By Paolo Mele, Tamio Endo, Shunichi Arisawa, Chaoyang Li, Tetsuo Tsuchiya
This e-book presents a entire evaluate of the technology of nanostructured oxides. It information the basic strategies and methodologies taken with oxides skinny movie and bulk progress, characterization and equipment processing, in addition to heterostructures. either, specialists in oxide nanostructures and specialists in skinny movie heteroepitaxy, give a contribution the interactions defined inside this book.
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Extra resources for Oxide Thin Films, Multilayers, and Nanocomposites
F. at 77 K for standard TFA- MOD (Y,Gd)BCO CCs. f. f. of 1 cm-width CCs saturates at thicker films shown in Fig. 19b. These saturation phenomena is generally related to blocking current at upper layer of films by pore , a-axis grain [30, 51], and second phase . f. values at thicker films, cross-sectional TEM images and EDS mappings of the standard (Y,Gd)BCO thick CCs were analyzed (Fig. 20a). We made two important observations: (1) many large RE2Cu2O5 precipitates were observed especially in the upper region, and (2) the average composition shows a variation in the thickness direction, and the upper region is Y and Cu rich.
22nd Intl. Conf. Composites/Nano Engineering (ICCE-22, Malta, 2014) 9. K. Endo, P. Badica, S. Arisawa, H. Kezuka, T. Endo, Growth aspect of thin-film composite heterostructures of 006Fxide multicomponent perovskites for electronics. Jpn. J. Appl. Phys. 51, 11PG09-1–11PG09-6 (2012) Chapter 3 High Tc Superconductivity in Engineered Cuprate Heterostructures Daniele Di Castro and Giuseppe Balestrino Abstract Given the layered structure of cuprate high-transition-temperature superconductors (HTS), essentially constituted by infinite layer (IL) blocks, containing the CuO2 planes, separated by charge reservoir (CR) blocks, the use of heterostructures and superlattices, made by stacking HTS with different magnetic and conductivity properties (metallic, superconducting, insulating), such as YBa2Cu3O7−x, PrBa2Cu3O7−x, and Bi2Sr2CunCan−1Ox, have been extensively exploited to investigate many fundamental issues in HTS physics.
1). Nonsuperconducting blocks play the role of charge reservoir, while Cu–O planes of the superconducting blocks are the easy transport path of the super carriers. Out-of-plane transport is also possible and, along the c-axis direction, HTS can be described as an array of superconductor-insulator-superconductor tunneling junctions, the so-called Josephson junctions. 87nm Bi-2223 Fig. 1 HTS c-axis type heterostructure composed of half c-axis Bi-2212 and Bi-2223 HTS phases and forming a SIS Josephson junction 2 Substrate-Film Lattice Engineering for the Growth… 29 described as an intrinsic heterostructure showing Josephson junction tunneling properties.