Quantum Paraelectric Model for Layered Superconductors
S. R. Shenoy, V. Subrahmanyam, A. R. Bishop
DOI 10.1103/PhysRevLett.79.4657 · Physical Review Letters
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Abstract
We consider a Hubbard-model (H) layer of charged-carrier fraction x≪1, and an rms buckling angle s≪1, that is elastically and electrically coupled to anharmonic (oxygen) dipoles in a ferroelectric Bilz-model (B) layer. We find that (a) the B-layer dipoles are driven to a paraelectric phase by H-layer zero-point fluctuations; (b) the c-axis (dipolar, optical) and H-layer (acoustic) modes are mixed by s to form ω±(q) modes; and (c) the mode exchange, enhanced by a (ω+2−ω−2)−1∼s−1 resonant denominator, produces dynamical local carrier pairing and 2D Anderson-Morel dx2−y2–type superconductivity, with peaks or plateaus in Tc(x).
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| SrTiO3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 0.1 | Pressure not reported | unknown |
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