首页> 外文期刊>Journal of Materials Science >Transmission electron microscopy study of GdBa_2Cu _3O_(7-x) containing nano-sized BaMO_3 (M: Hf, Zr, Sn) rods fabricated by pulsed laser deposition
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Transmission electron microscopy study of GdBa_2Cu _3O_(7-x) containing nano-sized BaMO_3 (M: Hf, Zr, Sn) rods fabricated by pulsed laser deposition

机译:脉冲激光沉积制备的纳米尺寸BaMO_3(M:Hf,Zr,Sn)棒的GdBa_2Cu _3O_(7-x)的透射电镜研究

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摘要

Three types of superconducting GdBa_2Cu_3O _(7-x) (GdBCO) layers containing rods of either BaHfO_3 (BHO), BaZrO_3 (BZO), or BaSnO3 (BSO) were fabricated by pulsed laser deposition on Hastelloy substrates with a CeO_2 based textured buffer layer. The critical currents (J _c) values of the GdBCO layers containing those nano-rods are enhanced compared with those of pristine GdBCO layer in high magnetic fields. In order to investigate the relationships between their superconductive properties and their nanostructures, they were characterized in detail by transmission electron microscopy (TEM). TEM is the only method for direct observation of these nano-rods in the GdBCO grains. The GdBCO layers were mainly composed of c-axis oriented GdBCO grains containing numerous nano-sized rods. The crystal orientation relationships between the GdBCO and the nano-rods were as follows; (001)GdBCO//(001)nano-rods and (100)GdBCO//(100) nano-rods. The average diameters of the BHO and the BZO nano-rods were 4.5 and 5.6 nm, respectively. The BSO nano-rods were thicker than other rods. These nano-rods in the central region of the c-axis oriented GdBCO grains were aligned parallel to the c-axis of the GdBCO, while nano-rods in the outer region of the c-axis oriented grains were tilted away from the c-axis. With increase in the thickness of the GdBCO layers, the ratio of the BZO or the BSO nano-rods aligned parallel to the c-axis to those tilted away from the c-axis decreased, so that the J _c-B-θ profiles of the thicker GdBCO layers containing the BZO or the BSO nano-rods became flatter. The BHO nano-rods were homogeneously distributed throughout the GdBCO, and their average length of was less than that of the other nano-rods. The homogeneous distribution and short length of the BHO nano-rods enhanced the J _c values of the GdBCO layers containing them in high magnetic fields. The J _c-B-θ profiles of the GdBCO layers containing the BHO were independent of the layer thickness. From these results, we will discuss about the morphologies and distributions of suitable vortex pinning for applications of GdBCO coated conductor in high magnetic fields.
机译:包含BaHfO_3(BHO),BaZrO_3(BZO)或BaSnO3(BSO)的棒的三种类型的超导GdBa_2Cu_3O _(7-x)(GdBCO)层是通过脉冲激光沉积在具有基于CeO_2的纹理缓冲层的Hastelloy基板上制成的。与原始GdBCO层相比,在高磁场中,包含这些纳米棒的GdBCO层的临界电流(J _c)值得到了提高。为了研究它们的超导性能和它们的纳米结构之间的关系,通过透射电子显微镜(TEM)对其进行了详细表征。 TEM是直接观察GdBCO晶粒中这些纳米棒的唯一方法。 GdBCO层主要由c轴取向的GdBCO晶粒组成,其中包含许多纳米级的棒。 GdBCO与纳米棒之间的晶体取向关系如下: (001)GdBCO //(001)纳米棒和(100)GdBCO //(100)纳米棒。 BHO和BZO纳米棒的平均直径分别为4.5和5.6 nm。 BSO纳米棒比其他棒厚。这些位于c轴取向的GdBCO晶粒中心区域的纳米棒与GdBCO的c轴平行排列,而位于c轴取向的GdBCO晶粒外部区域的纳米棒则远离c-轴。随着GdBCO层厚度的增加,平行于c轴排列的BZO或BSO纳米棒与远离c轴倾斜的纳米棒的比率降低,因此J_c-B-θ分布包含BZO或BSO纳米棒的较厚GdBCO层变得更平坦。 BHO纳米棒均匀分布在整个GdBCO中,其平均长度小于其他纳米棒的平均长度。 BHO纳米棒的均匀分布和较短的长度提高了在强磁场中包含它们的GdBCO层的J _c值。包含BHO的GdBCO层的J_c-B-θ轮廓与层厚度无关。从这些结果中,我们将讨论适用于GdBCO涂层导体在高磁场中的合适涡旋钉扎的形貌和分布。

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