Interplay of superconductivity and structural phase transition in the clathrate Ba6Ge25
H. Q. Yuan, F. M. Grosche, W. Carrillo-Cabrera, V. Pacheco, G. Sparn, M. Baenitz, U. Schwarz, Yu. Grin, F. Steglich
DOI 10.1103/PhysRevB.70.174512 · Physical Review B
Active bibliographic source — not scientific approval
Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.
Abstract
The cubic compound Ba6Ge25 undergoes a structural phase transition around 200 K, below which the electrical resistivity increases abruptly. However, out of this “bad” metallic state (ρ0≃1.5mΩcm), BCS-like superconductivity occurs at very low temperature (Tc≈0.24K). By applying hydrostatic pressure, the structural phase transition is suppressed at pc≃2.8GPa, but the superconducting transition temperature Tc increases remarkably, reaching a maximum of Tc≃3.8K at p∼pc. To understand these unusual properties, we have measured the upper critical magnetic field Hc2 for Ba6Ge25 and its isostructural compound Na2Ba4Ge25 under pressure, from which the density of states at the Fermi energy N(EF) is determined. It demonstrates that, in Ba6Ge25, the structural phase transition causes a significant reduction of N(EF) (by a factor of about 4) and therefore largely weakens superconductivity. Furthermore, the drastic enhancement of Tc under pressure is found to be solely governed by N(EF).
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Ba6Ge25 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 0.24 | Pressure unresolved | unknown |
| Ba6Ge25 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 0.14 | Pressure unresolved | unknown |
| Ba6Ge25 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 3.8 | 2.8 GPa | unknown |
| Na2Ba4Ge25 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 0.84 | Pressure unresolved | unknown |
| Na2Ba4Ge25 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 0.84 | Pressure unresolved | unknown |
Similar papers
Superconductivity in the Filled Cage Compounds Ba6Ge25 and Ba4Na2Ge25
similarity 0.96F. M. Grosche et al.
Source status unknown — claims are unverified
Superconductivity in germanium clathrate Ba8Ga16Ge30
similarity 0.93J. D. Bryan et al.
Source status unknown — claims are unverified
Enhanced high-pressure superconductivity and local structure of the Ba8Si46 clathrate
similarity 0.92F. Morales et al.
Source status unknown — claims are unverified
High-pressure synthesis and superconductivity of LaGe5 containing a tunnel germanium network
similarity 0.91Hiroshi Fukuoka & Shoji Yamanaka
Source status unknown — claims are unverified
Superconductivity and physical properties of Ba24Si100 determined from electric transport, specific-heat capacity, and magnetic susceptibility measurements
similarity 0.91Takeshi Rachi et al.
Source status unknown — claims are unverified
Superconductivity in Ban+2Ir4nGe12n+4 (n=1,2) with cage structure and softening of low-lying localized mode
similarity 0.91Jiangang Guo et al.
Source status unknown — claims are unverified