TY - JOUR
T1 - Magnetic and superconducting properties of CeTX3 (T
T2 - Transition metal and X: Si and Ge) with non-centrosymmetric crystal structure
AU - Kawai, Tomoya
AU - Muranaka, Hiroshi
AU - Measson, Marie Aude
AU - Shimoda, Tetsuya
AU - Doi, Yusuke
AU - Matsuda, Tatsuma D.
AU - Haga, Yoshinori
AU - Knebel, Georg
AU - Lapertot, Gérard
AU - Aoki, Dai
AU - Flouquet, Jacques
AU - Takeuchi, Tetsuya
AU - Settai, Rikio
AU - Onuki, Yoshichika
PY - 2008/6
Y1 - 2008/6
N2 - We grew single crystals of non-centrosymmetric compounds CeTSi3 and CeTGe3 (T: transition metal), and studied the magnetic properties by measuring the electrical resistivity, magnetic susceptibility and magnetization. We also studied the effect of pressure on the electronic states in antiferromagnets CeTGe3 (T: Co, Rh, Ir) by measuring the resistivity under pressure. No noticeable change of the Néel temperature was observed up to 8 GPa in CeRhGe3 and CeIrGe3, which are far from the magnetic quantum critical point. On the other hand, the Néel temperature in CeCoGe3 was strongly decreased as a function of pressure, and pressure-induced superconductivity was observed in the pressure region from 5.4 GPa to about 7.5 GPa. The slope of upper critical field Hc2 at 6.5 GPa is found to be extremely large, with an upturn curvature of Hc2 with decreasing temperature: -dHc2/dT = 200 kOe/K at the superconducting transition temperature Tsc = 0.69 K, revealing unconventional superconductivity.
AB - We grew single crystals of non-centrosymmetric compounds CeTSi3 and CeTGe3 (T: transition metal), and studied the magnetic properties by measuring the electrical resistivity, magnetic susceptibility and magnetization. We also studied the effect of pressure on the electronic states in antiferromagnets CeTGe3 (T: Co, Rh, Ir) by measuring the resistivity under pressure. No noticeable change of the Néel temperature was observed up to 8 GPa in CeRhGe3 and CeIrGe3, which are far from the magnetic quantum critical point. On the other hand, the Néel temperature in CeCoGe3 was strongly decreased as a function of pressure, and pressure-induced superconductivity was observed in the pressure region from 5.4 GPa to about 7.5 GPa. The slope of upper critical field Hc2 at 6.5 GPa is found to be extremely large, with an upturn curvature of Hc2 with decreasing temperature: -dHc2/dT = 200 kOe/K at the superconducting transition temperature Tsc = 0.69 K, revealing unconventional superconductivity.
KW - CeCoGe
KW - CeIrGe
KW - CeRhGe
KW - CeRuSi
KW - Magnetic susceptibility
KW - Non-centrosymmetry
KW - Pressure-induced superconductivity
KW - Upper critical field
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U2 - 10.1143/JPSJ.77.064716
DO - 10.1143/JPSJ.77.064716
M3 - Article
AN - SCOPUS:54349124810
SN - 0031-9015
VL - 77
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 6
M1 - 064716
ER -