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Quantum critical origin of the superconducting dome in SrTiO$_3$

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arxiv 1507.08275 v1 pith:UFMCE6VQ submitted 2015-07-29 cond-mat.supr-con

classification cond-mat.supr-con
keywords dopingquantumcriticaldomeferroelectricsuperconductingdensityexperimentally
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abstract

We investigate the origin of superconductivity in doped SrTiO$_3$ (STO) using a combination of density functional and strong coupling theories within the framework of quantum criticality. Our density functional calculations of the ferroelectric soft mode frequency as a function of doping reveal a crossover from quantum paraelectric to ferroelectric behavior at a doping level coincident with the experimentally observed top of the superconducting dome. Based on this finding, we explore a model in which the superconductivity in STO is enabled by its proximity to the ferroelectric quantum critical point and the soft mode fluctuations provide the pairing interaction on introduction of carriers. Within our model, the low doping limit of the superconducting dome is explained by the emergence of the Fermi surface, and the high doping limit by departure from the quantum critical regime. We predict that the highest critical temperature will increase and shift to lower carrier doping with increasing $^{18}$O isotope substitution, a scenario that is experimentally verifiable.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Two-phonon pairing and superconductivity in $SrTiO_3$

    cond-mat.supr-con 2026-08 conditional novelty 6.0 of 10

    The two-phonon pairing mechanism in SrTiO3 gives a small, monotonically doping-dependent Tc because the attraction is controlled by high-energy phonons, not the soft mode.

  2. Understanding the origin of superconducting dome in electron-doped MoS$_2$ monolayer

    cond-mat.supr-con 2024-12 conditional novelty 6.0 of 10

    The superconducting dome in electron-doped MoS2 is recreated from first principles and traced to the 1x1 H to 2x2 charge-density-wave transition and later structural phases.

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