Nearly isotropic superconductivity in (Ba,K)Fe2As2

被引:496
作者
Yuan, H. Q. [1 ,2 ]
Singleton, J. [2 ]
Balakirev, F. F. [2 ]
Baily, S. A. [2 ]
Chen, G. F. [3 ]
Luo, J. L. [3 ]
Wang, N. L. [3 ]
机构
[1] Zhejiang Univ, Dept Phys, Hangzhou 310027, Peoples R China
[2] Los Alamos Natl Lab, NHMFL, MS E536, Los Alamos, NM 87545 USA
[3] Chinese Acad Sci, Beijing Natl Lab Condensed Matter Phys, Beijing 10080, Peoples R China
基金
美国国家科学基金会;
关键词
UPPER CRITICAL-FIELD; FERMI-SURFACE;
D O I
10.1038/nature07676
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
Superconductivity was recently observed(1-7) in iron- arsenic- based compounds with a superconducting transition temperature (T-c) as high as 56 K, naturally raising comparisons with the high-T-c copper oxides. The copper oxides have layered crystal structures with quasi- two- dimensional electronic properties, which led to speculation that reduced dimensionality ( that is, extreme anisotropy) is a necessary prerequisite for superconductivity at temperatures above 40 K ( refs 8, 9). Early work on the iron- arsenic compounds seemed to support this view(7,10). Here we report measurements of the electrical resistivity in single crystals of (Ba,K)Fe2As2 in a magnetic field up to 60 T. We find that the superconducting properties are in fact quite isotropic, being rather independent of the direction of the applied magnetic fields at low temperature. Such behaviour is strikingly different from all previously known layered superconductors(9,11), and indicates that reduced dimensionality in these compounds is not a prerequisite for 'high- temperature' superconductivity. We suggest that this situation arises because of the underlying electronic structure of the iron- arsenic compounds, which appears to be much more three dimensional than that of the copper oxides. Extrapolations of low- field single- crystal data incorrectly suggest a high anisotropy and a greatly exaggerated zero- temperature upper critical field.
引用
收藏
页码:565 / 568
页数:4
相关论文
共 27 条
[1]  
ALTARAWNEH M, 2008, DETERMINATION ANISOT
[2]  
Anderson PW., 1997, The Theory of Superconductivity in the High-Tc Cuprate Superconductors
[3]   Resistive upper critical fields and irreversibility lines of optimally doped high-Tc cuprates [J].
Ando, Y ;
Boebinger, GS ;
Passner, A ;
Schneemeyer, LF ;
Kimura, T ;
Okuya, M ;
Watauchi, S ;
Shimoyama, J ;
Kishio, K ;
Tamasaku, K ;
Ichikawa, N ;
Uchida, S .
PHYSICAL REVIEW B, 1999, 60 (17) :12475-12479
[4]   A NOTE ON THE MAXIMUM CRITICAL FIELD OF HIGH-FIELD SUPERCONDUCTORS [J].
CHANDRASEKHAR, BS .
APPLIED PHYSICS LETTERS, 1962, 1 (01) :7-8
[5]   Superconductivity at 41 K and its competition with spin-density-wave instability in layered CeO1-xFxFeAs [J].
Chen, G. F. ;
Li, Z. ;
Wu, D. ;
Li, G. ;
Hu, W. Z. ;
Dong, J. ;
Zheng, P. ;
Luo, J. L. ;
Wang, N. L. .
PHYSICAL REVIEW LETTERS, 2008, 100 (24)
[6]  
CHEN GF, 2008, TRANSPORT ANISOTROPY
[7]   Superconductivity at 43 K in SmFeAsO1-xFx [J].
Chen, X. H. ;
Wu, T. ;
Wu, G. ;
Liu, R. H. ;
Chen, H. ;
Fang, D. F. .
NATURE, 2008, 453 (7196) :761-762
[8]   UPPER LIMIT FOR CRITICAL FIELD IN HARD SUPERCONDUCTORS [J].
CLOGSTON, AM .
PHYSICAL REVIEW LETTERS, 1962, 9 (06) :266-&
[9]   Observation of Fermi-surface-dependent nodeless superconducting gaps in Ba0.6K0.4Fe2As2 [J].
Ding, H. ;
Richard, P. ;
Nakayama, K. ;
Sugawara, K. ;
Arakane, T. ;
Sekiba, Y. ;
Takayama, A. ;
Souma, S. ;
Sato, T. ;
Takahashi, T. ;
Wang, Z. ;
Dai, X. ;
Fang, Z. ;
Chen, G. F. ;
Luo, J. L. ;
Wang, N. L. .
EPL, 2008, 83 (04)
[10]   Limits of the upper critical field in dirty two-gap superconductors [J].
Gurevich, A. .
PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS, 2007, 456 (1-2) :160-169