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过掺杂高温超导体中的共振自旋激发

Resonant spin excitation in an overdoped high temperature superconductor.

作者信息

He H, Sidis Y, Bourges P, Gu G D, Ivanov A, Koshizuka N, Liang B, Lin C T, Regnault L P, Schoenherr E, Keimer B

机构信息

Max-Planck-Institut für Festkörperforschung, Stuttgart, Germany.

出版信息

Phys Rev Lett. 2001 Feb 19;86(8):1610-3. doi: 10.1103/PhysRevLett.86.1610.

DOI:10.1103/PhysRevLett.86.1610
PMID:11290205
Abstract

An inelastic neutron scattering study of overdoped Bi(2)Sr(2)CaCu(2)O(8+delta) ( T(c) = 83 K) has revealed a resonant spin excitation in the superconducting state. The mode energy is E(res) = 38.0 meV, significantly lower than in optimally doped Bi(2)Sr(2)CaCu(2)O(8+delta) ( T(c) = 91 K, E(res) = 42.4 meV). This observation, which indicates a constant ratio E(res)/k(B)T(c) approximately 5.4, helps resolve a long-standing controversy about the origin of the resonant spin excitation in high temperature superconductors.

摘要

对过掺杂的Bi(2)Sr(2)CaCu(2)O(8+δ)(Tc = 83 K)进行的非弹性中子散射研究揭示了超导态下的共振自旋激发。该模式能量为E(res)= 38.0毫电子伏,明显低于最佳掺杂的Bi(2)Sr(2)CaCu(2)O(8+δ)(Tc = 91 K,E(res)= 42.4毫电子伏)。这一观察结果表明E(res)/k(B)Tc约为5.4的恒定比值,有助于解决关于高温超导体中共振自旋激发起源的长期争议。

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Disappearance of superconductivity due to vanishing coupling in the overdoped BiSrCaCuO.过掺杂BiSrCaCuO中由于耦合消失导致的超导性消失。
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