Two-dimensional geometry of spin excitations in the high-transition-temperature superconductor YBa2Cu3O6+x
V. Hinkov,
S. Pailhès,
P. Bourges,
Y. Sidis,
A. Ivanov,
A. Kulakov,
C. T. Lin,
D. P. Chen,
C. Bernhard and
B. Keimer ()
Additional contact information
V. Hinkov: Max-Planck-Institut für Festkörperforschung
S. Pailhès: Laboratoire Léon Brillouin, CEA-CNRS, CE-Saclay
P. Bourges: Laboratoire Léon Brillouin, CEA-CNRS, CE-Saclay
Y. Sidis: Laboratoire Léon Brillouin, CEA-CNRS, CE-Saclay
A. Ivanov: Institut Laue-Langevin, 156X
A. Kulakov: Max-Planck-Institut für Festkörperforschung
C. T. Lin: Max-Planck-Institut für Festkörperforschung
D. P. Chen: Max-Planck-Institut für Festkörperforschung
C. Bernhard: Max-Planck-Institut für Festkörperforschung
B. Keimer: Max-Planck-Institut für Festkörperforschung
Nature, 2004, vol. 430, issue 7000, 650-654
Abstract:
Abstract The fundamental building block of the copper oxide superconductors is a Cu4O4 square plaquette. The plaquettes in most of these materials are slightly distorted to form a rectangular lattice, for which an influential theory predicts that high-transition-temperature (high-Tc) superconductivity is nucleated in ‘stripes’ aligned along one of the axes1,2,3. This theory received strong support from experiments that indicated a one-dimensional character for the magnetic excitations in the high-Tc material YBa2Cu3O6.6 (ref. 4). Here we report neutron scattering data on ‘untwinned’ YBa2Cu3O6+x crystals, in which the orientation of the rectangular lattice is maintained throughout the entire volume. Contrary to the earlier claim4, we demonstrate that the geometry of the magnetic fluctuations is two-dimensional. Rigid stripe arrays therefore appear to be ruled out over a wide range of doping levels in YBa2Cu3O6+x, but the data may be consistent with liquid-crystalline stripe order5. The debate about stripes has therefore been reopened.
Date: 2004
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DOI: 10.1038/nature02774
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