Commensurate-Incommensurate Charge-Density Wave Phase Transition in One-Dimensional Electron-Phonon System. II
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概要
- 論文の詳細を見る
The Commensurate-Incommensurate (C-IC) phase transition at finite temperature is considered in mean-field approximation taking account of higher harmonics. The phase diagram is given in the (μ, T)-plane, where μ represents a measure of the deviation from l/3 filledness. It is shown that at proper values of μ successive phase transitions occur (a) from the normal (N) to the IC-phase, (b) from the IC- to the C-phase and (c) from the C- to the IC-phase as T is decreased to zero. The transition (b) is caused by the growth of the amplitude of the order parameter, whereas the transition (c) is due to the increase of the chemical potential.
- 理論物理学刊行会の論文
- 1978-02-25
著者
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YAMAMOTO Hikaru
Department of Molecular and Pharmacological Neuroscience, Graduate School of Biomedical Sciences, Hi
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Yamamoto Hikaru
Depart Of Physics Kyoto University
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OHMI Tetsuo
Department of Physics, Graduate School of Science, Kyoto University
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Ohmi Tetsuo
Depart Of Physics Kyoto University
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NAKAYAMA Isao
Depart of Physics, Kyoto University
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Nakayama Isao
Depart Of Physics Kyoto University
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Nakayama Isao
Department Of Physics Faculty Of Science Kyoto University
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YAMAMOTO Hikaru
Depart of Physics, Kyoto University
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NAKAYAMA Isao
Department of Physics, Kyoto University
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