Destruction of the Fermi surface in underdoped high-Tc superconductors

M. R. Norman, H. Ding, M. Randeria, J. C. Campuzano (), T. Yokoya, T. Takeuchi, T. Takahashi, T. Mochiku, K. Kadowaki, P. Guptasarma and D. G. Hinks
Additional contact information
M. R. Norman: Argonne National Laboratory
H. Ding: Argonne National Laboratory
M. Randeria: Tata Institute of Fundamental Research
J. C. Campuzano: Argonne National Laboratory
T. Yokoya: Tohoku University
T. Takeuchi: Nagoya University
T. Takahashi: Tohoku University
T. Mochiku: National Research Institute for Metals, Sengen
K. Kadowaki: Institute of Materials Science, University of Tsukuba
P. Guptasarma: Argonne National Laboratory
D. G. Hinks: Argonne National Laboratory

Nature, 1998, vol. 392, issue 6672, 157-160

Abstract: Abstract The Fermi surface—the set of points in momentum space describing gapless electronic excitations—is a central concept in the theory of metals. In this context, the normal ‘metallic’ state of the optimally doped high-temperature superconductors is not very unusual: above the superconducting transition temperature, Tc, there is evidence for a large Fermi surface1,2,3, despite the absence of well-defined elementary excitations. In contrast, the normal state of underdoped high-temperature superconductors differs in that there is evidence for a ‘pseudogap’ above Tc (4–7). Here we examine, using angle-resolved photoemission spectroscopy, the temperature dependence of the Fermi surface in underdoped Bi2Sr2CaCu2O8+δ. We find that, on cooling the sample, the pseudogap opens up at different temperatures for different points in momentum space. This leads to an initial breakup of the Fermi surface, at a temperature T*, into disconnected arcs, which then shrink with decreasing temperature before collapsing to the point nodes of the superconducting ground state below Tc. This unusual behaviour, where the Fermi surface does not form a continuous contour in momentum space as in conventional metals, is unprecedented in that it occurs in the absence of long-range order. Moreover, although the superconducting gap below Tc evolves smoothly into the pseudogap above Tc, the pseudogap differs in its unusual temperature-dependent anisotropy, implying an intimate but non-trivial relationship between the pseudogap and the superconducting gap.

Date: 1998
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DOI: 10.1038/32366

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