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Si金子 耕士; Stockert, O.*; F
k, B.*; Raymond, S.*; Skoulatos, M.*; 竹内 徹也*; 大貫 惇睦*
Physical Review B, 89(24), p.241105_1 - 241105_5, 2014/06
被引用回数：2 パーセンタイル：9.77(Materials Science, Multidisciplinary)The effect of magnetic field on the static and dynamic spin correlations in the non-centrosymmetric heavy-fermion superconductor CePtSi was investigated by neutron scattering. The application of a magnetic field B increases the antiferromagnetic (AFM) peak intensity. This increase depends strongly on the field direction: for 
the intensity increases by a factor of 4.6 at a field of 6.6T, which corresponds to more than a doubling of the AFM moment, while the moment increases by only 10% for 
at 5T. This is in strong contrast to the inelastic response near the antiferromagnetic ordering vector, where no marked field variations are observed for up to 3.8T. The results reveal that the AFM state in CePtSi, which coexists with superconductivity, is distinctly different from other unconventional superconductors.
Si金子 耕士; Stockert, O.*; Skoulatos, M.*; Schneidewind, A.*; 竹内 徹也*; 松田 達磨; 芳賀 芳範; 摂待 力生*; 大貫 惇睦; 目時 直人
Journal of the Physical Society of Japan, 81(Suppl.B), p.SB006_1 - SB006_7, 2012/12
被引用回数：3 パーセンタイル：26.68(Physics, Multidisciplinary)The discovery of heavy-fermion superconductivity in non-centrosymmetric compound CePtSi, and subsequent findings of Ce
(T: transition metal, X: Si, Ge) bring a new essence in the condensed matter physics, since a novel type of superconducting properties is expected to come out. In CePtSi, the compound shows an antiferromagnetic (AFM) order at 
=2.2 K and enters into a heavy-fermion superconducting state below 
0.5 K. Through neutron scattering experiments under external magnetic field, we identified anomalous field response in CePtSi in the AFM state; AFM intensity showed enormous enhancement with increasing an applied field. The intensity kept increasing up to 7 T with the kink at around the additional phase boundary. These features suggest that the magnetic order in CePtSi is not a simple AFM one, and imply that large fraction of magnetic response could be still missing in this compound.
Si金子 耕士; Stockert, O.*; Arndt, J.*; Borth, R.*; Skoulatos, M.*; Habicht, K.*; Kiefer, K.*; Schneidewind, A.*; Etzdorf, D.*; 竹内 徹也*; et al.
no journal, ,
The heavy-fermion superconductivity in CePtSi with a non-centrosymmetric structure attracts a lot of attention since novel superconducting properties are expected under this symmetry. Another characteristics of the superconductivity in CePtSi is its coexistence with long-range antiferromagnetic order. Therefore detailed antiferromagnetic properties and its interplay with superconductivity are of strong interest to investigate. The magnetic structure of CePtSi is represented by 
=(0,0,1/2). We have observed that the 0 0 1/2 antiferromagnetic reflection exhibits a peculiar response to an external magnetic field; its intensity increases with magnetic fields. These results imply unusual antiferromagnetism in CePtSi.
Si金子 耕士; Stockert, O.*; Arndt, J.*; Borth, R.*; Skoulatos, M.*; Habicht, K.*; Kiefer, K.*; Schneidewind, A.*; Etzdorf, D.*; 竹内 徹也*; et al.
no journal, ,
The heavy-fermion superconductivity in CePtSi with a non-centrosymmetric structure attracts a lot of attention since novel superconducting properties are expected under this symmetry. Another characteristics of the superconductivity in CePtSi is its coexistence with long-range antiferromagnetic order. Therefore detailed antiferromagnetic properties and its interplay with superconductivity are of strong interest to investigate. The magnetic structure of CePtSi is represented by 
=(0,0,1/2). We have observed that the 0 0 1/2 antiferromagnetic reflection exhibits a peculiar response to an external magnetic field; its intensity increases with magnetic fields. These results imply unusual antiferromagnetism in CePtSi.
Si金子 耕士; Stockert, O.*; Skoulatos, M.*; Schneidewind, A.*; 竹内 徹也*; 松田 達磨; 芳賀 芳範; 摂待 力生*; 大貫 惇睦; 目時 直人
no journal, ,
CePtSi without inversion symmetry exhibits an antiferromagnetic (AFM) order at 2.2 K and enters into a heavy-fermion superconducting state below 0.5 K. Additional anomalies inside the AFM state were found under external magnetic fields in the vicinity of the upper critical field of the superconducting state. Our neutron scattering experiments under magnetic fields revealed that the application of the magnetic fields leads to an enormous enhancement in the AFM peak intensity in CePtSi, opposite to what is observed in usual antiferromagnets. We have clarified that the reported anomaly under the magnetic fields corresponds to inflection points in the field variation of the AFM intensity. The observed huge increase in AFM intensity corresponds to an increase of the ordered moment under the magnetic fields. These results imply an existence of a missing magnetic response in the ground state, which might be related to the formation of the superconducting state in CePtSi.
Si金子 耕士; Stockert, O.*; Skoulatos, M.*; Schneidewind, A.*; 竹内 徹也*; 松田 達磨; 芳賀 芳範; 摂待 力生*; 大貫 惇睦; 目時 直人
no journal, ,
The discovery of heavy-fermion superconductivity in non-centrosymmetric compound CePtSi brings a new essence in the field of condensed matter physics, since a novel type of superconducting properties are expected to emerge. CePtSi shows an antiferromagnetic (AFM) order at 
=2.2 K and enters into a heavy-fermion superconducting state below 
0.5 K. We identified anomalous external magnetic field response in CePtSi by neutron scattering experiments in the AFM state. An observed huge increase in AFM intensity corresponds to an increase of the staggered moment under uniform field, opposite of what is observed in ordinary antiferromagnets. These features suggest that the magnetic order in CePtSi is not a simple AFM one, and imply that large fraction of magnetic response could be still missing in this compound.
