Systematic variation of superconductivity for the quaternary borocarbide system RNi2B2C (R=Sc, Y, La, Th, U, or a lanthanide)
C. C. Lai, M. S. Lin, Y. B. You, H. C. Ku
DOI 10.1103/PhysRevB.51.420 · 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
A superconducting transition temperature Tc of 8.0 K is reported for the nonmagnetic (Th4+) ThNi2B2C compound with the LuNi2B2C-type structure and a derived coherence length ξ(0) of 230 Å and a penetration depth λ(0) of 860 Å. No transition down to 2 K was observed for the magnetic, mixed-valence (U4+/U6+ or average valence of +5.2) UNi2B2C compound with the same structure. Systematic variation of Tc for the quaternary and pseudoquaternary compounds in the RNi2B2C system (R=Sc, Y, La, Lu, Th, U, or magnetic lanthanides) is studied through the variation of Tc with the R ionic radius, Ni-Ni nearest-neighbor in-plane distance, and the normal-state Pauli-like temperature-independent paramagnetic susceptibility. Maximum Tc at 16.6 K for LuNi2B2C with an optimum Ni-Ni distance of 2.45 Å was observed, along with a large normal-state Pauli paramagnetic susceptibility. As a comparison, the 8.0-K ThNi2B2C superconductor has a longer Ni-Ni distance of 2.60 Å and a smaller normal-state susceptibility. Variations of the Ni(3d)-dominated conduction band and the density of states at the Fermi level N(EF) are believed to be the driving force for the Tc variation of nonmagnetic compounds in the present system.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| ThNi2B2C Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 8 | Pressure not reported | zero_resistance |
| ThNi2B2C Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 8.4 | Pressure not reported | midpoint |
| ThNi2B2C Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 8.9 | Pressure not reported | onset |
| ThNi2B2C Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 8 | Pressure not reported | onset |
| (La0.5Th0.5)Ni2B2C Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 3.9 | Pressure not reported | onset |
| LuNi2B2C Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 16.6 | Pressure not reported | unknown |
| YNi2B2C Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 15.6 | Pressure not reported | unknown |
Similar papers
Electronic structure of Ni-based superconducting quaternary compounds: YNi2B2X (X=B, C, N, and O)
similarity 0.96J. I. Lee et al.
Source status unknown — claims are unverified
Superconductivity and magnetism in DyNi2B2C single crystals
similarity 0.96C. V. Tomy et al.
Source status unknown — claims are unverified
Electronic structure and phase-stability studies on superconducting YNi2B2C, YRh3B, and nonsuperconducting YNi4B
similarity 0.96P. Ravindran et al.
Source status unknown — claims are unverified
Superconductivity in RPt2B2C
similarity 0.96R. J. Cava et al.
Source status unknown — claims are unverified
Ab initio investigation of BCS-type superconductivity in LuNi2B2C-type superconductors
similarity 0.96H. M. Tütüncü et al.
Source status unknown — claims are unverified
Structural, superconducting, and magnetic properties of YNi2B2C and ErNi2B2C
similarity 0.96C. Godart et al.
Source status unknown — claims are unverified