By Anant V. Narlikar
Frontiers in Superconducting Materials supplies a state of the art document of crucial themes of the present study in superconductive fabrics and comparable phenomena. It includes 30 chapters written through popular overseas specialists within the box. it's of vital curiosity to researchers and experts in Physics and fabrics technology, either in educational and business learn, in addition to complicated scholars. It additionally addresses digital and electric engineers. Even non-specialists drawn to superconductivity may perhaps locate a few valuable answers.
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B1 or A15 compounds, is made of only two elements. Each element contributes an additional degree of freedom to the preparation route towards new compounds. For the metallurgist, this translates roughly into one order of magnitude more elaborate exploratory efforts. A new cuprate HTS compound requires therefore typically as much metallurgical optimization work as 100 binary compounds. As a further complication, the large number of adjacent phases in the phase diagram constituted by the contributing elements hamper the preparation of phase pure quaternary or quinary cuprates.
X. Xi Introduction Difficulties in Depositing MgB2 Films Deposition Techniques for MgB2 Properties of Clean Epitaxial HPCVD Films Properties of Carbon-Doped HPCVD Films Substrates and Heterostructures MgB2 Thin Film Devices Conclusions References 1073 1074 1076 1078 1080 1082 1084 1085 1086 SUBJECT INDEX 1093 SUPERCONDUCTING MATERIALS – A TOPICAL OVERVIEW Roland Hott1, Reinhold Kleiner2, Thomas Wolf1, and Gertrud Zwicknagl3 1 Forschungszentrum Karlsruhe, Institut für Festkörperphysik, P. O. Box 3640, 76021 Karlsruhe, GERMANY 2 Physikalisches Institut - Experimentalphysik II, Universität Tübingen, 72076 Tübingen, GERMANY 3 Institut für Mathematische Physik, Technische Universität Braunschweig, 38106 Braunschweig, GERMANY 1.
4). This quasi-2-dimensional nature of superconductivity in HTS leads to a pronounced anisotropy of the SC properties with much higher supercurrents along the CuO2 planes than in 30 31 In NCCO low-energy excitations are observed for T < 1 K which presumably have their origin in the interaction of the magnetic Nd ions [163,164]. However, this additional physics is not an intrinsic pecularity of electron-doped HTS: GdBa2Cu3O7-δ shows similar effects attributed to the magnetic Gd ions [165,166] but the same “high energy” superconducting behavior as other RE-123 HTS.