Metal-insulator transition and superconductivity induced by Rh doping in the binary pnictides RuPn (Pn=P, As, Sb)
Daigorou Hirai, Tomohiro Takayama, Daisuke Hashizume, Hidenori Takagi
DOI 10.1103/PhysRevB.85.140509 · 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
Binary ruthenium pnictides, RuP and RuAs, with an orthorhombic MnP structure, were found to show a metal to a nonmagnetic insulator transition at TMI = 270 and 200 K, respectively. In the metallic region above TMI, a structural phase transition, accompanied with a weak anomaly in the resistivity and the magnetic susceptibility, indicative of a pseudogap formation, was identified at Ts = 330 and 280 K, respectively. These two transitions were suppressed by substituting Ru with Rh. We found superconductivity with a maximum Tc = 3.7 and 1.8 K in a narrow composition range around the critical point for the pseudogap phase, Rh content xc = 0.45 and 0.25 for Ru1−xRhxP and Ru1−xRhxAs, respectively, which may provide us with a nonmagnetic route to superconductivity at a quantum critical point.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Ru0.55Rh0.45P Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 3.7 | Pressure not reported | zero_resistance |
| Ru0.55Rh0.45P Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 3.7 | Pressure not reported | onset |
| Ru0.55Rh0.45P Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 3.7 | Pressure not reported | midpoint |
| Ru0.75Rh0.25As Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 1.8 | Pressure not reported | zero_resistance |
| Ru0.75Rh0.25As Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 1.8 | Pressure not reported | onset |
| Ru0.75Rh0.25As Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 1.8 | Pressure not reported | midpoint |
| RuSb Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 1.2 | Pressure not reported | unknown |
Similar papers
Metal-insulator transition and superconductivity induced by Rh doping in binary Ru Pnictides RuPn (Pn = P, As and Sb)
similarity 1.00D. Hirai et al. · 2011 · arXiv:1112.0604
Source status unknown — claims are unverified
Superconductivity in Ru0.55Rh0.45P and Ru0.75Rh0.25As probed by muon spin relaxation and rotation measurements
similarity 0.94V. K. Anand et al.
Source status unknown — claims are unverified
Pseudogap behavior of RuP probed by photoemission spectroscopy
similarity 0.92K. Sato et al. · 2012 · arXiv:1205.2669
Source status unknown — claims are unverified
Superconductivity and ferromagnetism in hole-doped RbEuFe4As4
similarity 0.91Yi Liu et al.
Source status unknown — claims are unverified
Mixed-parity superconductivity in centrosymmetric crystals
similarity 0.91I. A. Sergienko
Source status unknown — claims are unverified
Magnetic ordering and superconductivity in R2Rh3Sn5(R=La-Tm,Y) systems
similarity 0.91N. G. Patil & S. Ramakrishnan
Source status unknown — claims are unverified