Complex biphase nature of the superconducting dome of the FeSe phase diagram
V. Svitlyk, M. Raba, V. Dmitriev, P. Rodière, P. Toulemonde, D. Chernyshov, M. Mezouar
DOI 10.1103/PhysRevB.96.014520 · 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
Single crystal synchrotron x-ray diffraction as a function of temperature and pressure has revealed a complex biphase mixture in superconducting FeSe. Based on our experimental results, we construct a phase diagram where structural behavior and superconducting properties of FeSe are found to be correlated. We show that below 6 GPa, where pressure promotes the superconducting critical temperature, the FeSe structure is composed of two-dimensional layers of edge-shared FeSe4 tetrahedra, while above 6 GPa, the superconductivity is strongly suppressed on formation of a new orthorhombic polymorph characterized by a three-dimensional network of face sharing FeSe6 octahedra. Therefore, changes in topology and connectivity of the FeSe structure are found to be detrimental to superconductivity. The previously controversial crystal structure of the high-pressure polymorph of FeSe was unambiguously determined in the present paper. High-pressure FeSe adopts an orthorhombic MnP-type structure (Pnma) which corresponds to a slightly distorted hexagonal NiAs-type arrangement (P63/mmc). The structural transformation from the low- to high-pressure FeSe polymorph is first order in nature and is manifested as antiparallel displacements within the Fe and Se sublattices.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| FeSe Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 8.5 | Pressure unresolved | unknown |
| FeSe Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 37 | 6 GPa | unknown |
| FeSe Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 65 | Pressure not reported | unknown |
Similar papers
Complex biphase nature of the superconducting dome of the FeSe phase diagram
similarity 1.00V. Svitlyk et al. · 2016 · arXiv:1611.07768
Source status unknown — claims are unverified
Evolution of the superconducting properties in FeSe1−xSx
similarity 0.95S. A. Moore et al.
Source status unknown — claims are unverified
Extended Magnetic Dome Induced by Low Pressures in Superconducting FeSe1−xSx
similarity 0.95S. Holenstein et al.
Source status unknown — claims are unverified
Discrete superconducting phases in proton-intercalated FeSe thin flakes
similarity 0.95W. X. Wang et al.
Source status unknown — claims are unverified
Interplay between lattice and spin states degree of freedom in the FeSe superconductor: Dynamic spin state instabilities
similarity 0.95Vladimir Gnezdilov et al.
Source status unknown — claims are unverified
Superconductivity in monolayer FeSe enhanced by quantum geometry
similarity 0.95Taisei Kitamura et al.
Source status unknown — claims are unverified