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Vitaly A. Gasparov

Publications and source records attributed to Vitaly A. Gasparov.

2 recordsLinked to original sources

Upper critical magnetic field in K0.83Fe1.83Se2 and Eu0.5K0.5Fe2As2 single crystals

The H-T phase diagrams of single crystalline electron-doped K0.83Fe1.83Se2 (KFS1), K0.8Fe2Se2 (KFS2) and hole-doped Eu0.5K0.5Fe2As2 (EKFA) have been deduced from tunnel diode oscillator-based contactless measurements in pulsed magnetic fields up to 57 T for the inter-plane (H//c) and in-plane (H//ab) directions. The temperature dependence of the upper critical magnetic field Hc2(T) relevant to EFKA is accounted for by the Pauli model including an anisotropic Pauli paramagnetic contribution (μ_BHp=114 T for H//ab and 86 T for H//c). This is also the case of KFS1 and KFS2 for H//ab whereas a significant upward curvature, accounted for by a two-gap model, is observed for H//c. Despite the presence of antiferromagnetic lattice order within the superconducting state of the studied compounds, no influence of magnetic ordering on the temperature dependence of Hc2(T) is observed.

cond-mat.supr-con↗

Electron Transport in Diborides: Observation of Superconductivity in ZrB2

We report on syntheses and electron transport properties of polycrystalline samples of diborides (AB2) with different transition metals atoms (A=Zr,Nb,Ta). The temperature dependence of resistivity, ρ(T), and ac susceptibility of these samples reveal superconducting transition of ZrB2 with Tc=5.5 K, while NbB2 and TaB2 have been observed nonsuperconducting up to 0.37 K. Hc2(T) is linear in temperature below Tc, leading to a rather low Hc2(0)= 0.1 T. At T close to Tc, Hc2(T) demonstrates a downward curvature. We conclude that these diborides as well as MgB2 samples behaves like a simple metals in the normal state with usual Bloch-Grüneisen temperature dependence of resistivity and with Debye temperatures: 280 K, 460 K and 440 K, for ZrB2, NbB2 and MgB2, respectively, rather than T^2 and T^3 as previously reported for MgB2.

cond-mat.mtrl-sci↗