By Anant V. Narlikar
ISBN-10: 3540245138
ISBN-13: 9783540245131
Frontiers in Superconducting Materials provides a state of the art file of an important issues of the present study in superconductive fabrics and comparable phenomena. It includes 30 chapters written through well known foreign specialists within the box. it's of crucial curiosity to researchers and experts in Physics and fabrics technological know-how, either in educational and commercial examine, in addition to complex 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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Extra info for Frontiers in Superconducting Materials
Sample text
Schematics of the HTS microstructure: Differently oriented single crystal grains are separated by regions filled with secondary phases. In addition, oxygen depletion may occur at grain boundaries. Fig. 9. Basic grain boundary geometries and experimentally observed Jc reduction Jc ~e-α/α0 as function of the misalignment angle α: α0 ≈ 5° for A) and B), α0 ≈ 3° for C) independent of temperature [178,179]. Fig. 10. Schematics of a boundary between HTS grains. Misorientation of the SC d-wave order parameter leads to partial cancellation of the supercurrents modified by the faceting of the grain boundaries.
In addition, oxygen depletion may occur at grain boundaries. Fig. 9. Basic grain boundary geometries and experimentally observed Jc reduction Jc ~e-α/α0 as function of the misalignment angle α: α0 ≈ 5° for A) and B), α0 ≈ 3° for C) independent of temperature [178,179]. Fig. 10. Schematics of a boundary between HTS grains. Misorientation of the SC d-wave order parameter leads to partial cancellation of the supercurrents modified by the faceting of the grain boundaries. 19 Another obstacle for supercurrents in HTS is misalignment of the grains: Exponential degradation of the supercurrent transport is observed as a function of the misalignment angle (see Fig.
A sophisticated process control during sample preparation is essential in order to reduce the amount of such stacking faults. 20 Since the CuO2 layers in YBCO are hole-doped this amounts to a reduction of the hole doping compared to the (hypothetical) canonical Cu-1212 compound. 10 The big metallurgical challenge introduced by the cuprate HTS materials in a previously unknown extent is the large number of chemical degrees of freedom of such materials. Binary compounds may have a 1-dimensional homogeneity range, e.
Frontiers in Superconducting Materials by Anant V. Narlikar
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