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Nature 450, 81-84 (1 November 2007) | doi:10.1038/nature06219; Received 28 May 2007; Accepted 4 September 2007
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Abrupt onset of a second energy gap at the superconducting transition of underdoped Bi2212
W. S. Lee1, I. M. Vishik1, K. Tanaka1,2, D. H. Lu1, T. Sasagawa1, N. Nagaosa3, T. P. Devereaux4, Z. Hussain2 & Z.-X. Shen1
- Department of Physics, Applied Physics, and Stanford Synchrotron Radiation Laboratory, Stanford University, Stanford, California 94305, USA
- Advanced Light Source, Lawrence Berkeley National Lab, Berkeley, California 94720, USA
- Department of Applied Physics, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan
- Department of Physics, University of Waterloo, Ontario N2L 3G1, Canada
Correspondence to: W. S. Lee1Z.-X. Shen1 Correspondence and requests for materials should be addressed to Z.X.S. (Email: zxshen@stanford.edu) or W.S.L. (Email: leews@stanford.edu).
Abstract
The superconducting gap—an energy scale tied to the superconducting phenomena—opens on the Fermi surface at the superconducting transition temperature (Tc) in conventional BCS superconductors. In underdoped high-Tc superconducting copper oxides, a pseudogap (whose relation to the superconducting gap remains a mystery) develops well above Tc (refs 1, 2). Whether the pseudogap is a distinct phenomenon or the incoherent continuation of the superconducting gap above Tc is one of the central questions in high-Tc research3, 4, 5, 6, 7, 8. Although some experimental evidence suggests that the two gaps are distinct9, 10, 11, 12, 13, 14, 15, 16, 17, 18, this issue is still under intense debate. A crucial piece of evidence to firmly establish this two-gap picture is still missing: a direct and unambiguous observation of a single-particle gap tied to the superconducting transition as function of temperature. Here we report the discovery of such an energy gap in underdoped Bi2Sr2CaCu2O8+
in the momentum space region overlooked in previous measurements. Near the diagonal of Cu–O bond direction (nodal direction), we found a gap that opens at Tc and has a canonical (BCS-like) temperature dependence accompanied by the appearance of the so-called Bogoliubov quasi-particles, a classical signature of superconductivity. This is in sharp contrast to the pseudogap near the Cu–O bond direction (antinodal region) measured in earlier experiments19, 20, 21.
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