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Pseudogap phase in strongly disordered conventional superconductors

X. T. Wu, R. Ikeda

DOI 10.1103/PhysRevB.83.104517 · Physical Review B

T1

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Abstract

Excited states of Bogoliubov–de Gennes equations are examined for a two-dimensional negative-U Hubbard Hamiltonian with on-site disorder. It is shown explicitly that the temperature (pseudogap temperature) when the superconducting gap opens is different from that (the superconducting transition temperature) where the long-range order appears. In the excited-state solutions the system is self-organized into blocks, which behave like superspins and are coupled with their neighbors. Only if the couplings between these blocks become strong enough can the true long-range order be realized.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
NbN

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

—Pressure not reportedunknown
TiN

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

—Pressure not reportedunknown

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