Constraints on possible mechanisms for high-Tc superconductivity

This paper discusses a phenomenological model used to describe various properties of a dx²−y² superconductor in its temperature as well as frequency dependence, namely, the London penetration depth, the optical conductivity, the microwave conductivity, and the electronic thermal conductivity. We ass...

Повний опис

Збережено в:
Бібліографічні деталі
Дата:1998
Автори: Schürrer, I., Schachinger, E.
Формат: Стаття
Мова:English
Опубліковано: Інститут фізики конденсованих систем НАН України 1998
Назва видання:Condensed Matter Physics
Онлайн доступ:http://dspace.nbuv.gov.ua/handle/123456789/118623
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Назва журналу:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Цитувати:Constraints on possible mechanisms for high-Tc superconductivity / E. Schachinger, I. Schürrer // Condensed Matter Physics. — 1998. — Т. 1, № 1(13). — С. 69-87. — Бібліогр.: 34 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
Опис
Резюме:This paper discusses a phenomenological model used to describe various properties of a dx²−y² superconductor in its temperature as well as frequency dependence, namely, the London penetration depth, the optical conductivity, the microwave conductivity, and the electronic thermal conductivity. We assume the CuO₂ planes to be the dominant feature for superconductivity and develop a 2D-formalism in which inelastic scattering is modelled explicitly by a spectral density which describes a fluctuation spectrum responsible for the superconducting transition and also for the large inelastic scattering observed in the normal state above the critical temperature Tc . The feedback effect of superconductivity on the spectral density is modelled by a temperature dependent low frequency cutoff. Theoretical results are compared with the experimental data and the fact that such a model allows a consistent description of a variety of phenomena is then used to formulate constraints on possible mechanisms of superconductivity in oxides.