A calculation method by the improved three-fluid model is shown to describe phenomenologically temperature and frequency dependence of surface resistance Rs for high-Tc superconductors. It is verified that this model is useful to describe temperature dependence of Rs for such high-Tc superconducting films as Y-Ba-Cu-O (YBCO), Eu-Ba-Cu-O, and Tl-Ba-Ca-Cu-O films. For the frequency dependence of Rs of a YBCO bulk, furthermore, the measured results which have not depended on f2 in the frequency range 10-25 GHz, can be described successfully by this model. Finally, a figure of merit is proposed to evaluate material quality for high-Tc superconductors from the values of electron densities and momentum relaxation time determined by the present model.
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Tadashi IMAI, Yoshio KOBAYASHI, "Phenomenological Description of Temperature and Frequency Dependence of Surface Resistance of High-Tc Superconductors by Improved Three-Fluid Model" in IEICE TRANSACTIONS on Electronics,
vol. E78-C, no. 5, pp. 498-502, May 1995, doi: .
Abstract: A calculation method by the improved three-fluid model is shown to describe phenomenologically temperature and frequency dependence of surface resistance Rs for high-Tc superconductors. It is verified that this model is useful to describe temperature dependence of Rs for such high-Tc superconducting films as Y-Ba-Cu-O (YBCO), Eu-Ba-Cu-O, and Tl-Ba-Ca-Cu-O films. For the frequency dependence of Rs of a YBCO bulk, furthermore, the measured results which have not depended on f2 in the frequency range 10-25 GHz, can be described successfully by this model. Finally, a figure of merit is proposed to evaluate material quality for high-Tc superconductors from the values of electron densities and momentum relaxation time determined by the present model.
URL: https://global.ieice.org/en_transactions/electronics/10.1587/e78-c_5_498/_p
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@ARTICLE{e78-c_5_498,
author={Tadashi IMAI, Yoshio KOBAYASHI, },
journal={IEICE TRANSACTIONS on Electronics},
title={Phenomenological Description of Temperature and Frequency Dependence of Surface Resistance of High-Tc Superconductors by Improved Three-Fluid Model},
year={1995},
volume={E78-C},
number={5},
pages={498-502},
abstract={A calculation method by the improved three-fluid model is shown to describe phenomenologically temperature and frequency dependence of surface resistance Rs for high-Tc superconductors. It is verified that this model is useful to describe temperature dependence of Rs for such high-Tc superconducting films as Y-Ba-Cu-O (YBCO), Eu-Ba-Cu-O, and Tl-Ba-Ca-Cu-O films. For the frequency dependence of Rs of a YBCO bulk, furthermore, the measured results which have not depended on f2 in the frequency range 10-25 GHz, can be described successfully by this model. Finally, a figure of merit is proposed to evaluate material quality for high-Tc superconductors from the values of electron densities and momentum relaxation time determined by the present model.},
keywords={},
doi={},
ISSN={},
month={May},}
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TY - JOUR
TI - Phenomenological Description of Temperature and Frequency Dependence of Surface Resistance of High-Tc Superconductors by Improved Three-Fluid Model
T2 - IEICE TRANSACTIONS on Electronics
SP - 498
EP - 502
AU - Tadashi IMAI
AU - Yoshio KOBAYASHI
PY - 1995
DO -
JO - IEICE TRANSACTIONS on Electronics
SN -
VL - E78-C
IS - 5
JA - IEICE TRANSACTIONS on Electronics
Y1 - May 1995
AB - A calculation method by the improved three-fluid model is shown to describe phenomenologically temperature and frequency dependence of surface resistance Rs for high-Tc superconductors. It is verified that this model is useful to describe temperature dependence of Rs for such high-Tc superconducting films as Y-Ba-Cu-O (YBCO), Eu-Ba-Cu-O, and Tl-Ba-Ca-Cu-O films. For the frequency dependence of Rs of a YBCO bulk, furthermore, the measured results which have not depended on f2 in the frequency range 10-25 GHz, can be described successfully by this model. Finally, a figure of merit is proposed to evaluate material quality for high-Tc superconductors from the values of electron densities and momentum relaxation time determined by the present model.
ER -