Fermi Liquid Theory on the Basis of the Periodic Anderson Model with Spin-Orbit Coupling and Crystalline Field : General and Mathematical Physics
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概要
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In order to discuss the normal-state properties of heavy-fermion systems, the Fermi liquid theory is developed on the basis of the periodic Anderson model with arbitrary spin-orbit coupling and crystalline field. For the unperturbed (U=0) case, the electronic band structure is determined; then the expressions of T-linear coefficient of specific heat and magnetic susceptibility are derived. For U≠0, the general expression for T-linear coefficient of specific heat and magnetization are derived. However, the expression for magnetic susceptibility cannot generally be brought into such a usual form that includes only the quantities on the Fermi surface because of the existence of off-diagonal elements of f-electron self-energy. Therefore, the susceptibility is calculated in the special case that only the lowest Kramers doublet is taken into account.
- 理論物理学刊行会の論文
- 1989-05-25
著者
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Yamada Kosaku
Department Of Mechanical Engineering Faculty Of Engineering Kagoshima University
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Hanzawa Katsurou
Department Of Physics Faculty Of Science And Technology Science University Of Tokyo
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Yosida Kei
Department Of Physics Faculty Of Science And Technology Science University Of Tokyo
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Yosida Kei
The Institute For Solid State Physics The University Of Tokyo
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Yoshida Kei
Department Of Science And Technology Science University Of Tokyo
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Yoshida Kei
Department Of Physics University Of Tokyo
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Yoshida Kei
Department Of Orthopedic Surgery Niigata University School Of Medicine
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Hanzawa Katsurou
Department Of Physics University Of Tokyo
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YOSIDA Kei
Department of Physics, Faculty of Science and Technology Science University of Tokyo
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YOSHIDA Kei
Department of Physics, University of Tokyo
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YOSHIDA Kei
The Institute of Solid State Physics, The University of Tokyo
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HANZAWA Katsurou
Department of Physics, University of Tokyo
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