Superconductivity and phase separation in electrochemically hydrogenized K1−δCr3As3Hx
Jin-Jin Xiang, Ye-Ting Shao, Yan-Wei Cui, Lin-Peng Nie, Si-Qi Wu, Bai-Zhuo Li, Zhi Ren, Tao Wu, Guang-Han Cao
DOI 10.1103/PhysRevMaterials.4.124802 · Physical Review Materials
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Abstract
We report preparation, crystal structure, and physical properties of a quasi-one-dimensional Cr-based arsenide hydride K1−δCr3As3Hx. Through an electrolysis using essentially nonsuperconducting samples as the cathode, additional hydrogen atoms can be successfully intercalated up to x=0.45 and, consequently, the in-plane and interplane Cr–Cr bond distances in the chains of face-sharing Cr octahedra increase by 3.7% and 1.5%, respectively. The electrochemically hydrogenized samples show a broad superconducting transition at Tc=5.8 K, a record in the K-Cr-As-H system, with nearly full magnetic shielding at 1.8 K. The electronic specific-heat coefficient extracted from the specific-heat measurement is as high as γn=47 mJ K−2 mol Cr−1, suggesting a stronger electron correlation that is likely to be associated with the expansions of Cr–Cr bonds. Meanwhile, the dimensionless specific-heat jump ΔC/(γnTc) is only 0.30, about 20% of the expected value in the BCS weak-coupling scenario. Furthermore, the normal-state magnetism is characterized by Curie-Weiss paramagnetism with an enhanced effective localized moment of 1.33 μB/Cr, suggesting that a nonsuperconducting phase with localized spins dominates. The H1 nuclear magnetic resonance measurement reveals two different spin-lattice relaxations, corresponding to superconducting and localized-spin phases, respectively. All the results point to phase separation with minority superconducting phase and majority nonsuperconducting phase in the quasi-one-dimensional K1−δCr3As3Hx system.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| K1-δCr3As3Hx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 5.8 | Pressure not reported | onset |
| K1-δCr3As3Hx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 5.8 | Pressure not reported | onset |
| K1-δCr3As3Hx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 5.8 | Pressure not reported | onset |
| K2Cr3As3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 6.1 | Pressure unresolved | unknown |
| CrAs Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 2 | Pressure not reported | unknown |
| Rb2Cr3As3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 4.8 | Pressure not reported | unknown |
| Cs2Cr3As3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 2.2 | Pressure not reported | unknown |
| Na2Cr3As3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 8.6 | Pressure not reported | unknown |
| KCr3As3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 4.7 | Pressure not reported | onset |
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