上部结构
四方晶系
超导电性
结晶学
转变温度
晶体结构
X射线晶体学
高温超导
无机化合物
材料科学
衍射
分析化学(期刊)
化学
凝聚态物理
物理
热力学
有机化学
色谱法
光学
作者
C.C. Torardi,M.A. Subramanian,J. C. CALABRESE,J. Gopalakrishnan,K. J. Morrissey,T.R. Askew,R. B. Flippen,U. Chowdhry,A.W. Sleight
出处
期刊:Science
[American Association for the Advancement of Science (AAAS)]
日期:1988-04-29
卷期号:240 (4852): 631-634
被引量:439
标识
DOI:10.1126/science.240.4852.631
摘要
There is now a new series of high-temperature superconductors that may be represented as (A(III)O)(2)A(2)(II)Can-1CunO2+2n where A(III) is Bi or Tl, A(II) is Ba or Sr, and n is the number of Cu-O sheets stacked consecutively. There is a general trend toward higher transition temperatures as n increases. The highest n value for a bulk phase is three and is found when A(III) is Tl. This compound, Tl(2)Ba(2)Ca(2)Cu(3)O(10), has the highest transition temperature( approximately 125 K) of any presently known bulk superconductor. The structure of Tl(2)Ba(2)Ca(2)Cu(3)O(10) has been determined from single-crystal x-ray diffraction data and is tetragonal, with a = 3.85 A and c = 35.9 A. No superstructure is observed, and the material is essentially twin-free. Electron microscopy in the Tl/Ba/Ca/Cu/O system has revealed intergrowths where n = 5; such regions may well be responsible for the superconducting onset behavior observed in this system at about 140 K.
科研通智能强力驱动
Strongly Powered by AbleSci AI