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BaPtSi3: A noncentrosymmetric BCS-like superconductor

E. Bauer, R. T. Khan, H. Michor, E. Royanian, A. Grytsiv, N. Melnychenko-Koblyuk, P. Rogl, D. Reith, R. Podloucky, E.-W. Scheidt, W. Wolf, M. Marsman

DOI 10.1103/PhysRevB.80.064504 · Physical Review B

T1

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Abstract

By investigations of phase relations in the alloy system Ba-Pt-Si at 900 °C we observe the formation of the compound BaPtSi3, which crystallizes in the noncentrosymmetric BaNiSn3 structure type. Its space group is I4mm with the tetragonal lattice parameters a=0.44094(2)nm and c=1.0013(2)nm for the arc-melted compound annealed at 900 °C. The characterization of the physical properties of BaPtSi3 reveals a superconducting transition at 2.25 K with an upper critical field at T=0 K of ≈0.05 T. For analyzing the electronic structure, density-functional theory calculations are performed yielding very good agreement between theory and experiment for the structural properties. From relativistic electronic-structure calculations, Fermi surface nesting features are found for two characteristic double sets of bands. The spin-orbit splitting of the relativistic electronic bands is in general rather small at Fermi energy and, therefore, superconductivity adheres to an almost undisturbed BCS state.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
BaPtSi3

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2Pressure not reportedonset
BaPtSi3

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2.25Pressure not reportedmidpoint
CePt3Si

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—Pressure unresolvedunknown
UIr

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—Pressure not reportedunknown
CeRhSi3

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—Pressure not reportedunknown
CeIrSi3

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—Pressure not reportedunknown
Cd2Re2O7

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1Pressure not reportedunknown
Li2Pd3B

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

—Pressure not reportedunknown
Li2Pt3B

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

—Pressure not reportedunknown
Mg2Al3

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—Pressure not reportedunknown

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