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Phys. Rev. B 80, 165132 (2009) [16 pages]

Doping dependence of the chemical potential and surface electronic structure in YBa2Cu3O6+x and La2−xSrxCuO4 using hard x-ray photoemission spectroscopy

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Kalobaran Maiti1, Jörg Fink2,3, Sanne de Jong4, Mihaela Gorgoi2, Chengtian Lin5, Markus Raichle5, Vladimir Hinkov5, Michael Lambacher6, Andreas Erb6, and Mark S. Golden4
1Department of Condensed Matter Physics and Materials’ Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400 005, India
2Helmholtz-Zentrum Berlin, Albert-Einstein-Strasse 15, 12489 Berlin, Germany
3Leibniz-Institute for Solid State and Materials Research Dresden, P.O. Box 270116, D-01171 Dresden, Germany
4Van der Waals-Zeeman Institute, University of Amsterdam, NL-1018XE Amsterdam, The Netherlands
5Max-Planck-Institute for Solid State Research, D-70569 Stuttgart, Germany
6Walther-Meißner-Institut, Bayerische Akademie der Wissenschaften, Walther-Meißner Strasse 8, 85748 Garching, Germany

Received 10 June 2009; published 30 October 2009

The electronic structure of YBa2Cu3O6+x and La2−xSrxCuO4 for various values of x has been investigated using hard x-ray photoemission spectroscopy. The experimental results establish that the cleaving of YBa2Cu3O6+x compounds occurs predominantly in the BaCuO3 complex, leading to charged surfaces at higher x and to uncharged surfaces at lower x values. The bulk component of the core-level spectra exhibits a shift in binding energy as a function of x, from which a shift of the chemical potential as a function of hole concentration in the CuO2 layers could be derived. The doping dependence of the chemical potential across the transition from a Mott-Hubbard insulator to a Fermi-liquid-like metal is very different in these two series of compounds. In agreement with previous studies in the literature the chemical-potential shift in La2−xSrxCuO4 is close to zero for small hole concentrations. In YBa2Cu3O6+x, similar to all other doped cuprates studied so far, a strong shift of the chemical potential at low hole doping is detected. However, the results for the inverse charge susceptibility at small x shows a large variation between different doped cuprates. The results are discussed in view of various theoretical models. None of these models turns out to be satisfactory.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.80.165132
DOI:
10.1103/PhysRevB.80.165132
PACS:
71.10.Hf, 71.30.+h, 73.20.−r, 74.25.Jb