Theory of Anomalous Hall Effect in Heavy Fermion System
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概要
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The theory of the anomalous Hall effect in the heavy fermion system in the coherent regime is developed on the basis of the periodic Anderson Hamiltonian with de-generate orbitals. The anomalous Hall conductivity arises from the skew-scattering due to the orbital momenta of f-electrons in the presence of magnetic field. By a newly developed analysis based on the phase factor of the f-electron wavefunction in x-y plane, a simple expression for the Hall conductivity σ_<xy> is derived. It makes possible to understand clearly the mechanism and to estimate the sign and the magnitude of the anomalous Hall coefficient. Our theory explains well experimental results in the heavy fermion systems. Finally, we discuss the extension of this theory to explain the temperature dependence of the Hall coefficient in the cuprate high-T_c superconductors.
- 社団法人日本物理学会の論文
- 1994-07-15
著者
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YAMADA Kosaku
Department of Physics, Kyoto University
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Yamada Kosaku
Department Of Mechanical Engineering Faculty Of Engineering Kagoshima University
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KONTANI Hiroshi
Department of Physics, Nagoya University
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Kontani Hiroshi
Department Of Physics Faculty Of Science Kyoto University
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Kontani Hiroshi
Department Of Physcis Kyoto University
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