首页> 外文期刊>journal of applied physics >Quantitative description of a highJcNb‐Ti superconductor during its final optimization strain. I. Microstructure,Tc, Hc2, and resistivity
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Quantitative description of a highJcNb‐Ti superconductor during its final optimization strain. I. Microstructure,Tc, Hc2, and resistivity

机译:高JcNb连字符Ti超导体在其最终优化应变过程中的定量描述。一、微观结构、Tc、Hc2和电阻率

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A most important step in the critical current density (Jc) optimization of Nb‐Ti is the large final drawing strain, in which agr;‐Ti precipitates, initially approximately equiaxed and 100–200 nm in diameter, are drawn into ribbons, whose thickness (1–2 nm) is less than the superconducting coherence length xgr; (4.2 K)∼5 nm. Using transmission electron microscopy, the precipitate thickness, spacing, cross‐sectional area, and circumference were measured over the whole final drawing strain range. Each of these parameters was found to have a simple power dependence on the wire diameter.Tc,Hc2, and the resistivity (rgr;n) were also change considerably during the refinement of the precipitates. Directly after precipitation,Tcincreased, and (dHc2/dT)Tcand rgr;nwere reduced from the single‐phase values. Drawing the wire returned these parameters to their single‐phase values, as the precipitate thickness was reduced to less than xgr;. This observation explains a long‐standing peculiarity in this system, namely that the optimumHc2of highJcconductors occurs for a composition close to Nb 46 wt. Ti, even when the precipitation of 18 vol  of agr;‐Ti shifts the matrix composition to a Nb‐rich composition of theoretically lowerHc2.
机译:Nb‐Ti 的临界电流密度 (Jc) 优化中最重要的一步是大的最终拉丝应变,其中 &agr;‐Ti 析出物(最初近似等轴且直径为 100–200 nm)被拉成带状,其厚度 (1–2 nm) 小于超导相干长度 [&xgr; (4.2 K)∼5 nm]。使用透射电子显微镜,测量了整个最终拉伸应变范围内的沉淀物厚度、间距、横截面积和周长。发现这些参数中的每一个都与导线直径有简单的功率依赖性。在析出物的精制过程中,Tc、Hc2和电阻率(&rgr;n)也发生了显著变化。沉淀后,Tc增加,(dHc2/dT)Tcand &rgr;n从单相和连字符相值降低。拉丝将这些参数返回到其单相值,因为沉淀物厚度减小到小于 &xgr;。这一观察结果解释了该系统中一个长期存在的特点,即高Jc导体的最佳Hc2发生在接近Nb46 wt.%Ti的成分中,即使18 vol%的沉淀将基体组成转变为理论上较低的Hc2的Nb&连字符丰富的成分。

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