TY - JOUR
T1 - As-NQR study of superconductivity in LaRAsO1-xFx (R=Fe and Ni)
AU - Oka, T.
AU - Tabuchi, T.
AU - Li, Z.
AU - Kawasaki, S.
AU - Chen, G. F.
AU - Luo, J. L.
AU - Wang, N. L.
AU - Zheng, Guo Qing
N1 - Funding Information:
This work was supported in part by research Grants from MEXT and JSPS, Japan, NSFC of China, and the ITSNEM program of CAS.
PY - 2011/5
Y1 - 2011/5
N2 - We report 75As nuclear quadrupole resonance (NQR) studies on oxypnictide superconductors LaFeAsO1-xFx (x=0.08, 0.15) and LaNiAsO1-xFx (x=0, 0.06, 0.10, 0.12). In LaFeAsO 0.92F0.08 (Tc=23 K), nuclear spin-lattice relaxation rate 1/T1 shows no coherence peak just below Tc and decreases with decreasing temperature accompanied by a hump structure at T∼0.4Tc, which is a characteristic of the multigap superconductivity. In the normal state, the quantity 1/T1T increases with decreasing temperature to Tc, indicating that the existence of antiferromagnetic correlation originating from its multiple electronic band structure. On the other hand, LaNiAsO1-xFx shows a clear HebelSlichter (coherence) peak just below Tc, evidencing that the LaNiAsO1-xFx is a BCS superconductor. In the normal state, 1/T1T is constant in the temperature range 4≤T≤10K for all LaNiAsO1-xFx, which indicates electron correlations are weak. We suggest that the contrasting behavior of both superconductivity and electron correlations in LaFeAsO0.92F0.08 and LaNiAsO 1-xFx between them relate to the difference of electronic band structure configuration. We also provide a possible interpretation for the pseudogap-like behavior in the normal state observed in both compounds.
AB - We report 75As nuclear quadrupole resonance (NQR) studies on oxypnictide superconductors LaFeAsO1-xFx (x=0.08, 0.15) and LaNiAsO1-xFx (x=0, 0.06, 0.10, 0.12). In LaFeAsO 0.92F0.08 (Tc=23 K), nuclear spin-lattice relaxation rate 1/T1 shows no coherence peak just below Tc and decreases with decreasing temperature accompanied by a hump structure at T∼0.4Tc, which is a characteristic of the multigap superconductivity. In the normal state, the quantity 1/T1T increases with decreasing temperature to Tc, indicating that the existence of antiferromagnetic correlation originating from its multiple electronic band structure. On the other hand, LaNiAsO1-xFx shows a clear HebelSlichter (coherence) peak just below Tc, evidencing that the LaNiAsO1-xFx is a BCS superconductor. In the normal state, 1/T1T is constant in the temperature range 4≤T≤10K for all LaNiAsO1-xFx, which indicates electron correlations are weak. We suggest that the contrasting behavior of both superconductivity and electron correlations in LaFeAsO0.92F0.08 and LaNiAsO 1-xFx between them relate to the difference of electronic band structure configuration. We also provide a possible interpretation for the pseudogap-like behavior in the normal state observed in both compounds.
KW - D. Nuclear quadrupole resonance
KW - D. Superconductivity
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U2 - 10.1016/j.jpcs.2010.10.022
DO - 10.1016/j.jpcs.2010.10.022
M3 - Article
AN - SCOPUS:79955759976
SN - 0022-3697
VL - 72
SP - 497
EP - 500
JO - Journal of Physics and Chemistry of Solids
JF - Journal of Physics and Chemistry of Solids
IS - 5
ER -