Interplay of electron-lattice interactions and superconductivity in Bi2Sr2CaCu2O8+δ

被引:306
作者
Lee, Jinho
Fujita, K.
McElroy, K.
Slezak, J. A.
Wang, M.
Aiura, Y.
Bando, H.
Ishikado, M.
Masui, T.
Zhu, J. -X.
Balatsky, A. V.
Eisaki, H.
Uchida, S.
Davis, J. C. [1 ]
机构
[1] Cornell Univ, Dept Phys, LASSP, Ithaca, NY 14853 USA
[2] Univ Tokyo, Dept Phys, Tokyo 1138656, Japan
[3] Univ Calif Berkeley, Lawrence Berkeley Lab, Div Mat Sci, Berkeley, CA 94720 USA
[4] AIST, Tsukuba, Ibaraki 3058568, Japan
[5] Osaka Univ, Dept Phys, Osaka 5600043, Japan
[6] Los Alamos Natl Lab, Div Theoret, Los Alamos, NM 87545 USA
关键词
TRANSITION-TEMPERATURE SUPERCONDUCTOR; COPPER-OXIDE SUPERCONDUCTORS; LINE-SHAPE; T-C; DISPERSION; EXCITATIONS; SPECTROSCOPY;
D O I
10.1038/nature04973
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
Formation of electron pairs is essential to superconductivity. For conventional superconductors, tunnelling spectroscopy has established that pairing is mediated by bosonic modes (phonons); a peak in the second derivative of tunnel current d(2)I/dV(2) corresponds to each phonon mode(1-3). For high-transition-temperature (high-T-c) superconductivity, however, no boson mediating electron pairing has been identified. One explanation could be that electron pair formation(4) and related electron - boson interactions are heterogeneous at the atomic scale and therefore challenging to characterize. However, with the latest advances in d(2)I/dV(2) spectroscopy using scanning tunnelling microscopy, it has become possible to study bosonic modes directly at the atomic scale(5). Here we report d(2)I/dV(2) imaging(6-8) studies of the high-T-c superconductor Bi2Sr2CaCu2O8+delta. We find intense disorder of electron - boson interaction energies at the nanometre scale, along with the expected modulations in d(2) I/dV(2) ( refs 9, 10). Changing the density of holes has minimal effects on both the average mode energies and the modulations, indicating that the bosonic modes are unrelated to electronic or magnetic structure. Instead, the modes appear to be local lattice vibrations, as substitution of O-18 for O-16 throughout the material reduces the average mode energy by approximately 6 per cent - the expected effect of this isotope substitution on lattice vibration frequencies(5). Significantly, the mode energies are always spatially anticorrelated with the superconducting pairing-gap energies, suggesting an interplay between these lattice vibration modes and the superconductivity.
引用
收藏
页码:546 / 550
页数:5
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