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用于未来太赫兹器件的外延非轴Bi₂Sr₂CaCu₂O薄膜

Epitaxial Non -Axis Bi₂Sr₂CaCu₂O Thin Films for Future THz Devices.

作者信息

Endo Kazuhiro, Arisawa Shunichi, Badica Petre

机构信息

Kanazawa Institute of Technology, Hakusan, Ishikawa 924-0838, Japan.

National Institute of Materials Science, Tsukuba, Ibaraki 305-0047, Japan.

出版信息

Materials (Basel). 2019 Apr 5;12(7):1124. doi: 10.3390/ma12071124.

DOI:10.3390/ma12071124
PMID:30959795
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6479393/
Abstract

Thin films of (117) Bi₂Sr₂Ca₂CuO (Bi-2212) were grown by Molecular Organic Chemical Vapor Deposition (MOCVD) on (110) SrTiO₃ and (110) LaAlO₃ substrates. Substrates were vicinal with off angles up to 20°. Films are 3D epitaxial and X-ray diffraction - scans demonstrate that, while the films grown on a flat substrate are composed of twinned grains, the films on vicinal substrate are . A higher quality is obtained if growth is performed at two temperatures: Growth starts at 550⁻600 °C and continues at 700⁻750 °C. The twin-free film grown by the two-temperature method shows a zero-resistance critical temperature of 37 and 32 K when the measuring current is applied in-plane parallel and perpendicular to [001] direction of the substrate. Twin-free non -axis thin films are promising for fabrication of novel planar THz devices.

摘要

通过分子有机化学气相沉积(MOCVD)在(110)SrTiO₃和(110)LaAlO₃衬底上生长了(117)Bi₂Sr₂Ca₂CuO(Bi - 2212)薄膜。衬底是倾斜的,倾斜角高达20°。薄膜是三维外延的,X射线衍射扫描表明,虽然在平坦衬底上生长的薄膜由孪晶晶粒组成,但在倾斜衬底上的薄膜是……如果在两个温度下进行生长,则可获得更高的质量:生长在550⁻600°C开始,并在700⁻750°C继续。当测量电流沿面内平行和垂直于衬底的[001]方向施加时,通过双温法生长的无孪晶薄膜显示出37 K和32 K的零电阻临界温度。无孪晶非轴向薄膜有望用于制造新型平面太赫兹器件。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/c7319df6f767/materials-12-01124-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/550b185ca7f2/materials-12-01124-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/ce5cb6100e6a/materials-12-01124-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/e072b4374814/materials-12-01124-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/64c1c7bec7a2/materials-12-01124-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/25de04d3daa5/materials-12-01124-g005a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/249834bf37a2/materials-12-01124-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/2705017b49d0/materials-12-01124-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/334c711bb6cc/materials-12-01124-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/c7319df6f767/materials-12-01124-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/550b185ca7f2/materials-12-01124-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/ce5cb6100e6a/materials-12-01124-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/e072b4374814/materials-12-01124-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/64c1c7bec7a2/materials-12-01124-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/25de04d3daa5/materials-12-01124-g005a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/249834bf37a2/materials-12-01124-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/2705017b49d0/materials-12-01124-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/334c711bb6cc/materials-12-01124-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ba2e/6479393/c7319df6f767/materials-12-01124-g009.jpg

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