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Phase fluctuations and pseudogap phenomena
Institution:1. Bogolyubov Institute for Theoretical Physics, 14-b Metrologicheskaya Str., 03143 Kiev, Ukraine;2. Department of Physics, University of Pretoria, Pretoria 0002, South Africa;1. Center of Excellence in Quantum Technology, Faculty of Engineering, Chiang Mai University, Chiang Mai, 50200, Thailand;2. Research Center for Quantum Technology, Faculty of Science, Chiang Mai University, Chiang Mai, 50200, Thailand;3. Department of Physics and Materials Science, Faculty of Science, Chiang Mai University, 50200, Thailand;4. Athens Institute for Education and Research, Mathematics and Physics Divisions, 8 Valaoritou Street, Kolonaki, 10671, Athens, Greece;1. Materials Science and Engineering Program, UC San Diego, La Jolla, CA 92093, USA;2. Department of Physics, Chemistry, and Biology (IFM) Linköping University, SE-581 83 Linköping, Sweden;3. Department of NanoEngineering, UC San Diego, La Jolla, CA 92093, USA;1. Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, PR China;2. University of Science and Technology of China, Hefei 230026, PR China
Abstract:This article reviews the current status of precursor superconducting phase fluctuations as a possible mechanism for pseudogap formation in high-temperature superconductors. In particular we compare this approach which relies on the two-dimensional nature of the superconductivity to the often used T-matrix approach. Starting from simple pairing Hamiltonians we present a broad pedagogical introduction to the BCS–Bose crossover problem. The finite temperature extension of these models naturally leads to a discussion of the Berezinskii–Kosterlitz–Thouless superconducting transition and the related phase diagram including the effects of quantum phase fluctuations and impurities. We stress the differences between simple Bose–BCS crossover theories and the current approach where one can have a large pseudogap region even at high carrier density where the Fermi surface is well-defined. Green's function and its associated spectral function, which explicitly show non-Fermi liquid behavior, is constructed in the presence of vortices. Finally different mechanisms including quasi-particle–vortex and vortex–vortex interactions for the filling of the gap above Tc are considered.
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