Electronic phase diagram of strongly correlated electron system at T = 0 K, n = 2 Insulator diamagnetic : Electron chemical potential = Fermi level 2 electrons/atom T=0K s orbital Electronic phase diagram of strongly correlated electron system at T = 0 K, n = 1 : Electron chemical potential = Fermi level 1 electrons/atom T=0K s orbital 1 Material Science I. d electron systems Fujimori II. p electron systems Kanoda Transition elements 1st series: Incomplete 3d shell Lanthanides Actinides KEK home page 2 Transition elements 2nd series: Incomplete 4d shell Lanthanides Actinides KEK home page Transition elements 3rd series: Incomplete 5d shell Lanthanides Actinides KEK home page 3 Transition elements Shallow core levels Lanthanides Actinides Lanthanide series: Incomplete 4f shell KEK home page Transition elements Shallow core levels Lanthanides Actinides Actinide series: Incomplete 5f shell KEK home page 4 Material Science I. d Electron systems 1. Electronic structure of transition-metal ions (April 8) 2. 3. 4. 5. 6. Crystal structure and band structure (April 15) Mott insulators (April 22) Metal-insulator transition (May 13, May 20) High-temperature superconductivity (May 27) Spin-related phenomena (June 3) References 1. 藤森 淳「強相関物質の基礎 ― 原子,分子から固体へ」(内田老鶴圃, 2005年) 2. M. Imada, A. Fujimori, and Y. Tokura: Metal-Insulator Transitions, Review in Modern Physics 70, 1039 (1998) 3. 津田惟雄,那須圭一郎,藤森 淳,白鳥紀一「電気伝導性酸化物(改訂版)」 (裳華房,1993年) Lecture note 理・物理 藤森研ホームページ→講義→物質科学 http://wyvern.phys.s.u-tokyo.ac.jp/f/lecture/matscig/index.htm Fujimori group home Lectures Material Science http://wyvern.phys.s.u-tokyo.ac.jp/f/lecture/matscig/index_en.htm 公用でやむを得ず欠席する場合は,藤森までメールで連絡下さい。出席扱いにします。 If you are absent from a lecture due to an unavoidable schedule, please let Fujimori know by email. Your attendance will be marked. 5
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