corner
corner

Phys. Rev. B 72, 014504 (2005) [8 pages]

Evolution of the density of states at the Fermi level of Bi2−yPbySr2−xLaxCuO6+δ and Bi2Sr2−xLaxCuO6+δ cuprates with hole doping

Download: PDF (226 kB) Buy this article Export: BibTeX or EndNote (RIS)

M. Schneider1, R.-S. Unger1, R. Mitdank1, R. Müller2, A. Krapf1, S. Rogaschewski1, H. Dwelk1, C. Janowitz1, and R. Manzke1
1Humboldt Universität, Institut für Physik, Newtonstrasse 15, 12489 Berlin, Germany
2Physikalisch-Technische Bundesanstalt, Abbestrasse 2-12, 10587 Berlin, Germany

Received 16 March 2005; published 5 July 2005

Bi2Sr2−xLaxCuO6+δ and Bi2−yPbySr2−xLaxCuO6+δ high-Tc superconductors in a wide doping range from overdoped to heavily underdoped were studied by x-ray absorption and photoemission spectroscopy. The hole concentration p was determined by an analysis of the Cu L3-absorption edge. Besides the occupied density of states derived from photoemission, the unoccupied density of states was determined from the prepeak of the O K-absorption edge. Both, the occupied as well as the unoccupied density of states reveal the same dependence on hole doping, i.e., a continuous increase with increasing doping in the hole underdoped region and a constant density in the hole overdoped region. By comparing these results of single-layer BSLCO with previous results on single-layer LSCO it could be argued that besides the localized holes on Cu sites the CuO2-planes consist of two types of doped holes, from which the so-called mobile holes determine the intensity of the prepeak of the O 1s absorption edge.

© 2005 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.72.014504
DOI:
10.1103/PhysRevB.72.014504
PACS:
74.72.−h, 78.40.−q, 79.60.−i, 74.25.−q