Template Synthesis, Structure, and Magnetic Properties of Layered Nanowires
- Autores: Zagorskii D.L.1,2, Doludenko I.M.1, Cherkasov D.A.1, Zhigalina O.M.1,3, Khmelenin D.N.1, Ivanov I.M.1,3, Bukharaev A.A.4, Bizyaev D.A.4, Khaibullin R.I.4, Shatalov S.A.1
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Afiliações:
- Shubnikov Institute of Crystallography, Russian Academy of Sciences
- Gubkin Russian State University of Oil and Gas
- Bauman Moscow State Technical University
- Zavoisky Physical-Technical Institute, Kazan, Federal Research Center Kazan Scientific Center, Russian Academy of Sciences
- Edição: Volume 61, Nº 9 (2019)
- Páginas: 1634-1645
- Seção: Magnetism
- URL: https://ogarev-online.ru/1063-7834/article/view/206163
- DOI: https://doi.org/10.1134/S1063783419090282
- ID: 206163
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Resumo
Nanowires (NWs) consisting of Ni/Cu and Co/Cu alternating layers with a diameter of 100 nm and layer thicknesses varying between 10 and 500 nm are prepared by template synthesis in pores of polymer track-etched membranes. Bath compositions and different regimes for pulsed electrodeposition of NWs are explored. A procedure for electrodeposition of NWs using pulses of equal charge is developed. By diminishing the amount of charge per pulse, initially we manage to lower the layer thickness to 10–15 nm, but further diminishing of charge in pulses leads to the blending of elemental composition of adjacent layers and/or formation of rod–shell nanostructures within the NWs. The coercive force (15–30 mT) and residual magnetization of our layered NWs are determined from magnetization measurements. For NWs with a layer thickness of 50–100 nm, the magnetization curves recorded in the out-of-plane and in-plane geometries are similar in shape and have similar parameters. For NWs with thicker layers (250 and 500 nm), magnetization curves are markedly different due to magnetic anisotropy (an easy magnetization axis emerges longitudinally to NWs) and interference between neighboring NWs. Magnetic force microscopy of isolated NWs identifies that the NWs comprise magnetic regions extending over ~100–150 nm. The NW can be partially remagnetized by applying an external magnetic field (+16 mT) longitudinally.
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Sobre autores
D. Zagorskii
Shubnikov Institute of Crystallography, Russian Academy of Sciences; Gubkin Russian State University of Oil and Gas
Autor responsável pela correspondência
Email: dzagorskiy@gmail.com
Rússia, Moscow; Moscow
I. Doludenko
Shubnikov Institute of Crystallography, Russian Academy of Sciences
Email: dzagorskiy@gmail.com
Rússia, Moscow
D. Cherkasov
Shubnikov Institute of Crystallography, Russian Academy of Sciences
Email: dzagorskiy@gmail.com
Rússia, Moscow
O. Zhigalina
Shubnikov Institute of Crystallography, Russian Academy of Sciences; Bauman Moscow State Technical University
Email: dzagorskiy@gmail.com
Rússia, Moscow; Moscow
D. Khmelenin
Shubnikov Institute of Crystallography, Russian Academy of Sciences
Email: dzagorskiy@gmail.com
Rússia, Moscow
I. Ivanov
Shubnikov Institute of Crystallography, Russian Academy of Sciences; Bauman Moscow State Technical University
Email: dzagorskiy@gmail.com
Rússia, Moscow; Moscow
A. Bukharaev
Zavoisky Physical-Technical Institute, Kazan, Federal Research Center Kazan Scientific Center,Russian Academy of Sciences
Email: dzagorskiy@gmail.com
Rússia, Kazan
D. Bizyaev
Zavoisky Physical-Technical Institute, Kazan, Federal Research Center Kazan Scientific Center,Russian Academy of Sciences
Email: dzagorskiy@gmail.com
Rússia, Kazan
R. Khaibullin
Zavoisky Physical-Technical Institute, Kazan, Federal Research Center Kazan Scientific Center,Russian Academy of Sciences
Email: dzagorskiy@gmail.com
Rússia, Kazan
S. Shatalov
Shubnikov Institute of Crystallography, Russian Academy of Sciences
Email: dzagorskiy@gmail.com
Rússia, Moscow
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