as a consequence no change of the crystal structure. Besides, the peak intensities belonging to major phase (Y123) decrease monotonously with the increment of the Gd content in the system; however, new peaks belonging to the minor phases start to appear after the doping level of x = 0.0250 beyond which these peaks enhance monotonously, resulting in the decrement of the grain size. Further, the Lotgering indices calculated from the XRD patterns indicate that the texturing of the Y123 grains reduces systematically with the Gd content. According to the SEM investigations, the micro-structures of the samples prepared degrade slightly with the content up to the doping level of x = 0.025 after which the morphology suddenly deteriorates due to the appearance of the different phases in the system. EDX measurements show that not only do the elements used for the preparation of the Y123 superconductors with and without Gd content distribute homogeneously but also the level of Cu element rapidly decreases with the increment of the Gd content compared to the other elements, illustrating that the Cu~(2+) ions may partly be substituted by Gd~(3+) ions. Moreover, the porosity analyses for the samples depict that the porosity increases with the Gd content, leading to the degradation of the grain connectivity. We also discuss on the mechanical properties of the samples to examine both the elastic modulus and the strength of connection between superconducting grains.
机译:本研究研究了部分Gd〜(3+)取代Cu对X = 0的YBa_2Cu_(3-x)Gd_xO_(7-δ)陶瓷超导体的电,微结构,物理,机械和超导性能的影响直流电阻率,传输临界电流密度(J_c),X射线分析(XRD),扫描电子显微镜(SEM),电子色散X射线(EDX),维氏显微硬度(0.025、0.050、0.100和0.150) H_v)和密度测量。本工作中研究的样品是通过标准的固态反应方法制备的。电阻率(在室温下),临界(开始和偏移)温度,转变温度的变化,临界电流密度,空穴载流子浓度,晶粒尺寸,相纯度,晶格参数,纹理,表面形态,元素分布,密度,孔隙率获得样品的结晶度,维氏显微硬度和弹性模量(E)值,并将其相互比较。所得结果表明,当根据电阻率确定临界温度(T_c〜(offset))和偏移临界温度(T_c〜(offset))时,由于填充孔洞,室温电阻率随着Gd含量的增加而系统地增加。发现曲线分别从95.2降低到93.6 K,从92.0降低到83.3 K,这表明超导晶粒之间存在杂质和弱连接。对于临界电流密度的测量,随着Gd掺杂的增加,J_c值从132 A / cm〜2降低到34 A / cm〜2。 X射线衍射结果表明,尽管被取代的Gd〜(3+)离子倾向于同时占据Cu(1)和Cu(2)位置,但这些离子对Cu(2)位置更有利,因此没有改变。晶体结构。此外,随着体系中Gd含量的增加,主相(Y123)的峰强度单调降低。然而,在x = 0.0250的掺杂水平之后,开始出现属于次要相的新峰,超过这些峰时,这些峰单调增强,导致晶粒尺寸减小。此外,由XRD图谱计算得到的洛格廷指数表明,随着Gd含量的增加,Y123晶粒的织构逐渐降低。根据SEM研究,所制备的样品的微观结构随含量的增加而略微降解,直到x = 0.025的掺杂水平,此后由于系统中不同相的出现,形态突然恶化。 EDX测量结果表明,与其他元素相比,制备具有和不具有Gd含量的Y123超导体所用的元素不仅分布均匀,而且Cu元素的含量随Gd含量的增加而迅速降低。 〜(2+)离子可部分被Gd〜(3+)离子取代。此外,对样品的孔隙率分析表明,孔隙率随Gd含量的增加而增加,导致晶粒连通性降低。我们还讨论了样品的机械性能,以检查弹性模量和超导晶粒之间的连接强度。

著录项

  • 来源
    《Journal of materials science》 |2013年第6期|1842-1854|共13页
  • 作者单位

    Department of Physics, Abant Izzet Baysal University,14280 Bolu, Turkey;

    Department of Physics, Abant Izzet Baysal University,14280 Bolu, Turkey;

    Department of Physics, Abant Izzet Baysal University,14280 Bolu, Turkey;

    Department of Physics, Abant Izzet Baysal University,14280 Bolu, Turkey;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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