TY - JOUR
T1 - Low temperature magnetic properties of Ce3Pd20Si 6
AU - Mitamura, Hiroyuki
AU - Tayama, Takashi
AU - Sakakibara, Toshiro
AU - Tsuduku, Seiji
AU - Ano, Genki
AU - Ishii, Isao
AU - Akatsu, Mitsuhiro
AU - Nemoto, Yuichi
AU - Goto, Terutaka
AU - Kikkawa, Akiko
AU - Kitazawa, Hideaki
PY - 2010/7
Y1 - 2010/7
N2 - Magnetization of a single crystalline Ce3Pd20Si 6 was measured at low temperatures down to 90mK in fields up to 11 T for the three principal directions [100], [110], and [111]. For all directions, two transitions were observed in the temperature variation of the magnetization M(T) at 0.2 T; a broad peak at 0.28K associated with a phase-III transition, and an upward bending at ∼0:5K due to a phase-II ordering from the paramagnetic state (phase-I). The latter critical temperature TI-II is found to be strongly enhanced in magnetic fields B, depending on the field direction, and TI-II(B) becomes highly anisotropic. These results suggest that phase-II is an antiferroquadrupole state originated from a Γ8 ground state. By contrast, no appreciable anisotropy is found in the phase-III state. At 90 mK, phase-III collapses by applying a field of ∼0:63 T for all directions. Above this field, the magnetization curve M(B) becomes strongly anisotropic. The magnetization value per Ce in the phase-I region at 90mK is apparently smaller than the Γ8 moment, indicating that either 8c or 4a site has a Γ7 ground state.
AB - Magnetization of a single crystalline Ce3Pd20Si 6 was measured at low temperatures down to 90mK in fields up to 11 T for the three principal directions [100], [110], and [111]. For all directions, two transitions were observed in the temperature variation of the magnetization M(T) at 0.2 T; a broad peak at 0.28K associated with a phase-III transition, and an upward bending at ∼0:5K due to a phase-II ordering from the paramagnetic state (phase-I). The latter critical temperature TI-II is found to be strongly enhanced in magnetic fields B, depending on the field direction, and TI-II(B) becomes highly anisotropic. These results suggest that phase-II is an antiferroquadrupole state originated from a Γ8 ground state. By contrast, no appreciable anisotropy is found in the phase-III state. At 90 mK, phase-III collapses by applying a field of ∼0:63 T for all directions. Above this field, the magnetization curve M(B) becomes strongly anisotropic. The magnetization value per Ce in the phase-I region at 90mK is apparently smaller than the Γ8 moment, indicating that either 8c or 4a site has a Γ7 ground state.
KW - Antiferroquadrupole transition
KW - CePdSi
KW - Magnetic phase diagram
KW - Magnetization
UR - http://www.scopus.com/inward/record.url?scp=77956245725&partnerID=8YFLogxK
U2 - 10.1143/JPSJ.79.074712
DO - 10.1143/JPSJ.79.074712
M3 - 学術論文
AN - SCOPUS:77956245725
SN - 0031-9015
VL - 79
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 7
M1 - 074712
ER -