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Crystal symmetry, electron-phonon coupling, and superconducting tendencies in Li2Pd3B and Li2Pt3B

K.-W. Lee, W. E. Pickett

DOI 10.1103/PhysRevB.72.174505 · Physical Review B

T1

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Abstract

After theoretical determination of the internal structural coordinates in Li2Pd3B, we calculate and analyze its electronic structure and obtain the frequencies of the two Ag phonons (40.6 meV for nearly pure Li mode, 13.0 meV for the strongly mixed Pd-Li mode). Pd can be ascribed a 4d10 configuration, but strong 4d character remains up to the Fermi level. Small regions of flat bands occur at −70meV at both the Γ and X points. Comparison of the Fermi level density of states to the linear specific heat coefficient gives a dynamic mass enhancement of λ=0.75. Rough Fermi surface averages of the deformation potentials D of individual Pd and Li displacements are obtained. While ⟨DLi⟩ is small, ⟨DPd⟩≈1.15eV∕Å is sizable, and a plausible case exists for its superconductivity at 8 K being driven primarily by coupling to Pd vibrations. The larger d bandwidth in Li2Pt3B leads to important differences in the bands near the Fermi surface. The effect on the band structure of spin-orbit coupling plus lack of inversion is striking, and is much larger in the Pt compound.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
Li2Pd3B

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8Pressure not reportedunknown
Li2Pt3B

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2.8Pressure not reportedunknown
CePt3Si

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0.75Pressure not reportedunknown
UIr

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0.142.6 GPaunknown
MgCNi3

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8Pressure not reportedunknown

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