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  • From a Single-Band Metal to...
    He, Rui-Hua; Hashimoto, M.; Karapetyan, H.; Koralek, J. D.; Hinton, J. P.; Testaud, J. P.; Nathan, V.; Yoshida, Y.; Yao, Hong; Tanaka, K.; Meevasana, W.; Moore, R. G.; Lu, D. H.; Mo, S.-K.; Ishikado, M.; Eisaki, H.; Hussain, Z.; Devereaux, T. P.; Kivelson, S. A.; Orenstein, J.; Kapitulnik, A.; Shen, Z.-X.

    Science (American Association for the Advancement of Science), 03/2011, Volume: 331, Issue: 6024
    Journal Article

    The nature of the pseudogap phase of cuprate high-temperature superconductors is a major unsolved problem in condensed matter physics. We studied the commencement of the pseudogap state at temperature T* using three different techniques (angle-resolved photoemission spectroscopy, polar Kerr effect, and time-resolved reflectivity) on the same optimally doped Bi2201 crystals. We observed the coincident, abrupt onset at T* of a particle-hole asymmetric antinodal gap in the electronic spectrum, a Kerr rotation in the reflected light polarization, and a change in the ultrafast relaxational dynamics, consistent with a phase transition. Upon further cooling, spectroscopic signatures of superconductivity begin to grow close to the superconducting transition temperature (T c ), entangled in an energy-momentum—dependent manner with the preexisting pseudogap features, ushering in a ground state with coexisting orders.