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      In-plane anisotropy of spin excitations in the normal and superconducting states of underdoped YBa\(_2\)Cu\(_3\)O\(_{6+x}\)

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          Abstract

          A detailed inelastic neutron scattering study of the in-plane anisotropy of magnetic excitations in twin-free YBa\(_2\)Cu\(_3\)O\(_{6.6}\) (\(T_c =\) 61 K) reveals that the spin excitation spectra in the superconducting and normal states are qualitatively different. Below \(T_c\), the spectrum consists of upward- and downward-dispersing branches with modest in-plane anisotropy merging at an energy \(E_{res} =\) 37.5 meV. In the normal state, the singularity at \(E_{res}\) disappears, and the spectrum exhibits a steep dispersion with a strongly anisotropic in-plane geometry. These data have important implications for models based on static or dynamic "stripe" order of spins and charges.

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          Two-Dimensional Geometry of Spin Excitations in the High Temperature Superconductor YBa2Cu3O6+x

          The fundamental building block of the copper oxide superconductors is a Cu4O4 square plaquette. In most of these materials, the plaquettes are slightly distorted and form a rectangular lattice. An influential theory predicts that high-temperature superconductivity is nucleated in "stripes" aligned along one of the axes of this lattice. This theory had received strong support from experiments that appeared to indicate a one-dimensional character of the magnetic excitations in the high temperature superconductor YBa2Cu3O6.6. 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 claim, 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 order.
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            The Spin Excitation Spectrum in Superconducting \({\bf YBa_2Cu_3O_{6.85}}\)

            A comprehensive inelastic neutron scattering study of magnetic excitations in the near-optimally doped high-temperature superconductor \({\rm YBa_{2}Cu_{3}O_{6.85}}\) is presented. The spin correlations in the normal state are commensurate with the crystal lattice, and the intensity is peaked around the wave vector characterizing the antiferromagnetic state of the insulating precursor \({\rm YBa_{2}Cu_{3}O_{6}}\). Profound modifications of the spin excitation spectrum appear abruptly below the superconducting transition temperature, \(\rm T_C\), where a commensurate resonant mode and a set of weaker incommensurate peaks develop. The data are consistent with models based on an underlying two-dimensional Fermi surface that predict a continuous, downward dispersion relation connecting the resonant mode and the incommensurate excitations. The magnetic incommensurability in the \({\rm YBa_{2}Cu_{3}O_{6+x}}\) system is thus not simply related to that of another high temperature superconductor, \({\rm La_{2-x}Sr_xCuO_{4}}\), where incommensurate peaks persist well above \(\rm T_C\). The temperature dependent incommensurability is difficult to reconcile with interpretations based on charge stripe formation in \({\rm YBa_{2}Cu_{3}O_{6+x}}\) near optimum doping.
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              FLOTATION | Pre-aeration of Feed

              M XU, Z. Zhou, Z Xu (2000)
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                Author and article information

                Journal
                2006-01-03
                2006-01-05
                Article
                10.1038/nphys720
                cond-mat/0601048
                aa9af569-a337-4627-a7b6-22be30606582
                History
                Custom metadata
                Nature Physics 3, 780 (2007)
                New version with no changes of the contents, but now all figures in .EPS
                cond-mat.str-el cond-mat.supr-con

                Condensed matter
                Condensed matter

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