Characteristic heavy fermion properties in YbCu
Si
and YbT
Zn
(T: Co, Rh, Ir)
YbCu
Si
とYbT
Zn
(T: Co, Rh, Ir)の重い電子系特性
大貫 惇睦; 安井 慎一*; 松下 昌輝*; 吉内 伸吾*; 大家 政洋*; 広瀬 雄介*; Dung, N. D.*; 本多 史憲*; 竹内 徹也*; 摂待 力生*; 杉山 清寛*; 山本 悦嗣
; 松田 達磨; 芳賀 芳範
; 田中 斗志貴*; 久保 康則*; 播磨 尚朝*
Onuki, Yoshichika; Yasui, Shinichi*; Matsushita, Masaki*; Yoshiuchi, Shingo*; Oya, Masahiro*; Hirose, Yusuke*; Dung, N. D.*; Honda, Fuminori*; Takeuchi, Tetsuya*; Settai, Rikio*; Sugiyama, Kiyohiro*; Yamamoto, Etsuji; Matsuda, Tatsuma; Haga, Yoshinori; Tanaka, Toshiki*; Kubo, Yasunori*; Harima, Hisatomo*
We studied the Fermi surface properties of YbCu
Si
and YbCu
Ge
with the tetragonal structure by measuring the de Haas-van Alphen (dHvA) oscillations, together with the energy band calculations. It was clarified that 4f electrons contribute to the Fermi surface of a valence fluctuating compound YbCu
Si
, but not to that of a divalent compound YbCu
Ge
. We also studied the heavy fermion properties of YbT
Zn
(T: Co, Rh, Ir) with the cubic caged structure. The metamagnetic behavior or an abrupt nonlinear increase of magnetization was observed. By measuring the electrical resistivity under pressure and magnetic field, we clarified that the electronic state close to the quantum critical point is realized in YbIr
Zn
at 5.2 GPa and also YbCo
Zn
at ambient pressure.