Angle-resolved photoemission spectroscopy of Sr2CuO2Cl2

C. Dürr, S. Legner, R. Hayn, S. V. Borisenko, Z. Hu, A. Theresiak, M. Knupfer, M. S. Golden, J. Fink, F. Ronning, Z.-X. Shen, H. Eisaki, S. Uchida, C. Janowitz, R. Müller, R. L. Johnson, K. Rossnagel, L. Kipp, and G. Reichardt
Phys. Rev. B 63, 014505 – Published 11 December 2000
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Abstract

We have investigated the lowest binding-energy electronic structure of the model cuprate Sr2CuO2Cl2 using angle-resolved photoemission spectroscopy. Our data from about 80 cleavages of Sr2CuO2Cl2 single crystals give a comprehensive, self-consistent picture of the nature of the first electron-removal state in this model undoped CuO2-plane cuprate. First, we show a strong dependence on the polarization of the excitation light which is understandable in the context of the matrix element governing the photoemission process, which gives a state with the symmetry of a Zhang-Rice singlet. Secondly, the strong, oscillatory dependence of the intensity of the Zhang-Rice singlet on the exciting photon energy is shown to be consistent with interference effects connected with the periodicity of the crystal structure in the crystallographic c direction. Thirdly, we measured the dispersion of the first electron-removal states along Γ(π,π) and Γ(π,0), the latter being controversial in the literature, and have shown that the data are best fitted using an extended tJ model, and extract the relevant model parameters. An analysis of the spectral weight of the first ionization states for different excitation energies within the approach used by Leung et al. [Phys. Rev. B 56, 6320 (1997)] results in a strongly photon-energy dependent ratio between the coherent and incoherent spectral weight. The possible reasons for this observation and its physical implications are discussed.

  • Received 18 July 2000

DOI:https://doi.org/10.1103/PhysRevB.63.014505

©2000 American Physical Society

Authors & Affiliations

C. Dürr, S. Legner, R. Hayn, S. V. Borisenko, Z. Hu, A. Theresiak, M. Knupfer, M. S. Golden, and J. Fink

  • Institute for Solid State and Materials Research Dresden, P.O. Box 270016, D-01171 Dresden, Germany

F. Ronning and Z.-X. Shen

  • Department of Physics and Stanford Synchrotron Radiation Laboratory, Stanford University, Stanford, California 94305-4045

H. Eisaki and S. Uchida

  • Department of Superconductivity, The University of Tokyo, Bunkyo-ku, Tokyo 113, Japan

C. Janowitz and R. Müller

  • Institut für Physik der Humboldt-Universität Berlin, Invalidenstrasse 110, 10115 Berlin, Germany

R. L. Johnson

  • II. Institut für Experimentalphysik der Universität Hamburg, Luruper Chaussee 149, 22761 Hamburg, Germany

K. Rossnagel and L. Kipp

  • Institut für Experimentelle und Angewandte Physik, Christian-Albrechts-Universität zu Kiel, Leibnizstrasse 19, 24118 Kiel, Germany

G. Reichardt

  • BESSY GmbH, Albert-Einstein-Strasse 15, 12489 Berlin, Germany

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Vol. 63, Iss. 1 — 1 January 2001

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