Exact solution of the mixed spin-1/2 and spin-S Ising-Heisenberg diamond chain
The geometric frustration in a class of the mixed spin-1/2 and spin-S Ising-Heisenberg diamond chains is investigated by combining three exact analytical techniques: Kambe projection method, decoration-iteration transformation and transfer-matrix method. The ground state, the magnetization process...
Збережено в:
Дата: | 2009 |
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Автори: | , , |
Формат: | Стаття |
Мова: | English |
Опубліковано: |
Інститут фізики конденсованих систем НАН України
2009
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Назва видання: | Condensed Matter Physics |
Онлайн доступ: | http://dspace.nbuv.gov.ua/handle/123456789/120001 |
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Назва журналу: | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
Цитувати: | Exact solution of the mixed spin-1/2 and spin-S Ising-Heisenberg diamond chain / L. Čanová, J. Strečka, T. Lučivjanský // Condensed Matter Physics. — 2009. — Т. 12, № 3. — С. 353-368. — Бібліогр.: 56 назв. — англ. |
Репозитарії
Digital Library of Periodicals of National Academy of Sciences of UkraineРезюме: | The geometric frustration in a class of the mixed spin-1/2 and spin-S Ising-Heisenberg diamond chains is
investigated by combining three exact analytical techniques: Kambe projection method, decoration-iteration
transformation and transfer-matrix method. The ground state, the magnetization process and the specific heat
as a function of the external magnetic field are particularly examined for different strengths of the geometric
frustration. It is shown that the increase of the Heisenberg spin value S raises the number of intermediate
magnetization plateaux, which emerge in magnetization curves provided that the ground state is highly degenerate
on behalf of a sufficiently strong geometric frustration. On the other hand, all intermediate magnetization
plateaux merge into a linear magnetization versus magnetic field dependence in the limit of classical Heisenberg
spin S → ∞. The enhanced magnetocaloric effect with cooling rate exceeding the one of paramagnetic
salts is also detected when the disordered frustrated phase constitutes the ground state and the external
magnetic field is small enough. |
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