Pressure effects on electronic structure and magnetic properties of anisotropic metallic compounds

Pressure effects on electronic structure and magnetic properties of anisotropic metallic materials (CrB₂, FeGe₂, LaFeAsO) are investigated. Magnetic susceptibilities of CrB₂ and FeGe₂ compounds were studied under hydrostatic pressure at fixed temperatures, 77 and 300 K. In order to analyze the exper...

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Збережено в:
Бібліографічні деталі
Дата:2008
Автори: Grechnev, G.E., Panfilov, A.S., Fedorchenko, A.V., Svechkarev, I.V., FIlippov, V.B., Lyashchenko, A.B., Vasiliev, A.N.
Формат: Стаття
Мова:English
Опубліковано: Донецький фізико-технічний інститут ім. О.О. Галкіна НАН України 2008
Назва видання:Физика и техника высоких давлений
Онлайн доступ:http://dspace.nbuv.gov.ua/handle/123456789/70464
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Назва журналу:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Цитувати:Pressure effects on electronic structure and magnetic properties of anisotropic metallic compounds / G.E. Grechnev, A.S. Panfilov, A.V. Fedorchenko, I.V. Svechkarev, V.B. Filippov, A.B. Lyashchenko, A.N. Vasiliev // Физика и техника высоких давлений. — 2008. — Т. 18, № 4. — С. 112-118. — Бібліогр.: 19 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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Резюме:Pressure effects on electronic structure and magnetic properties of anisotropic metallic materials (CrB₂, FeGe₂, LaFeAsO) are investigated. Magnetic susceptibilities of CrB₂ and FeGe₂ compounds were studied under hydrostatic pressure at fixed temperatures, 77 and 300 K. In order to analyze the experimental magnetovolume effects, the electronic structures were calculated ab initio in external magnetic field as a function of atomic volume by employing a full-potential LMTO method. The calculated field-induced magnetic moments and their volume derivatives compare favorably with the experimental pressure effects in magnetic properties of CrB₂ and FeGe₂. The main role of pressure in high-Tc superconductivity of LaFeAsO is found to reduce density of states at the Fermi level and to suppress ferromagnetic spin fluctuations.