NMR and NQR Studies of Spin Dynamics and Superconductivity in High-T-c Oxides

被引:23
|
作者
Kitaoka, Y. [1 ]
Ishida, K. [1 ]
Ohsugi, S. [1 ]
Fujiwara, K. [1 ]
Zheng, G. -Q. [1 ]
Asayama, K. [1 ]
机构
[1] Osaka Univ, Dept Mat Phys, Fac Engn Sci, Toyonaka, Osaka 560, Japan
关键词
D O I
10.1007/BF03166283
中图分类号
O64 [物理化学(理论化学)、化学物理学]; O56 [分子物理学、原子物理学];
学科分类号
070203 ; 070304 ; 081704 ; 1406 ;
摘要
The magnetic and superconducting properties in the high-T-c cuprates have been investigated over a wide hole doping range by Cu-63, O-17 and Tl-205 NMR and NQR in the lightly-doped La2-xSrxCuO4 (LSCO), the heavily-doped Tl2Ba2CuO6+y (TBCO) and the Zn-doped YBa2Cu3O7 (YBCO7). In low doping region, the large antiferromagnetic (AF) spin correlation around the zone boundary (q = Q) causes the Curie-Weiss behavior of (63)(1/T1T) associated with that of the staggered susceptibility chi(Q)(T) in LSCO. In the vicinity of the hole content where T-c has a peak, the AF spin correlation still survives, although the magnetic coherence length xi(M) is considerably short being presumably (xi(M)/a) similar to 1. The further doping destroys progressively the AF spin correlation, which is no longer present is non-superconducting TBCO compounds. These NMR evidences signify that there is an intimate relation between the presence of the AF spin correlation and the onset of the superconductivity. The local collapse of AF spin correlation is a primary cause for the unexpected strong reduction of T-c in case of the substitution of Zn impurities into the CuO2 plane. The superconducting properties clarified by NMR experiments cannot be accounted for by the conventional BCS model or other isotropic s-wave models. A d-wave model is applicable in interpreting consistently most of the NMR results, if the finite density of states at the Fermi level is taken into consideration and is associated with the pair breaking effect. There are increasing evidences that the magnetic mechanism for the superconductivity is promising in high-T-c cuprates.
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收藏
页码:549 / 596
页数:48
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