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Publications and source records attributed to Klimczuk, T..
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We present the synthesis and experimental characterization of the binary intermetallic compound Pr 7 Ru 3 . The polycrystalline sample was prepared by arc melting pure Pr and Ru, followed by homogenization at 500 °C and 600 °C for 48 and 89 h, respectively. Powder x-ray diffraction confirms that Pr 7 Ru 3 crystallizes in an orthorhombic crystal structure (Pnma, space group no. 62) with the lattice parameters: a = 7.3606(7) Å, b = 23.120(1) Å and c = 6.5959(5) Å. Magnetization, resistivity, and heat capacity measurements reveal a ferromagnetic transition in Pr 7 Ru 3 with the Curie temperature T C ~ 24.5 K. The bulk transition is confirmed by a large λ-shape anomaly observed in the specific heat measurement. The magnetic susceptibility above the transition obeys the modified Curie-Weiss law with a positive Curie-Weiss temperature $\ominus$ CW = 30(1) K and an effective magnetic moment of 3.39(1) μ B /Pr. Resistivity data for Pr 7 Ru 3 reveals metallic-like behavior with a clear anomaly at the transition temperature which is smeared by an applied magnetic field. We also synthesized high-quality nonmagnetic analog La 7 Ru 3 for which superconducting transition is observed with T c = 1.95 K, in agreement with the literature.
For this study, the B20-type cobalt germanide CoGe was investigated by measuring the specific heat, resistivity, and 59 Co nuclear magnetic resonance (NMR). We observed a phase transition at T Q = 13.7 K, evidenced by a very narrow peak of the specific heat and sharp changes of the nuclear spin-spin (T 2 –1 ) and spin-lattice ( T 1 – 1 ) relaxation rates. The fact that the entropy release is extremely small and the Knight shift is almost independent of temperature down to low temperatures as anticipated in a paramagnetic metal indicates that the T Q transition is of nonmagnetic origin. In addition, we detected a crossover scale T 0 ~ 30 K below which the resistivity and the NMR linewidth increase, and T 1 –1 is progressively distributed in space, that is, a static and dynamical spatial inhomogeneity develops. While the order parameter for the T Q transition remains an open question, a group-theoretical analysis suggests that the finite electric quadrupole density arising from the low local site symmetry at cobalt sites could drive the crystal symmetry lowering from the P2 1 3 symmetry that is commensurate to the R3 symmetry with an incommensurate wave vector, which fairly well accounts for the T Q transition. The quadrupole-order-driven commensurate-incommensurate phase transition may be another remarkable phenomenon arising from the structural chirality inherent in the noncentrosymmetric B20 family.
Effects of pressure on the electronic structure, electron-phonon interaction and superconductivity of the high entropy alloy (TaNb) 0.67 (HfZrTi) 0.33 , is studied in the range from 0 to 100 GPa. Electronic structure is calculated using the Korringa-Kohn-Rostoker method and the coherent potential approximation. Effects of pressure on the lattice dynamics were simulated using the Debye- Gru ¨neisen model, and the Gruneisen parameter at ambient conditions, Debye temperature and Sommerfeld electronic heat capacity coefficient were additionally experimentally determined. The electron-phonon coupling parameter λ is calculated using the McMillan-Hopfield parameters, computed in the rigid muffin tin approximation. We find, that the system undergoes the Lifshitz transition, as one of the bands cross the Fermi level at elevated pressures. The electron-phonon coupling parameter ? decreases above 10 GPa, however, calculated superconducting Tc increases up to 40 - 50 GPa and later is stabilized at the larger value than for the ambient conditions, in agreement with the experimental findings. Our results show, that the evolution of Tc with pressure in (TaNb) 0.67 (HfZrTi) 0.33 can be very well explained by the classical electron-phonon mechanism.
Polycrystalline Zr 5 Al 4 was synthesized using the arc-melting method. Powder X-ray diffraction confirms the previously reported crystal structure of the Ti 5 Ga 4 -type ( P 6 3 / mcm ) with lattice parameters: a = 8.4312(6) Å, and c = 5.7752(8) Å. Electrical resistivity and low-temperature magnetic susceptibility measurements indicate that Zr 5 Al 4 exhibits superconducting behavior below 2K. The normalized heat capacity jump at T c = 1.82 K, Δ C/γT c = 1.50, confirms the bulk superconductivity. The Sommerfeld coefficient γ = 28.5 mJ mol -1 K -2 and the Debye temperature Θ D = 320 K were obtained by fitting the low-temperature heat capacity data. The electron-phonon coupling strength λ el-ph = 0.49 and estimated upper critical field μ 0 H c2 (0) = 1.09 T (dirty limit) suggest that Zr 5 Al 4 is a weakly coupled type-II superconductor. Finally, first-principles calculations show the presence of a van Hove singularity near the Fermi energy.
Here, we show that the superhard boride WB 4.2 is a superconductor with a T c of 2.05(5) K. Temperature-dependent magnetic susceptibility, electrical resistivity, and specific heat measurements were used to characterize the superconducting transition. The Sommerfeld constant gamma for WB 4.2 is 2.07(3) mJ mol( -1 ) K -2 and the Δ C/γ T c = 1.56, which is somewhat higher than what is expected for weakly coupled Bardeen-Cooper-Schrieffer type superconductors. The H c2 versus T plot is linear over a wide temperature range but does show signs of flattening by the lowest temperatures studied and therefore the zero temperature upper critical field ( μ 0 H c2 (0)) for WB 4.2 lies somewhere between the linear extrapolation of μ 0 H c2 (T) to 0 K and expectations based on the Werthamer-Helfand-Hohenberg model.
La 3 Co and La 3 Ni are reported superconductors with transition temperatures of 4.5 and 6 K, respectively. In this work, we reinvestigate the physical properties of these two intermetallic compounds with magnetic susceptibility χ, specific heat C p and electrical resistivity ρ measurements down to 1.9 K. Although bulk superconductivity is confirmed in La 3 Co, as observed previously, only a trace of it is found in La3Ni, indicating that the superconductivity in La 3 Ni originates from an impurity phase. Superconducting state parameters for La 3 Co, including lower and upper critical fields and the superconducting gap, are estimated. Results of the theoretical calculations of the electronic structure for both materials are also presented, and comparison of the Fermi level location in La 3 Co versus La 3 Ni explains its larger superconducting T c . A major discrepancy between band structure calculations and the experimentally measured Sommerfeld coefficient is found. The measured electronic density of states is about 2.5 times larger than the theoretical value for La 3 Co. This effect cannot be explained by the electron-phonon interaction alone. Renormalization of γ, as well as an ~T 2 behavior of the resistivity, suggests the presence of spin fluctuations in both systems.
We observed superconductivity with critical temperature T c = 2.0 K in self-flux-grown single crystals of CaBi 2 . This material adopts the ZrSi 2 structure type with lattice parameters a = 4.696(1) Å, b = 17.081(2) Å and c = 4.611(1) Å. The crystals of CaBi 2 were studied by means of magnetic susceptibility, specific heat and electrical resistivity measurements. The heat capacity jump at T c is ΔC/γT c = 1.41, confirming bulk superconductivity; the Sommerfeld coefficient γ = 4.1 mJ mol -1 K -2 and the Debye temperature Θ D = 157 K. The electron–phonon coupling strength is λ el–ph = 0.59, and the thermodynamic critical field H c is low, between 111 and 124 Oe CaBi 2 is a moderate coupling type-I superconductor. Our results of electronic structure calculations are reported and charge densities, electronic bands, densities of states and Fermi surfaces are discussed, focusing on the effects of spin–orbit coupling and electronic property anisotropy. Furthermore, we find a mixed quasi-2D + 3D character in the electronic structure, which reflects the layered crystal structure of the material.
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