Structural evolution and phase diagram of the superconducting iron selenides Lix(C2H8N2)yFe2Se2(x=0∼0.8)
Linlin Zhao, Da Wang, Qingzhen Huang, Hui Wu, Ruijin Sun, Xiao Fan, Yanpeng Song, Shifeng Jin, Xiaolong Chen
DOI 10.1103/PhysRevB.99.094503 · 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
Here we report on the structural and electronic phase diagram of lithium and ethylenediamine intercalated FeSe in a wide range of dopant concentration (x=0∼0.8). Undoped (C2H8N2)yFe2Se2 crystallizes in an orthorhombic phase. With increasing lithium doping, an orthorhombic to tetragonal phase transition occurs at x=0.35, and the superconducting tetragonal phase persists until x=0.5. Meanwhile, the Tc is found dependent strongly on dopant concentration, raising rapidly from 30 K at x=0.35 to 45 K at x=0.5. The crystal structures of Li0.31(3)(C2H8N2)0.52(7)Fe2.03(2)Se2 are determined by using high-resolution neutron diffraction data at 5, 60, 150, and 295 K, respectively. The distortion of the FeSe tetrahedron is enhanced significantly from 150 to 295 K, meanwhile, the normal-state Hall resistivity changes sign from negative to positive in the same temperature range. The dominant hole carrier in electron-doped Li0.5(C2H8N2)yFe2Se2 above 230 K suggests that the temperature-induced structure distortion may lead to a reconstruction of the Fermi surface topology and the appearance of hole pockets.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Li0.35(C2H8N2)yFe2Se2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 30 | Pressure not reported | onset |
| Li0.5(C2H8N2)yFe2Se2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 45 | Pressure not reported | onset |
Similar papers
Enhanced superconducting transition temperature in hyper-interlayer-expanded FeSe despite the suppressed electronic nematic order and spin fluctuations
similarity 0.95Matevž Majcen Hrovat et al.
Source status unknown — claims are unverified
Superconductivity in the iron selenide KxFe2Se2 (0≤x≤1.0)
similarity 0.94Jiangang Guo et al.
Source status unknown — claims are unverified
Local structure and phonon states mediated by intercalation-driven doping in superconducting Li1.0(C5H5N)yFe2−zSe2
similarity 0.93Alexandros Deltsidis et al.
Source status unknown — claims are unverified
Superconductivity and phase diagram of (Li0.8Fe0.2)OHFeSe1−xSx
similarity 0.93X. F. Lu et al.
Source status unknown — claims are unverified
Enhanced superconductivity and anisotropy of FeTe0.6Se0.4 single crystals with Li−NH3 intercalation
similarity 0.93Chenghe Li (李承贺) et al.
Source status unknown — claims are unverified
Robustness of superconducting properties to transition metal substitution and impurity phases in Fe1−xVxSe
similarity 0.93Franziska K. K. Kirschner et al.
Source status unknown — claims are unverified