Relating atomic-scale electronic phenomena to wave-like quasiparticle states in superconducting Bi2Sr2CaCu2O8+δ

被引:406
作者
McElroy, K
Simmonds, RW
Hoffman, JE
Lee, DH
Orenstein, J
Eisaki, H
Uchida, S
Davis, JC [1 ]
机构
[1] Univ Calif Berkeley, Dept Phys, Berkeley, CA 94720 USA
[2] Univ Calif Berkeley, Lawrence Berkeley Lab, Div Mat Sci, Berkeley, CA 94720 USA
[3] Tsinghua Univ, Ctr Adv Study, Beijing 100084, Peoples R China
[4] AIST, Tsukuba, Ibaraki 3058568, Japan
[5] Univ Tokyo, Dept Phys, Bunkyo Ku, Tokyo 1138656, Japan
[6] Cornell Univ, Dept Phys, LASSP, Ithaca, NY 14850 USA
基金
美国国家科学基金会;
关键词
D O I
10.1038/nature01496
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
The electronic structure of simple crystalline solids can be completely described in terms either of local quantum states in real space (r-space), or of wave-like states defined in momentum-space (k-space). However, in the copper oxide superconductors, neither of these descriptions alone may be sufficient. Indeed, comparisons between r-space(1-5) and k-space(6-13) studies of Bi2Sr2CaCu2O8+delta (Bi-2212) reveal numerous unexplained phenomena and apparent contradictions. Here, to explore these issues, we report Fourier transform studies of atomic-scale spatial modulations in the Bi-2212 density of states. When analysed as arising from quasiparticle interference(14-16), the modulations yield elements of the Fermi-surface and energy gap in agreement with photoemission experiments(12,13). The consistency of numerous sets of dispersing modulations with the quasiparticle interference model shows that no additional order parameter is required. We also explore the momentum-space structure of the unoccupied states that are inaccessible to photoemission, and find strong similarities to the structure of the occupied states. The copper oxide quasiparticles therefore apparently exhibit particle-hole mixing similar to that of conventional superconductors. Near the energy gap maximum, the modulations become intense, commensurate with the crystal, and bounded by nanometre-scale domains(4). Scattering of the antinodal quasiparticles is therefore strongly influenced by nanometre-scale disorder.
引用
收藏
页码:592 / 596
页数:6
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