Superconductivity and magnetism in RbxFe2−ySe2: Impact of thermal treatment on mesoscopic phase separation
S. Weyeneth, M. Bendele, F. von Rohr, P. Dluzewski, R. Puzniak, A. Krzton-Maziopa, S. Bosma, Z. Guguchia, R. Khasanov, Z. Shermadini, A. Amato, E. Pomjakushina, K. Conder, A. Schilling, H. Keller
DOI 10.1103/PhysRevB.86.134530 · 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
An extended study of the superconducting and normal-state properties of various as-grown and post-annealed RbxFe2−ySe2 single crystals is presented. Magnetization experiments evidence that annealing of RbxFe2−ySe2 at 413 K, well below the onset of phase separation Tp≃489 K, neither changes the magnetic nor the superconducting properties of the crystals. In addition, annealing at 563 K, well above Tp, suppresses the superconducting transition temperature Tc and leads to an increase of the antiferromagnetic susceptibility accompanied by the creation of ferromagnetic impurity phases, which are developing with annealing time. However, annealing at T=488K≃Tp increases Tc up to 33.3 K, sharpens the superconducting transition, increases the lower critical field, and strengthens the screening efficiency of the applied magnetic field. Resistivity measurements of the as-grown and optimally annealed samples reveal an increase of the upper critical field along both crystallographic directions as well as its anisotropy. Muon spin rotation and scanning transmission electron microscopy experiments suggest the coexistence of two phases below Tp: a magnetic majority phase of Rb2Fe4Se5 and a nonmagnetic minority phase of Rb0.5Fe2Se2. Both microscopic techniques indicate that annealing the specimens just at Tp does not affect the volume fraction of the two phases, although the magnetic field distribution in the samples changes substantially. This suggests that the microstructure of the sample, caused by mesoscopic phase separation, is modified by annealing just at Tp, leading to an improvement of the superconducting properties of RbxFe2−ySe2 and an enhancement of Tc.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| RbxFe2-ySe2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 33.3 | Pressure not reported | onset |
| RbxFe2-ySe2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 30.1 | Pressure not reported | onset |
| RbxFe2-ySe2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 30 | Pressure not reported | onset |
| RbxFe2-ySe2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 31.6 | Pressure not reported | onset |
| RbxFe2-ySe2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 31.7 | Pressure not reported | onset |
| RbxFe2-ySe2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 31.8 | Pressure not reported | onset |
| RbxFe2-ySe2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 28 | Pressure not reported | onset |
| RbxFe2-ySe2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 21.8 | Pressure not reported | onset |
| RbxFe2-ySe2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 33.1 | Pressure not reported | onset |
| FeSe1-x Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 8 | Pressure not reported | unknown |
Similar papers
Correlation between superconductivity and antiferromagnetism in Rb0.8Fe2−ySe2−xTex single crystals
similarity 0.96Dachun Gu et al.
Source status unknown — claims are unverified
Magnetic imaging of antiferromagnetic and superconducting phases in RbxFe2−ySe2 crystals
similarity 0.96J. Hazi et al.
Source status unknown — claims are unverified
Superconductivity close to magnetic instability in Fe(Se1−xTex)0.82
similarity 0.96M. H. Fang et al.
Source status unknown — claims are unverified
Pressure dependence of the electronic structure and spin state in Fe1.01Se superconductors probed by x-ray absorption and x-ray emission spectroscopy
similarity 0.96J. M. Chen et al.
Source status unknown — claims are unverified
Disorder-dependent superconducting phase diagram at high magnetic fields in Fe1+ySexTe1−x (x∼0.4)
similarity 0.96T. Gebre et al.
Source status unknown — claims are unverified
Superconductivity at 32 K in single-crystalline RbxFe2−ySe2
similarity 0.96A. F. Wang et al.
Source status unknown — claims are unverified