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Zero Cu valence and superconductivity in high-quality CuxBi2Se3 crystal

Shih-Hsun Yu, Tsu Lien Hung, Min-Nan Ou, Mitch M. C. Chou, Yang-Yuan Chen

DOI 10.1103/PhysRevB.100.174502 · Physical Review B

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Abstract

In this work, the role of Cu dopants in the development of superconductivity in Bi2Se3 is investigated. A series of CuxBi2Se3 (x=0–0.3) crystals is grown using the Bridgman method and electrochemical techniques. Based on the observable lattice increases along the c axis, the existence of Cu atoms intercalated in the van der Waals (vdW) gaps in Bi2Se3 is verified by x-ray diffraction, scanning electron microsopy–energy dispersive spectroscopy, and transmission electron microscopy analysis. Furthermore, the chemical state of the Cu is found to be zero valence by characterization of the x-ray photoelectron and Auger electron spectra. The absence of Cu1+ and Cu2+ in the electron energy-loss spectroscopy near-edge fine structure is confirmed as well. Meanwhile, our Raman data also show the same result: the intercalation of Cu in the vdW gap which weakens the binding of the quintuple layers in the Cu0.1Bi2Se3 crystal. The electric resistance and magnetic susceptibility show a superconducting transition near 3–3.4 K in the series of Cu-doped Bi2Se3. A sharp superconducting transition with the highest value of TC=3.4K and the largest magnetic shielding fraction of 84% is observed in the optimized 10% Cu-doped Bi2Se3. These results imply that the formation of superconducting quasiparticles is not related to the charge transfer of Cu, but is supported by the internal stress of Cu intercalated in the van der Waals gap. The superconducting transition observed in the specific heat implies that the superconductivity in CuxBi2Se3 is unconventional.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
CuxBi2Se3

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3.4Pressure unresolvedonset
CuxBi2Se3

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

3.4Pressure unresolvedonset
CuxBi2Se3

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

3.4Pressure unresolvedonset
Cu0.1Bi2Se3

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3.4Pressure unresolvedonset
Cu0.1Bi2Se3

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

3.4Pressure unresolvedonset

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