By Neeraj Khare
Dedicated to the practise, characterization, and overview of HTS digital units, the "Handbook of High-Temperature Superconductor Electronics" offers details on utilizing high-Tc skinny motion pictures and junctions to extend pace, reduce noise, decrease energy intake and improve higher frequency limits in superconductor electronics. Compiled through a gaggle of across the world well known authors, it discusses the implementation of HTS electronic circuits, microwave filters and subsystems and transition-edge bolometers. different themes contain cryocooler utilization in high-Tc units, HTS skinny motion pictures for digital units, and the fabrication and purposes of varied HTS junctions.
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Extra resources for Handbook of High-Temperature Superconductor Electronics (Applied Physics)
In situ growth requires significant and uniform substrate heating in an oxygen ambient during film deposition. For most HTS phases, the temperature range at a given oxygen pressure for achieving optimal Copyright © 2003 by Marcel Dekker, Inc. All Rights Reserved. 40 Norton film properties is rather narrow, on the order of 20–40°C. This proves challenging for large-area, double-sided, or continuous-length deposition of HTS films. In contrast, ex situ processing requires no substrate heating during precursor deposition, greatly simplifying the film-growth apparatus.
33. 23 RJ Cava, B Batlogg, JJ Krajewski, R Farrow, LW Rupp, AE White Jr, K Short, T Kometani. 4BiO3 Perovskite. Nature 332:814–816, 1988. YS Yao, YF Xiong, D Jin, JW Li, JL Luo, ZX Zhao. 5Ba2Cu3Oz. Physica C 282–287:49–52, 1997. SSP Parkin, VY Lee, AI Nazzal, R Savoy, R Beyers, SJ LaPlaca. Tl1CanϪ1Ba2CunO2nϩ3 (nϭ1,2,3): A new class of crystal structures exhibiting volume superconductivity at up to Ӎ 110 K. Phys Rev Lett 61:750–753, 1988. SN Putillin, EV Antipov, M Marezio. Superconductivity above 120 K in HgBa2CaCu2O6ϩ␦.
Compared to the other HTS materials, epitaxial YBa2Cu3O7 films are the easiest to synthesize and achieve a Tc for the film that is near the bulk value. This is due, in part, to the relative stability of the YBa2Cu3O7 phase, as there are no n ϭ 1 or n ϭ 3 members to compete with in phase formation. 11, can be derived by stacking three oxygen-deficient perovskite unit cells (ACuOy) in the layered sequence BaO–CuO2–Y–CuO2– BaO–CuO. YBa2Cu3O7 contains two CuO2 planes per unit cell separated by an Y atom.