Abstract:A novel strontium−gold silicide (SrAuSi 3 ) was successfully synthesized for the first time using a high-pressure technique, at ∼6 GPa. X-ray Rietveld analysis and scanning transmission electron microscopy studies clearly revealed that SrAuSi 3 crystallizes in a BaNiSn 3 -type structure, in space group I4mm with the following lattice parameters: a = 4.4090(1) Å, and c = 9.9475(3) Å. The structure was found not to have inversion symmetry in real space. From direct measurements of polycrystalline SrAuSi 3 , the … Show more
“…The spin-orbit interaction is included as a perturbation to the scalar-relativistic equations. This theoretical work [24] reveals that the spin-orbit interaction for this superconductor has only negligible effect on the band structure around the Fermi energy. Moreover, this theoretical work [24] shows that the band structure around the Fermi energy is dominated by Si p states and the mechanism of superconductivity is suggested as phonon induced.…”
Section: Introductionmentioning
confidence: 82%
“…Recently, the lattice parameters, electronic structures, elastic constants, Vicker's hardness and thermodynamics properties of SrAuSi 3 were systematically investigated by using first-principles and the quasi-harmonic Debye model [35]. In this theoretical work [35], the superconducting transition temperature (T c ) for SrAuSi 3 is calculated to be 9.94 K which is much larger than its experimental value of 1.54 K [24].…”
Section: Introductionmentioning
confidence: 94%
“…A recent experiment shows that SrAuSi 3 [24], which also has the body-centered tetragonal BaNiSn 3 -type structure, exhibits superconductivity with a critical temperature (T c ) of 1.54 K. This material is the first reported noncentrosymmetric superconductor that contains Au as a principal constituent element [24]. The electronic properties of SrAuSi 3 have been studied by means of the full-potential linearized augmented plane wave (FLAPW) employing a generalized gradient approximation of the density functional theory [24].…”
Section: Introductionmentioning
confidence: 99%
“…The electronic properties of SrAuSi 3 have been studied by means of the full-potential linearized augmented plane wave (FLAPW) employing a generalized gradient approximation of the density functional theory [24]. The spin-orbit interaction is included as a perturbation to the scalar-relativistic equations.…”
Section: Introductionmentioning
confidence: 99%
“…With this in mind, in this work, we have investigated the structural and electronic properties of SrAuSi 3 and SrAu 2 Si 2 using the ab initio pseudo-potential method based on a generalized gradient approximation of the density functional theory [36]. The calculated lattice and internal parameters for both materials are compared with their experimental values [24,25]. Details of the electronic band structure and the electronic density of states near the Fermi energy are presented and discussed.…”
The structural and electronic properties of BaNiSn 3 -type SrAuSi 3 and ThCr 2 Si 2 -type SrAu 2 Si 2 have been investigated by using the planewave pseudopotential method and the density functional theory. The electronic structures and phonon dispersion relations of these two materials have been analyzed with and without the inclusion of spin-orbit interaction, and similarities and differences highlighted. By integrating the Eliashberg spectral function α 2 F(ω), the average electron-phonon coupling parameter is determined to be λ = 0.47 for SrAuSi 3 and 0.42 for SrAu 2 Si 2 . The largest contribution to the electron-phonon coupling for SrAuSi 3 comes from the Si p electrons near the Fermi energy and Si-related vibrations. Using a reasonable value of µ * = 0.12 for the effective Coulomb repulsion parameter, the superconducting critical temperature T c for SrAuSi 3 is found to be 1.47 K which compares very well with its experimental value of 1.54 K.
“…The spin-orbit interaction is included as a perturbation to the scalar-relativistic equations. This theoretical work [24] reveals that the spin-orbit interaction for this superconductor has only negligible effect on the band structure around the Fermi energy. Moreover, this theoretical work [24] shows that the band structure around the Fermi energy is dominated by Si p states and the mechanism of superconductivity is suggested as phonon induced.…”
Section: Introductionmentioning
confidence: 82%
“…Recently, the lattice parameters, electronic structures, elastic constants, Vicker's hardness and thermodynamics properties of SrAuSi 3 were systematically investigated by using first-principles and the quasi-harmonic Debye model [35]. In this theoretical work [35], the superconducting transition temperature (T c ) for SrAuSi 3 is calculated to be 9.94 K which is much larger than its experimental value of 1.54 K [24].…”
Section: Introductionmentioning
confidence: 94%
“…A recent experiment shows that SrAuSi 3 [24], which also has the body-centered tetragonal BaNiSn 3 -type structure, exhibits superconductivity with a critical temperature (T c ) of 1.54 K. This material is the first reported noncentrosymmetric superconductor that contains Au as a principal constituent element [24]. The electronic properties of SrAuSi 3 have been studied by means of the full-potential linearized augmented plane wave (FLAPW) employing a generalized gradient approximation of the density functional theory [24].…”
Section: Introductionmentioning
confidence: 99%
“…The electronic properties of SrAuSi 3 have been studied by means of the full-potential linearized augmented plane wave (FLAPW) employing a generalized gradient approximation of the density functional theory [24]. The spin-orbit interaction is included as a perturbation to the scalar-relativistic equations.…”
Section: Introductionmentioning
confidence: 99%
“…With this in mind, in this work, we have investigated the structural and electronic properties of SrAuSi 3 and SrAu 2 Si 2 using the ab initio pseudo-potential method based on a generalized gradient approximation of the density functional theory [36]. The calculated lattice and internal parameters for both materials are compared with their experimental values [24,25]. Details of the electronic band structure and the electronic density of states near the Fermi energy are presented and discussed.…”
The structural and electronic properties of BaNiSn 3 -type SrAuSi 3 and ThCr 2 Si 2 -type SrAu 2 Si 2 have been investigated by using the planewave pseudopotential method and the density functional theory. The electronic structures and phonon dispersion relations of these two materials have been analyzed with and without the inclusion of spin-orbit interaction, and similarities and differences highlighted. By integrating the Eliashberg spectral function α 2 F(ω), the average electron-phonon coupling parameter is determined to be λ = 0.47 for SrAuSi 3 and 0.42 for SrAu 2 Si 2 . The largest contribution to the electron-phonon coupling for SrAuSi 3 comes from the Si p electrons near the Fermi energy and Si-related vibrations. Using a reasonable value of µ * = 0.12 for the effective Coulomb repulsion parameter, the superconducting critical temperature T c for SrAuSi 3 is found to be 1.47 K which compares very well with its experimental value of 1.54 K.
Large plate crystals of LaPtGe2 have been grown by using an inert indium metal flux. This compound crystallizes in the CeNiSi2‐type structure (orthorhombic space group Cmcm) with lattice parameters a = 4.3770(9) Å, b = 17.186(3) Å, and c = 4.3942(9) Å. The structure of LaPtGe2 is a three‐dimensional framework with alternating PbO‐type layers of PtGe and infinite Ge chains, separated by La atoms. Electrical resistivity and Hall effect measurements characterize LaPtGe2 as a metal with holes that act as the charge carriers. Strong temperature dependence of the Hall coefficient and a violation of Kohler's rule (from magnetoresistance data) both indicate possible multiband effects. The electronic structure calculations suggest the metallic nature of LaPtGe2 and show that the strongest bonding exists between Pt and Ge within the PbO‐type layers.
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