Magnetic Microstructure Aluminum-substituted Barium Hexaferrite for Microwave Devices mm-Wavelength Range

Authors	M.N. Shipko¹^,² , V.V. Korovushkin¹ , V.G. Kostishyn¹ , N.D. Ursulyak³, A.G. Nalogin³ , E.S. Savtchenko¹
Affiliations	¹ National University of Science and Technology "MISiS", 4, Leninsky Prosp., 119049 Moscow, Russia ² Ivanovo Branch «Plekhanov Russian University of Economics», 53, Dzerzhinskogo St., 153025 Ivanovo, Russia ³ JSC “RPC “ISTOK” named after Shokin”, 2A, Vokzalnaya St., 141190 Fryazino, Moscow region, Russia
Е-mail	drvgkostishyn@mail.ru
Issue	Volume 7, Year 2015, Number 4
Dates	Received 01 October 2015; published online 24 December 2015
Citation	M.N. Shipko, V.V. Korovushkin, V.G. Kostishyn, et al., J. Nano- Electron. Phys. 7 No 4, 04075 (2015)
DOI
PACS Number(s)	75.50.Gg, 75.75. + a
Keywords	Hexaferrite (6) , Magnetic microstructure, Cationic distribution (2) , Microwave (8) , Crystal structure (8) .
Annotation	The magnetic structure and cationic distribution was investigate in ferrite with a hexagonal structure BaFe12 – хAlхO12 (х ≤ 2). It is found that when х = 2 Al3+ ions are localized mainly in the positions of 12k (а-sublattice) and 4f1 (с-sublattice). This contribute to change of number magnetically active connections and therefore the magnetic structure of ferrite and magnetic parameters. It was concluded about the possibility of using the results obtained with the choice of optimal composition of substrates for millimeter-wave devices.
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