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Bose–Einstein condensation of strongly correlated electrons and phonons in cuprate superconductors

A S Alexandrov

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The long-range Fröhlich electron–phonon interaction has been identified as the most essential for pairing in high-temperature superconductors owing to poor screening, as is now confirmed by optical, isotope substitution, recent photoemission and some other measurements. I argue that low-energy physics in cuprate superconductors is that of superlight small bipolarons, which are real-space hole pairs dressed by phonons in doped charge-transfer Mott insulators. They are itinerant quasiparticles existing in the Bloch states at low temperatures as also confirmed by the continuous-time quantum Monte–Carlo algorithm (CTQMC) fully taking into account realistic Coulomb and long-range Fröhlich interactions. Here I suggest that a parameter-free evaluation of Tc, unusual upper critical fields, the normal state Nernst effect, diamagnetism, the Hall–Lorenz numbers and giant proximity effects strongly support the three-dimensional (3D) Bose–Einstein condensation (BEC) of mobile small bipolarons with zero off-diagonal order parameter above the resistive critical temperature Tc at variance with phase fluctuation scenarios of cuprates.


PACS

71.27.+a Strongly correlated electron systems; heavy fermions

74.72.-h Cuprate superconductors (high-Tc and insulating parent compounds)

74.45.+c Proximity effects; Andreev effect; SN and SNS junctions

74.25.Kc Phonons

71.38.-k Polarons and electron-phonon interactions

74.40.+k Fluctuations (noise, chaos, nonequilibrium superconductivity, localization, etc.)

Subjects

Superconductivity

Condensed matter: electrical, magnetic and optical

Dates

Issue 12 (28 March 2007)

Received 13 July 2006, in final form 3 August 2006

Published 6 March 2007



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