磁控溅射-热处理过程中Nb3Sn薄膜的界面演变与生长机制
1 中色创新研究院(天津)有限公司 天津 300393
2 松山湖材料实验室 东莞 523000
收稿日期: 2026-04-09
修回日期: 2026-05-21
录用日期: 2026-06-30
网络出版日期: 2026-06-30
Microstructural Evolution and Growth Mechanisms of Nb3Sn Thin Films During Magnetron Sputtering and Heat Treatment
1 China Nonferrous Metals Innovation Research Institute (Tianjin) Co. Ltd., Tianjin 300393, China
2 Songshan Lake Materials Laboratory, Dongguan 523000, China
Received date: 2026-04-09
Revised date: 2026-05-21
Accepted date: 2026-06-30
Online published: 2026-06-30
巩晓乐 , 高勇 , 陈岩 , 信纪军 , 杨清 , 尹圆圆 , 赵红运 , 王维 . 磁控溅射-热处理过程中Nb3Sn薄膜的界面演变与生长机制[J]. 金属学报, 0 : 0 . DOI: 10.11900/0412.1961.2026.00101
A15-type Nb3Sn, owing to its high superconducting transition temperature, high upper critical field, and potential for superconducting radio-frequency applications, is regarded as a promising candidate for next-generation superconducting radio-frequency functional films. In this study, Nb3Sn thin films were prepared on single-crystal Nb substrates by Nb/Sn dual-target magnetron co-sputtering followed by vacuum annealing at 900 °C, with the aim of clarifying the microstructural evolution and growth-controlling mechanism during sputtering and heat treatment. The growth of Nb3Sn films is not governed solely by the Nb substrate orientation or by simple interfacial epitaxy, but by the coupled effects of Nb substrate orientation, Sn diffusion, local compositional fluctuation, and interfacial defects. The Nb substrate orientation can locally induce the orientation relationship of (210)Nb3Sn//(110)Nb and contribute to interfacial strain relaxation; however, because the film is composed of competing multi-oriented grains, its role is mainly local and modulatory. By contrast, dislocations, grain boundaries, and interfacial defects provide preferential short-circuit diffusion paths for Sn and therefore dominate local Sn enrichment, A15 phase nucleation/growth, and the evolution of compositional inhomogeneity. After heat treatment, the superconducting transition temperature (Tc) increases from 9.8 K to 12.6 K, indicating the promoted formation of the A15-Nb3Sn phase, whereas the broadening of the transition width (ΔTc) to 6.0 K suggests that residual compositional and structural inhomogeneities still limit further performance improvement.
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