首页> 外文期刊>Physica, C. Superconductivity and its applications >Suppression of superconductivity by nonmagnetic impurities, structural properties and magnetic ordering in Ho sub(x)La sub(1-x)Ni sub(2)B sub(2)C
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Suppression of superconductivity by nonmagnetic impurities, structural properties and magnetic ordering in Ho sub(x)La sub(1-x)Ni sub(2)B sub(2)C

机译:Ho sub(x)La sub(1-x)Ni sub(2)B sub(2)C中的非磁性杂质,结构特性和磁有序性对超导的抑制

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Superconducting and magnetic properties as well as the lattice structure of polycrystalline Ho sub(x)La sub(1-x)Ni sub(2)B sub(2)C samples have been studied by susceptibility, X-ray, and neutron diffraction measurements, respectively. A miscibility gap has been found between x identical with 0.4 and x identical with 0.7 if the samples are prepared by standard arc-melting. Samples in this concentration range have been successfully prepared by melt-spinning. All samples exhibit the LuNi sub(2)B sub(2)C-type structure and the lattice parameters depend linearly on the La content. Already a low lanthanum concentration of about 10% leads to a rapid depression of T sub(c) from 8.5 K to 2 K. Furthermore this concentration leads to a complete depression of the a-axis modulated incommensurate antiferromagnetic structure. Two other magnetic structures, one with commensurate (0 0 1) and one with incommensurate wave vector (0 0 0.915) were found to be less sensitive to the La concentration. The neutron-diffraction peak intensities connected to these structures decrease with increasing La content and disappear at x identical with 0.75 (commensurate structure) and x identical with 0.55 (incommensurate structure). A comparison with Ho sub(x)R sub(1-x)Ni sub(2)B sub(2)C compounds (R identical with Y, Lu) shows that these two magnetic structures are influenced in different way by the size of the nonmagnetic rare-earth ion R. No size effect was observed for the magnetic ordering temperature of the commensurate antiferromagnetic structure, whereas the incommensurate spiral structure along c-axis was found to be sensitive to the difference in the size of the R and the Ho ions.
机译:通过磁化率,X射线和中子衍射测量研究了多晶Ho sub(x)La sub(1-x)Ni sub(2)B sub(2)C样品的超导和磁性以及晶格结构, 分别。如果样品是通过标准电弧熔化制备的,则发现x等于0.4,x等于0.7。通过熔融纺丝成功制备了该浓度范围内的样品。所有样品均表现出LuNi sub(2)B sub(2)C型结构,晶格参数与La含量线性相关。大约10%的低镧浓度已经导致T sub(c)从8.5 K迅速降低到2K。此外,该浓度还导致a轴调制的不对称反铁磁结构的完全降​​低。发现另外两个磁性结构,一个具有相对应的(0 0 1)和一个具有不相称的波矢(0 0 0.915)对La浓度较不敏感。与这些结构相关的中子衍射峰强度随La含量的增加而降低,并在x等于0.75(相称结构)和x等于0.55(不相称结构)时消失。与Ho sub(x)R sub(1-x)Ni sub(2)B sub(2)C化合物(R与Y,Lu相同)的比较表明,这两个磁性结构受磁化强度的影响不同。相对的反铁磁结构的磁有序温度没有观察到尺寸效应,而发现沿c轴的不相称的螺旋结构对R和Ho的尺寸差异敏感离子。

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