Competition between composite and modulated configurations in Bi2Sr2CaCu2O8+δ and its relation to oxygen stoichiometry

J. M. Perez-Mato, J. Etrillard, J. M. Kiat, B. Liang, and C. T. Lin
Phys. Rev. B 67, 024504 – Published 14 January 2003
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Abstract

The possible interpretation of the compound Bi2Sr2CaCu2O8+δ as a composite or a single modulated incommensurate structure is deeply interconnected with the existence of discontinuous atomic domains in the superspace description of the structure. Single-crystal neutron diffraction data have been used to obtain Fourier maps within the superspace description, which show that some atomic domains are indeed either discontinuous, like that of the atoms in the BiO layers, or strongly anharmonic. This contrasts with the structural models of this material, which usually consider a single modulated incommensurate structure with continuous modulations containing a few harmonics. The results demonstrate that these models are bound to yield unrealistic configurations for the so-called bridging zones in the BiO layers. The intrinsic discontinuous features of the atomic modulations, especially the longitudinal sawtooth modulations of the oxygens in the Bi2O2 slabs, are shown to be the signature of two competing length scales corresponding to the Bi2O2 slabs and the perovskite blocks Sr2CaCu2O6. In principle, this feature can be naturally included in a modulated composite description with occupational steplike modulations. An ideal composite configuration can be also proposed as a reference structure for describing the effects of the strong coupling between the Bi2O2 slabs and the perovskite blocks Sr2CaCu2O6, including its effect on the compound stoichiometry, in particular its oxygen content.

  • Received 25 July 2002

DOI:https://doi.org/10.1103/PhysRevB.67.024504

©2003 American Physical Society

Authors & Affiliations

J. M. Perez-Mato1,2, J. Etrillard1,3, J. M. Kiat1,4, B. Liang5, and C. T. Lin5

  • 1Laboratoire Léon Brillouin, CEA-CNRS, CE Saclay, 91191 Gif sur Yvette Cedex, France
  • 2Departamento de Física de la Materia Condensada, Facultad de Ciencias, Universidad del País Vasco, Apdo. 644, 48080 Bilbao, Spain
  • 3Groupe Matière Condensée et Matériaux, UMR au CNRS 6626, Université de Rennes I, 35042 Rennes Cedex, France
  • 4Laboratoire Structures, Propriétés et Modélisation des Solides, UMR au CNRS 8580, Ecole Centrale Paris, 92295 Châtenay-Malabry Cedex, France
  • 5Max-Planck-Institute for Solid State Research, 70569 Stuttgart, Germany

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Vol. 67, Iss. 2 — 1 January 2003

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