Spin dynamics in the pseudogap state of a high-temperature superconductor

被引:198
作者
Hinkov, V.
Bourges, P.
Pailhes, S.
Sidis, Y.
Ivanov, A.
Frost, C. D.
Perring, T. G.
Lin, C. T.
Chen, D. P.
Keimer, B. [1 ]
机构
[1] Max Planck Inst Solid State Res, D-70569 Stuttgart, Germany
[2] CEA, CNRS, CE Saclay, Lab Leon Brillouin, F-91191 Gif Sur Yvette, France
[3] Inst Max Von Laue Paul Langevin, F-38042 Grenoble, France
[4] Rutherford Appleton Lab, ISIS Facil, Didcot OX11 0QX, Oxon, England
关键词
D O I
10.1038/nphys720
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
The pseudogap is one of the most pervasive phenomena of high-temperature superconductors(1). It is attributed either to incoherent Cooper pairing setting in above the superconducting transition temperature, T c, or to a hidden order parameter competing with superconductivity. Here, we use inelastic neutron scattering from underdoped YBa2Cu3O6.6 to show that the dispersion relations of spin excitations in the superconducting and pseudogap states are qualitatively different. Specifically, the extensively studied 'hour glass' shape of the magnetic dispersions in the superconducting state(2-4) is no longer discernible in the pseudogap state and we observe an unusual 'vertical' dispersion with pronounced in-plane anisotropy. The differences between superconducting and pseudogap states are thus more profound than generally believed, suggesting a competition between these two states. Whereas the high-energy excitations are common to both states and obey the symmetry of the copper oxide square lattice, the low-energy excitations in the pseudogap state may be indicative of collective fluctuations towards a state with broken orientational symmetry predicted in theoretical work(5-8).
引用
收藏
页码:780 / 785
页数:6
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