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Spectroscopic evidence for a pseudogap in the normal state of underdoped high-Tc superconductors H. Ding*†, T. Yokoya‡, J. C. Campuzano*†, T. Takahashi‡, M. Randeria§, M. R. Norman†, T. Mochiku ¶, K. Kadowaki ¶ & J. Giapintzakis£
* Department of Physics, University of Illinois at Chicago, Chicago, Illinois 60607, USA
† Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA
‡Department of Physics, Tohoku University, Sendai 980, Japan
§Tata Institute of Fundamental Research, Bombay 400005, India
Institute of Materials Science, University of Tsukuba, Tsukuba, Ibaraki 305, Japan
¶ National Research Institute for Metals, Tsukuba, Ibaraki 305, Japan
£ Department of Physics, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA
IT is well known that BCS mean-field theory is remarkably successful in describing conventional superconductors. A central concept of BCS theory is the energy gap in the electronic excitation spectrum below the superconducting transition temperature, T
c. The gap also serves as the order parameter: quite generally, long-range phase coherence and a non-zero gap go hand-in-hand1. But in underdoped high-T
c superconductors there is considerable evidence that a pseudogap (a suppression of spectral weight) is already formed in the normal state above T
c—first, from studies of the spin excitation spectrum2–5,24, which measure a 'spin gap', and later from a variety of other probes6–10. Here we present a study of underdoped Bi2Sr2CaCu2O8+ (Bi2212) using angle-resolved photoemission spectroscopy (ARPES), which directly measures the momentum-resolved electron excitation spectrum of the CuO2 planes. We find that a pseudogap with d-wave symmetry opens up in the normal state below a temperature T
* > T
c, and develops into the d-wave superconducting gap once phase coherence is established below T
c.
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