Manifestations of the electron orbital moment in high-frequency properties of ferroelectrics with 3d-ions
A phenomenological theory of high-frequency properties of ferroelectric and ferroelectric-ferromagnet with the 3d-ions has been elaborated based on the separate accounting for spin and orbital electron moments, electron and ion contributions to electric polarization. In the ferroelectric state, t...
Збережено в:
Дата: | 1999 |
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Автор: | |
Формат: | Стаття |
Мова: | English |
Опубліковано: |
Інститут фізики конденсованих систем НАН України
1999
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Назва видання: | Condensed Matter Physics |
Онлайн доступ: | http://dspace.nbuv.gov.ua/handle/123456789/121019 |
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Назва журналу: | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
Цитувати: | Manifestations of the electron orbital moment in high-frequency properties of ferroelectrics with 3d-ions / I.E. Chupis // Condensed Matter Physics. — 1999. — Т. 2, № 4(20). — С. 745-753. — Бібліогр.: 8 назв. — англ. |
Репозитарії
Digital Library of Periodicals of National Academy of Sciences of UkraineРезюме: | A phenomenological theory of high-frequency properties of ferroelectric
and ferroelectric-ferromagnet with the 3d-ions has been elaborated based
on the separate accounting for spin and orbital electron moments, electron
and ion contributions to electric polarization. In the ferroelectric state, the
existence of the electron orbital moment leads to the breaks in the temperature dependencies of the transverse components of dielectric susceptibility
at the ferroelectric transition temperature. The values of these breaks are
proportional to the square of the electron part of spontaneous polarization
and the parameter of freezing of the orbital moment. Similar breaks and
the decrease of the phonon frequencies in the ferroelectric state should
occur in the modes which are not soft. Besides, the effect of induction of
high-frequency orbital moment by electron part of electric polarization has
been predicted as well. This effect would lead to the break in the temperature dependence of paramagnetic susceptibility at ferroelectric transition
temperature. In the ferroelectromagnetic state, the electron orbital moment
also manifests itself in λ increase of magnetoelectric gyration ( λ is the
constant of spin-orbital interaction). |
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