Sd-model with strong exchange coupling and a metal-insulator phase transition
Sd-exchange model (Kondo lattice model) is formulated for strong sd-coupling within the framework of the Xoperators technique and the generating functional approach. The X-operators are constructed based on the exact eigen functions of a single-site sd-exchange Hamiltonian. Such representation ena...
Збережено в:
Дата: | 2006 |
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Автори: | , , |
Формат: | Стаття |
Мова: | English |
Опубліковано: |
Інститут фізики конденсованих систем НАН України
2006
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Назва видання: | Condensed Matter Physics |
Онлайн доступ: | http://dspace.nbuv.gov.ua/handle/123456789/121358 |
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Назва журналу: | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
Цитувати: | Sd-model with strong exchange coupling and a metal-insulator phase transition / Yu.A. Izyumov, N.I. Chaschin, D.S. Alexeev // Condensed Matter Physics. — 2006. — Т. 9, № 3(47). — С. 545–555. — Бібліогр.: 9 назв. — англ. |
Репозитарії
Digital Library of Periodicals of National Academy of Sciences of UkraineРезюме: | Sd-exchange model (Kondo lattice model) is formulated for strong sd-coupling within the framework of the Xoperators
technique and the generating functional approach. The X-operators are constructed based on the
exact eigen functions of a single-site sd-exchange Hamiltonian. Such representation enables us to develop a
perturbation theory near the atomic level. A locator-type representation was derived for the electron Green’s
function. The electron self-energy includes interaction of electrons and spin fluctuations. An integral equation
for the self-energy was obtained in the limit of infinite localized spins. A solution of this equation in the static
approximation for spin fluctuations leads to a structure of electron Green’s function showing a metal-insulator
phase transition. This transition is similar to that in the Hubbard model at half filling. |
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