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Quaternary borocarbides: A testbed for DFT for superconductors

Viktor Christiansson, Philipp Werner

DOI 10.1103/PhysRevB.109.L180505 · Physical Review B

T1

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Abstract

Using ab initio density functional theory for superconductors (SCDFT), we systematically study the quaternary borocarbides RM2B2C. Treating the retarded (frequency-dependent) interaction W(ω) within the random-phase approximation, we find good agreement with experiments for the calculated superconducting critical temperature Tc in the nonmagnetic Ni- and Pd-based compounds. Replacing the density functional theory (DFT) bands with a one-shot GW-derived quasiparticle band structure in the SCDFT calculations further improves the agreement with experiment for several of the tested systems. We argue that the problem of accurately placing the f bands within DFT, and possibly the lack of an explicit magnetic pair-breaking mechanism, explains the difficulties of SCDFT in reproducing Tc in members of the magnetic RNi2B2C series (R rare-earth elements with partially filled 4f states). While the calculated Tc is overestimated, SCDFT qualitatively captures the experimentally observed trend along the rare-earth series, which indicates that the electron-phonon couplings and dynamically screened interactions have a significant effect on Tc.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
LaNi2B2C

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0.4Pressure not reportedunknown
TmNi2B2C

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—Pressure not reportedunknown
ThNi2B2C

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—Pressure not reportedunknown
ErNi2B2C

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

—Pressure not reportedunknown
YNi2B2C

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

—Pressure not reportedunknown
HoNi2B2C

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

—Pressure not reportedunknown
LuNi2B2C

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

—Pressure not reportedunknown
DyNi2B2C

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

—Pressure not reportedunknown
ScNi2B2C

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

—Pressure not reportedunknown
TbNi2B2C

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

—Pressure not reportedunknown
YbNi2B2C

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

—Pressure not reportedunknown
GdNi2B2C

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

—Pressure not reportedunknown
LuPd2B2C

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

—Pressure not reportedunknown
YPt2B2C

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

—Pressure not reportedunknown
YPd2B2C

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

23Pressure not reportedunknown
ThPt2B2C

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

—Pressure not reportedunknown
ThPd2B2C

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

—Pressure not reportedunknown
PrPt2B2C

Archive — visibility unverified

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

—Pressure not reportedunknown
LaPd2B2C

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

—Pressure not reportedunknown
LaPt2B2C

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

—Pressure not reportedunknown

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