TY - JOUR
T1 - Structural phase transition, antiferromagnetism and two superconducting domes in LaFeAsO1-xFx (0 < x ≤ 0.75)
AU - Yang, Jie
AU - Oka, Toshihide
AU - Li, Zheng
AU - Yang, Huai Xin
AU - Li, Jian Qi
AU - Chen, Gen Fu
AU - Zheng, Guo Qing
N1 - Funding Information:
This work was supported by the National Key Research and Development Program of China (Grant No. 2017YFA0302904), the National Natural Science Foundation of China (Grant Nos. 11674377, and 11634015), and the Chinese Academy of Sciences (Grant No. XDB07020200). Work in Okayama was supported by research grants from Japan Society for the Promotion of Science (JSPS) (Grant No. 16H0401618). Jie Yang is supported by the Youth Innovation Promotion Association of Chinese Academy of Sciences. We thank Zhong-Xian Zhao for useful communication and Shinji Kawasaki for help in some of the measurements.
Publisher Copyright:
© 2018, Science China Press and Springer-Verlag GmbH Germany, part of Springer Nature.
PY - 2018/11/1
Y1 - 2018/11/1
N2 - We report 75As nuclear magnetic resonance (NMR)/nuclear quadrupole resonance (NQR) and transmission electron microscopy (TEM) studies on LaFeAsO1−xFx. There are two superconducting domes in this material. The first one appears at 0.03 ≤ x ≤ 0.2 with Tc max = 27 K, and the second one at 0.25 ≤ x ≤ 0.75 with Tc max = 30 K. By NMR and TEM, we demonstrate that a C4-to-C2 structural phase transition (SPT) takes place above both domes, with the transition temperature Ts varying strongly with x. In the first dome, the SPT is followed by an antiferromagnetic (AF) transition, but neither AF order nor low-energy spin fluctuations are found in the second dome. By 75As nuclear spin-lattice relaxation rate (1/T1) measurements, we find that AF order and superconductivity coexist microscopically in LaFeAsO0.97F0.03. In the coexisting region, 1/T1 decreases at Tc but becomes proportional to T below 0.6Tc, indicating gapless excitations. Therefore, in contrast to the early reports, the obtained phase diagram for x ≤ 0.2 is quite similar to the doped BaFe2As2 system. The electrical resistivity ρ in the second dome can be fitted by ρ = ρ0 + ATn with n = 1 and a maximal coefficient A at around xopt = 0.5-0.55 at which Ts extrapolates to zero and Tc is the maximal, which suggests the importance of quantum critical fluctuations associated with the SPT. We have constructed a complete phase diagram of LaFeAsO1−xFx, which provides insight into the relationship between SPT, antiferromagnetism and superconductivity.
AB - We report 75As nuclear magnetic resonance (NMR)/nuclear quadrupole resonance (NQR) and transmission electron microscopy (TEM) studies on LaFeAsO1−xFx. There are two superconducting domes in this material. The first one appears at 0.03 ≤ x ≤ 0.2 with Tc max = 27 K, and the second one at 0.25 ≤ x ≤ 0.75 with Tc max = 30 K. By NMR and TEM, we demonstrate that a C4-to-C2 structural phase transition (SPT) takes place above both domes, with the transition temperature Ts varying strongly with x. In the first dome, the SPT is followed by an antiferromagnetic (AF) transition, but neither AF order nor low-energy spin fluctuations are found in the second dome. By 75As nuclear spin-lattice relaxation rate (1/T1) measurements, we find that AF order and superconductivity coexist microscopically in LaFeAsO0.97F0.03. In the coexisting region, 1/T1 decreases at Tc but becomes proportional to T below 0.6Tc, indicating gapless excitations. Therefore, in contrast to the early reports, the obtained phase diagram for x ≤ 0.2 is quite similar to the doped BaFe2As2 system. The electrical resistivity ρ in the second dome can be fitted by ρ = ρ0 + ATn with n = 1 and a maximal coefficient A at around xopt = 0.5-0.55 at which Ts extrapolates to zero and Tc is the maximal, which suggests the importance of quantum critical fluctuations associated with the SPT. We have constructed a complete phase diagram of LaFeAsO1−xFx, which provides insight into the relationship between SPT, antiferromagnetism and superconductivity.
KW - antiferromagnetism
KW - nuclear magnetic resonance
KW - structural phase transition
KW - superconductivity
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U2 - 10.1007/s11433-018-9240-0
DO - 10.1007/s11433-018-9240-0
M3 - Article
AN - SCOPUS:85049327334
SN - 1674-7348
VL - 61
JO - Science China: Physics, Mechanics and Astronomy
JF - Science China: Physics, Mechanics and Astronomy
IS - 11
M1 - 117411
ER -