TY - JOUR
T1 - 75As and 139La NMR studies on LaFeAs (O1 - x Fx)
AU - Ishida, K.
AU - Nakai, Y.
AU - Kitagawa, S.
AU - Kamihara, Y.
AU - Hirano, M.
AU - Hosono, H.
N1 - Funding Information:
We thank Y. Ihara, K. Kitagawa, Y. Maeno and K. Yoshimura for experimental supports and valuable discussions. We also thank H. Ikeda, S. Fujimoto and K. Yamada for valuable theoretical discussions. This work was supported by the grant-in-aid for the Global COE Program “The Next Generation of Physics, Spun from Universality and Emergence” from the Ministry of Education, Culture, Sports, Science and Technology (MEXT) of Japan and by the grants-in-aid for Scientific Research from Japan Society for Promotion of Science (JSPS). One of the authors (Y.N.) is financially supported as a JSPS Research Fellow.
PY - 2009/10/15
Y1 - 2009/10/15
N2 - We report experimental results of 75As and 139La nuclear magnetic resonance (NMR) in the layered oxypnictide system LaFeAs (O1 - x Fx) (x = 0.0, 0.04, 0.07 and 0.11) where superconductivity occurs in x greater than 0.04. In the undoped LaFeAsO, 1 / T1 of 139La exhibits a distinct peak at TN ~ 142 K below which the La NMR spectra become broadened due to the internal magnetic field attributed to an antiferromagnetic (AFM) ordering. In the x = 0.04 sample, 1 / T1 T of 75As exhibits a Curie-Weiss temperature dependence down to 30 K, suggesting the development of AFM spin fluctuations with decreasing temperature. In the x = 0.11 sample, in contrast, pseudogap behavior is observed in 1 / T1 T at the 75As site with a gap value of ΔPG ~ 175 K. The spin dynamics vary markedly with F-doping, which is ascribed to the change of the Fermi-surface structure by the electron-doping. As for the superconducting properties for x = 0.04, 0.07 and 0.11, 1 / T1 of 75As in all compounds does not exhibit a coherence peak just below Tc and follows a T3 dependence at low temperatures. These results seemingly suggests that unconventional superconductivity with zero gap along lines, whereas the lack of the residual density of states at the low temperatures is incompatible with the presence of the line-nodes. We discuss similarity and difference between LaFeAs (O1 - x Fx) and cuprates, and also discuss the relationship between spin dynamics and superconductivity on the basis of F-doping dependence of Tc and 1 / T1. Crown
AB - We report experimental results of 75As and 139La nuclear magnetic resonance (NMR) in the layered oxypnictide system LaFeAs (O1 - x Fx) (x = 0.0, 0.04, 0.07 and 0.11) where superconductivity occurs in x greater than 0.04. In the undoped LaFeAsO, 1 / T1 of 139La exhibits a distinct peak at TN ~ 142 K below which the La NMR spectra become broadened due to the internal magnetic field attributed to an antiferromagnetic (AFM) ordering. In the x = 0.04 sample, 1 / T1 T of 75As exhibits a Curie-Weiss temperature dependence down to 30 K, suggesting the development of AFM spin fluctuations with decreasing temperature. In the x = 0.11 sample, in contrast, pseudogap behavior is observed in 1 / T1 T at the 75As site with a gap value of ΔPG ~ 175 K. The spin dynamics vary markedly with F-doping, which is ascribed to the change of the Fermi-surface structure by the electron-doping. As for the superconducting properties for x = 0.04, 0.07 and 0.11, 1 / T1 of 75As in all compounds does not exhibit a coherence peak just below Tc and follows a T3 dependence at low temperatures. These results seemingly suggests that unconventional superconductivity with zero gap along lines, whereas the lack of the residual density of states at the low temperatures is incompatible with the presence of the line-nodes. We discuss similarity and difference between LaFeAs (O1 - x Fx) and cuprates, and also discuss the relationship between spin dynamics and superconductivity on the basis of F-doping dependence of Tc and 1 / T1. Crown
KW - LaFeAsO
KW - NMR/NQR
KW - Nuclear-spin-lattice relaxation rate (1 / T)
KW - Oxypnictide
KW - Pseudogap
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U2 - 10.1016/j.physb.2009.07.078
DO - 10.1016/j.physb.2009.07.078
M3 - Article
AN - SCOPUS:70349124579
SN - 0921-4526
VL - 404
SP - 3089
EP - 3094
JO - Physica B: Condensed Matter
JF - Physica B: Condensed Matter
IS - 19
ER -