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Normal state and superconducting state properties of high entropy Ta0.2Nb0.2V0.2Ti0.2X0.2 (X=Zr and Hf)

Nikita Sharma, J. Link, Kuldeep Kargeti, Neha Sharma, I. Heinmaa, S. K. Panda, R. Stern, Tirthankar Chakraborty, Tanmoy Chakrabarty, Sourav Marik

DOI 10.1103/PhysRevMaterials.9.064801 · Physical Review Materials

T1

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Abstract

High-entropy alloy superconductors represent a unique blend of advanced material systems and quantum physics, offering significant potential for advancing superconducting technologies. In this study, we report a detailed theoretical and experimental investigation of high-entropy alloy superconductors Ta0.2Nb0.2V0.2Ti0.2X0.2 (X=Zr and Hf). Our study unveils that both the materials crystallize in a body-centered-cubic structure (space group: Im-3m) and exhibit bulk superconductivity with a superconducting onset temperature of (Tconset) of 5 K for X= Hf and 6.19 K for X=Zr sample. Our detailed analysis, including magnetization, resistivity, heat capacity measurements, and density functional X=Zr theory (DFT) calculations indicates moderately coupled isotropic s-wave superconductivity in these materials. Our DFT results find significant spectral weight at the Fermi energy and phonon spectra is free of imaginary modes, confirming the dynamical stability and metallic nature of these alloys. Remarkably, we have observed a high upper critical field [Hc2(0)] surpassing the Pauli paramagnetic limit for the X= Hf sample and explained it on the basis of the increased spin-orbit coupling in the structure. Ta0.2Nb0.2V0.2Ti0.2Zr0.2, on the other hand, shows a conventional Hc2 behavior. With the dynamical stability of these alloys, excellent normal state metallic nature, high microhardness, and high upper critical field, these samples emerge as potential candidates for future applications in superconducting devices.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
Ta0.2Nb0.2V0.2Ti0.2Zr0.2

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6.19Pressure not reportedonset
Ta0.2Nb0.2V0.2Ti0.2Zr0.2

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

6Pressure not reportedonset
Ta0.2Nb0.2V0.2Ti0.2Hf0.2

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

5Pressure not reportedonset
Ta0.2Nb0.2V0.2Ti0.2Hf0.2

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

4.9Pressure not reportedonset

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