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Features of growth of non-cubic bicrystals from the melt (example of leucosapphire and neodymium gallate)

机译:熔体中非立方双晶的生长特征(隐色蓝宝石和没食子酸钕)

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Neodymium gallate (NdGaO_3) and sapphire (Al_2O_3) are most suitable materials to produce bicrystal substrates for high-temperature superconducting (HTSC) films' microwaves Josephson junctions. Perfect bicrystal border is important for the devices, and it can be obtained in bicrystals grown directly from the melt. Unfortunately both materials have non-cubic symmetry and anisotropic thermophysical properties what complicates the bicrystal growth process. The experimental results of NdGaO_3 bicrystals growth by Czochralski method using compound bicrystal seeds with different symmetries in the plane perpendicular to the growth axis are presented. The results proved to be very unstable and depended critically upon growth conditions and on bicrystal border orientation. The bicrystals with misorientation angle 180° which correspond to the natural (110) twins are grown. When bicrystal angles are within 22-28 ° range which is optimum for bicrystal Josephson junctions it is very difficult to grow the long bicrystals: the bicrystal border goes out of the crystal quickly. It is supposed that in the last case the symmetry of compound bicrystal seed in the plane perpendicular to the growth direction can differ from the heat field symmetry in the growth system. Requirements for growth of anisotropic crystals by Czochralski method are formulated. It is shown that the requirements of seed and heat field symmetry correspondence can be satisfied more easily in Stepanov's growth method (EFG). The sapphire bicrystal ribbons suitable for manufacturing of high quality substrates for HTSC film Josephson junctions using Stepanov's method are grown.
机译:镓酸钕(NdGaO_3)和蓝宝石(Al_2O_3)是生产高温超导(HTSC)薄膜微波约瑟夫森结的双晶衬底的最合适材料。完美的双晶边界对器件很重要,并且可以直接从熔体中生长出双晶来获得。不幸的是,两种材料都具有非立方对称性和各向异性的热物理性质,这使双晶的生长过程变得复杂。提出了用直拉法在垂直于生长轴的平面上具有不同对称性的复合双晶种通过Czochralski法生长NdGaO_3双晶的实验结果。结果证明是非常不稳定的,并且主要取决于生长条件和双晶边界取向。生长了与自然孪晶(110)相对应的取向角为180°的双晶。当双晶角在22-28°的范围内(对于双晶约瑟夫森结最合适)时,很难长长的双晶:双晶边界迅速脱离晶体。假定在最后一种情况下,化合物双晶种在垂直于生长方向的平面内的对称性可能不同于生长系统中的热场对称性。提出了通过直拉法生长各向异性晶体的要求。结果表明,采用Stepanov生长方法(EFG)可以更容易地满足种子和热场对称对应的要求。生长出适用于使用Stepanov方法制造HTSC薄膜约瑟夫森结的高质量衬底的蓝宝石双晶带。

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