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Heavy fermion state and quantum criticality

重い電子状態と量子臨界性

大貫 惇睦; 摂待 力生*; 本多 史憲*; Dung, N. D.*; 石倉 達朗*; 竹内 徹也*; 松田 達磨; 立岩 尚之; 中村 彰夫; 山本 悦嗣; 芳賀 芳範; 青木 大*; 本間 佳哉*; 播磨 尚朝*; 山上 浩志*

Onuki, Yoshichika; Settai, Rikio*; Honda, Fuminori*; Dung, N. D.*; Ishikura, Tatsuro*; Takeuchi, Tetsuya*; Matsuda, Tatsuma; Tateiwa, Naoyuki; Nakamura, Akio; Yamamoto, Etsuji; Haga, Yoshinori; Aoki, Dai*; Homma, Yoshiya*; Harima, Hisatomo*; Yamagami, Hiroshi*

The heavy fermion state in the f-electron systems is due to competition between the RKKY interaction and the Kondo effect. To understand the electronic state, we studied the Fermi surface properties via the de Haas-van Alphen (dHvA) experiments and energy band calculations for CeSn$$_{3}$$, CeRu$$_{2}$$Si$$_{2}$$, UPt$$_{3}$$, and nowadays, transuranium compounds of NpGe$$_{3}$$ and PuIn$$_{3}$$, together with YbCu$$_{2}$$Si$$_{2}$$.

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パーセンタイル:92.59

分野:Physics, Condensed Matter

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