简介概要

Temperature Dependence of phase Transitions and Superconductivity in YBa2Cu3O7-X

来源期刊:JOURNAL OF MATERIALS SCIENCE TECHNOLOG1989年第3期

论文作者:张彦生 田兴 陆兴 李晓丽 滕颖丽 庞旭

文章页码:164 - 169

摘    要:<正> By means of X-ray diffraction investigationsand electric resistivity measurements the tempera-ture dependence of phase structure and supercon-ductivity in YBa2Cu3O7x over the temperaturerange of 20℃-950℃ have been studied.The latticeparameters a,b and c as well as conductivityas a function of annealing temperatures canbe roughly divided into three zones which aresuperconductive orthorhombic structure 1(a<bc/3)at 20℃-500℃,normal conductive orthorhombicstructure 2(a<b<c/3)from 550℃ to about 750℃and semiconductive-like tetragonal structure(a=b<c/3)from about 800℃ to 950℃.However,the boundaries of the three zones is not muchdistinctive because there is a continuous transi-tion from the orthorhombic to tetragonal struc-ture.Furthermore,the processes of orthorhom-bic-tetragonal transition in the range of350℃-950℃ are not only continuous but alsoreversible.The isothermal transition oforthorhombic 2 to orthorhombic 1 occurs at350℃-500℃,while the maximum rate of transitionand high Tc superconductivity can be obtainedat about 460℃.This process of isothermaltransition depends on the ordering of oxygenatoms or vacancies and the thermodynamicequilibrium to allow the oxygen diffusion.

详情信息展示

Temperature Dependence of phase Transitions and Superconductivity in YBa2Cu3O7-X

张彦生,田兴,陆兴,李晓丽,滕颖丽,庞旭

摘 要:<正> By means of X-ray diffraction investigationsand electric resistivity measurements the tempera-ture dependence of phase structure and supercon-ductivity in YBa2Cu3O7x over the temperaturerange of 20℃-950℃ have been studied.The latticeparameters a,b and c as well as conductivityas a function of annealing temperatures canbe roughly divided into three zones which aresuperconductive orthorhombic structure 1(a<bc/3)at 20℃-500℃,normal conductive orthorhombicstructure 2(a<b<c/3)from 550℃ to about 750℃and semiconductive-like tetragonal structure(a=b<c/3)from about 800℃ to 950℃.However,the boundaries of the three zones is not muchdistinctive because there is a continuous transi-tion from the orthorhombic to tetragonal struc-ture.Furthermore,the processes of orthorhom-bic-tetragonal transition in the range of350℃-950℃ are not only continuous but alsoreversible.The isothermal transition oforthorhombic 2 to orthorhombic 1 occurs at350℃-500℃,while the maximum rate of transitionand high Tc superconductivity can be obtainedat about 460℃.This process of isothermaltransition depends on the ordering of oxygenatoms or vacancies and the thermodynamicequilibrium to allow the oxygen diffusion.

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