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Phys. Rev. B 70, 094522 (2004) [6 pages]

Change of quasiparticle dispersion in crossing Tc in the underdoped cuprates

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T. Eckl1,*, W. Hanke1, S. V. Borisenko2,†, A. A. Kordyuk2,3, T. Kim2, A. Koitzsch2, M. Knupfer2, and J. Fink2
1Institut für Theoretische Physik und Astrophysik, Universität Würzburg, Am Hubland, D-97074 Würzburg, Germany
2Institute for Solid State Research, IFW-Dresden, P. O. Box 27 00 16, D-01171 Dresden, Germany
3Institute of Metal Physics of National Academy of Sciences of Ukraine, 03142 Kyiv, Ukraine

Received 12 February 2004; revised 7 June 2004; published 29 September 2004

One of the most remarkable properties of the high-temperature superconductors is a pseudogap regime appearing in the underdoped cuprates above the superconducting transition temperature Tc. The pseudogap continously develops out of the superconducting gap. In this paper, we demonstrate by means of a detailed comparison between theory and experiment that the characteristic change of quasiparticle dispersion in crossing Tc in the underdoped cuprates can be understood as being due to phase fluctuations of the superconducting order parameter. In particular, we show that within a phase fluctuation model the characteristic back-turning BCS bands disappear above Tc whereas the gap remains open. Furthermore, the pseudogap rather has a U shape instead of the characteristic V shape of a dx2y2-wave pairing symmetry and starts closing from the nodal k⃗=(π∕2,π∕2) directions, whereas it rather fills in at the antinodal k⃗=(π,0) regions, yielding further support to the phase fluctuation scenario.

© 2004 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.70.094522
DOI:
10.1103/PhysRevB.70.094522
PACS:
71.10.Fd, 71.27.+a, 74.25.Jb, 74.72.−h

*Electronic address: eckl@physik.uni-wuerzburg.de

Electronic address: S.Borisenko@ifw-dresden.de