Fe<font size="-1">1+δ</font>Se<font size="-1">x</font>Te<font size="-1">1-x</font>における超伝導と反強磁性量子臨界点近傍の物性
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Macroscopic and microscopic physical properties of Fe<font size="-1">1+δ</font>Se<font size="-1">x</font>Te<font size="-1">1-x</font> were investigated through the magnetic susceptibility, electrical resistivity, heat capacity and nuclear magnetic resonance (NMR) measurements. The mother compound Fe<font size="-1">1.14</font>Te shows an antiferromagnetic phase transition accompanied by the structural change at 61.5K. The antiferromagnetic transition temperature of Fe<font size="-1">1+δ</font>Se<font size="-1">x</font>Te<font size="-1">1-x</font> decreases with increasing x, then the superconducting transition appears above x = 0.2. The superconductivity with clean limit occurs when δ is small. In such a compound, the temperature dependence of the nuclear spin - lattice relaxation rate and the electron contributed specific heat reveals presence of the nodal superconducting gap structure, suggesting that the superconductivity occurs in an unconventional mechanism. From a systematic investigation of the nuclear spin - lattice relaxation rate in Fe<font size="-1">1+δ</font>Se<font size="-1">x</font>Te<font size="-1">1-x</font>, it was found that the antiferromagnetic quantum critical point lies at x ∼0.03. The superconductivity occurs in the vicinity of the antiferromagnetic quantum critical point, resulting in that the superconductivity in Fe<font size="-1">1+δ</font>Se<font size="-1">x</font>Te<font size="-1">1-x</font> is mediated by the antiferromagnetic spin fluctuations.
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