TY - JOUR
T1 - Electronic and magnetic phase diagram of superconductors, SmFeAsO 1-xFx
AU - Kamihara, Yoichi
AU - Nomura, Takatoshi
AU - Hirano, Masahiro
AU - Kim, Jung Eun
AU - Kato, Kenichi
AU - Takata, Masaki
AU - Kobayashi, Yasuhiro
AU - Kitao, Shinji
AU - Higashitaniguchi, Satoshi
AU - Yoda, Yoshitaka
AU - Seto, Makoto
AU - Hosono, Hideo
PY - 2010/3/5
Y1 - 2010/3/5
N2 - A crystallographic and magnetic phase diagram of SmFeAsO 1-xFx is determined as a function of x in terms of temperature based on electrical transport and magnetization, synchrotron powder x-ray diffraction, 57Fe Mössbauer spectra (MS), and 149Sm nuclear resonant forward scattering (NRFS) measurements. MS revealed that the magnetic moments of Fe were aligned antiferromagnetically at ~144 K (TN(Fe)). The magnetic moment of Fe (MFe) is estimated to be 0.34 μB/Fe at 4.2 K for undoped SmFeAsO; MFe is quenched in superconducting F-doped SmFeAsO. 149Sm NRFS spectra revealed that the magnetic moments of Sm start to order antiferromagnetically at 5.6 K (undoped) and 4.4 K (TN(Sm)) (x = 0.069). Results clearly indicate that the antiferromagnetic (AF) Sm sublattice coexists with the superconducting phase in SmFeAsO1-xFx below T N(Sm), while the AF Fe sublattice does not coexist with the superconducting phase.
AB - A crystallographic and magnetic phase diagram of SmFeAsO 1-xFx is determined as a function of x in terms of temperature based on electrical transport and magnetization, synchrotron powder x-ray diffraction, 57Fe Mössbauer spectra (MS), and 149Sm nuclear resonant forward scattering (NRFS) measurements. MS revealed that the magnetic moments of Fe were aligned antiferromagnetically at ~144 K (TN(Fe)). The magnetic moment of Fe (MFe) is estimated to be 0.34 μB/Fe at 4.2 K for undoped SmFeAsO; MFe is quenched in superconducting F-doped SmFeAsO. 149Sm NRFS spectra revealed that the magnetic moments of Sm start to order antiferromagnetically at 5.6 K (undoped) and 4.4 K (TN(Sm)) (x = 0.069). Results clearly indicate that the antiferromagnetic (AF) Sm sublattice coexists with the superconducting phase in SmFeAsO1-xFx below T N(Sm), while the AF Fe sublattice does not coexist with the superconducting phase.
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U2 - 10.1088/1367-2630/12/3/033005
DO - 10.1088/1367-2630/12/3/033005
M3 - Article
AN - SCOPUS:77951198972
SN - 1367-2630
VL - 12
JO - New Journal of Physics
JF - New Journal of Physics
M1 - 033005
ER -