Electronic structure of high-entropy ROBiS2 (R=La, Ce, Pr, Nd, Sm, Gd) superconductors studied by soft x-ray absorption and photoemission spectroscopy
F. Minati, G. Tomassucci, F. Bondino, I. Pis, I. Napal Azcona, Y. Fujita, M. Nagao, L. Tortora, G. Campi, L. Boeri, T. Mizokawa, N. L. Saini
DOI 10.1103/wmvk-jnnp · Physical Review B
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Abstract
High-entropy alloy (HEA) superconductors are known to exhibit a robust superconducting state with adaptable thermomechanical properties. In this study, we have investigated the electronic structure of HEA-type ROBiS2 (R = rare earth) layered superconductors with mixing entropy using soft x-ray absorption (XAS) and x-ray photoemission spectroscopy (XPS) measurements. The electronic structure evolution differs between equivalent and nonequivalent R mixing as a function of mixing entropy. Ce M4,5-edge XAS and Ce 3d XPS reveal clear evidence of Ce3+/Ce4+ mixed valence in the HEA-type ROBiS2, similar to the pristine CeOBiS2 compound, suggesting a similar charge transfer mechanism responsible for self-doping in these materials. Unlike Ce, all other R atoms exhibit a nominal R3+ valence state across samples with varying mixing entropy. The self-doped charge is consistent with the Luttinger volume estimated by previous angle-resolved photoemission spectroscopy (ARPES) studies. The distinct behaviors observed in equivalent and nonequivalent mixing are discussed in terms of differing potential energy landscapes of the Bi sites manifested in the Bi 4f XPS spectra, where intrinsic disorder is expected to have different characteristics of the superconductivity.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Ta34Nb33Hf8Zr14Ti11 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| RBa2Cu3O7±δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 92 | Pressure not reported | onset |
| CeOBiS2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Ce0.33Pr0.33Nd0.33OBiS2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| La0.25Ce0.25Nd0.25Sm0.25OBiS2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| La0.20Ce0.20Pr0.20Nd0.20Sm0.20OBiS2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| La0.10Ce0.30Pr0.30Nd0.10Sm0.20OBiS2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| La0.20Ce0.30Pr0.20Nd0.10Sm0.10Gd0.10OBiS2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
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