期刊
PHYSICAL REVIEW B
卷 105, 期 21, 页码 -出版社
AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.105.214502
关键词
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资金
- Scientific Discovery through Advanced Computing (Sci-DAC) program - U.S. Department of Energy, Office of Science, Advanced Scientific Computing Research and Basic Energy Sciences, Division of Materials Sciences and Engineering
- U.S. Department of Energy, Office of Science, Office of Workforce Development for Teachers and Scientists, Office of Science Graduate Student Research (SCGSR) program
- DOE [DE-SC0014664]
- U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences [DE-SC-0020385]
- U.S. Department of Energy (DOE), Office of Science, Basic Energy Sciences (BES), Materials Sciences and Engineering Division
- DOE Office of Science User Facility [DE-AC05-00OR22725]
- U.S. Department of Energy [DE-AC0500OR22725]
This study investigates the effect of coupling a metal on the superconducting transition temperature of an unconventional superconductor. The results show a nonmonotonic dependence of the transition temperature on the strength of hybridization and interlayer hopping.
It has been proposed that the superconducting transition temperature T-c of an unconventional superconductor with a large pairing scale but strong phase fluctuations can be enhanced by coupling it to a metal. However, the general efficacy of this approach across different parameter regimes remains an open question. Using the dynamical cluster approximation, we study this question in a system composed of an attractive Hubbard layer in the intermediate coupling regime, where the magnitude of the attractive Coulomb interaction vertical bar U vertical bar is slightly larger than the bandwidth W, hybridized with a noninteracting metallic layer. We find that while the superconducting transition becomes more mean-field-like with increasing interlayer hopping, the superconducting transition temperature T-c exhibits a nonmonotonic dependence on the strength of the hybridization t(perpendicular to). This behavior arises from a reduction of the effective pairing interaction in the correlated layer that outcompetes the growth in the intrinsic pair-field susceptibility induced by the coupling to the metallic layer. We find that the largest T-c inferred here for the composite system is comparable to the maximum value currently estimated for the isolated negative-U Hubbard model.
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