Evolution of structure and superconductivity in Ba(Ni1−xCox)2As2
Chris Eckberg, Limin Wang, Halyna Hodovanets, Hyunsoo Kim, Daniel J. Campbell, Peter Zavalij, Philip Piccoli, Johnpierre Paglione
DOI 10.1103/PhysRevB.97.224505 · 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 effects of Co substitution on Ba(Ni1−xCox)2As2 (0≤x≤0.251) single crystals grown out of Pb flux are investigated via transport, magnetic, and thermodynamic measurements. BaNi2As2 exhibits a first-order tetragonal to triclinic structural phase transition at Ts=137 K upon cooling, and enters a superconducting phase below Tc=0.7 K. The structural phase transition is sensitive to cobalt content and is suppressed completely by x≥0.133. The superconducting critical temperature, Tc, increases continuously with x, reaching a maximum of Tc=2.3 K at x=0.083 and then decreases monotonically until superconductivity is no longer observable well into the tetragonal phase. In contrast to similar BaNi2As2 substitutional studies, which show an abrupt change in Tc at the triclinic-tetragonal boundary that extends far into the tetragonal phase, Ba(Ni1−xCox)2As2 exhibits a domelike phase diagram centered around the zero-temperature tetragonal-triclinic boundary. Together with an anomalously large heat capacity jump ΔCe/γT∼2.2 near optimal doping, the smooth evolution of Tc in the Ba(Ni1−xCox)2As2 system suggests a mechanism for pairing enhancement other than phonon softening.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| BaNi2As2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 0.7 | Pressure not reported | unknown |
| Ba(Ni1-xCox)2As2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 2.3 | Pressure not reported | unknown |
| Ba(Ni0.917Co0.083)2As2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 2.3 | Pressure not reported | unknown |
| Ba(Ni0.937Co0.063)2As2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 1.8 | Pressure not reported | midpoint |
Similar papers
Unconventional Charge Density Wave Order in the Pnictide Superconductor Ba(Ni1−xCox)2As2
similarity 0.96Sangjun Lee et al.
Source status unknown — claims are unverified
Competing superconducting and magnetic order parameters and field-induced magnetism in electron-doped Ba(Fe1−xCox)2As2
similarity 0.96J. Larsen et al.
Source status unknown — claims are unverified
Impact of Ca substitution on competing orders in superconducting BaNi2As2
similarity 0.95F. Henssler et al.
Source status unknown — claims are unverified
Electrodynamics of electron-doped iron pnictide superconductors: Normal-state properties
similarity 0.95N. Barišić et al.
Source status unknown — claims are unverified
Superconductivity at 22 K in Co-Doped BaFe2As2 Crystals
similarity 0.95Athena S. Sefat et al.
Source status unknown — claims are unverified
Structure determination in thin film Ba1−xLaxFe2As2: Relation between the FeAs4 geometry and superconductivity
similarity 0.95Kensuke Kobayashi et al.
Source status unknown — claims are unverified