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(S)TEM/EELS characterization of phase and structural state in Fe

88

Zr

10

N

11

ferromagnetic films

O.M. Zhigalina1, D.N. Khmelenin1, E.N. Sheftel2, G.Sh. Usmanova2 and A. Carlsson3 1. Institute of Crystallography, Russian Academy of Sciences, 119333, Moscow, Russia

2. Baikov Institute of Metallurgy and Materials Science, Russian Academy of Sciences, 119333, Moscow, Russia

3. FEI Company, P.O. Box 80066, 5600 KA Eindhoven, The Netherlands zhigal@ns.crys.ras.ru

Keywords: films, ferromagnetic, diffraction pattern, phases

A new generation of magnetic films with required complex of properties determines in great extent a success in the development of the modern microelectronics. In this connection an attention of the researches is focused on investigations of nanocrystalline magnetic soft films based on Fe-Me-X system (X=B, C, N, O и Me=Ti, Zr, Hf, Nb, Ta) with unique combinations of properties, such as high saturation induction (up to 2T), low coercive field (<0.1 Oe), high thermal stability. [1].

In this work we report about a structural characterization of Fe88Zr10N11 ferromagnetic films fabricated by a reactive rf magnetron sputtering technique on heat resistant glass substrates and annealed at temperatures in the range of T=200-6500 C at residual pressure of 3× 10-6Torr. The films have a thickness of about 1-2 µm.

Cross sections for (S)TEM and HREM investigations were prepared by ion milling in Gatan PIPs 691. All samples were characterized in a Tecnai G2 30ST at accelerating voltage of 300kV. EELS-mapping was carried out in a Tecnai F20 XTwin equipped with a Gatan Tridium 863 GIF and high-angle-annular dark-field (HAADF) STEM detector. The probe size used for the experiment was 1 nm. The images and SAED patterns were processed and analyzed with the Gatan Digital Micrograph 3.11.1 software and JEMS package [2].

Nitrogen-oversaturated α –Fe phase with sizes in the range of 2-5 nm was observed in the structure of as-sputtered films, fig.1. ZrN-crystals appeared after annealing at the T=2000C. Such kind of structural state remained stable till temperature of annealing of T=6000C. At high temperatures of heat treatment we observed nanocrystals of α –Fe, γ –Fe (for some films), ZrN and perhaps both Fe2N and Zr1Ox-1 in accordance with SAED patterns, DF TEM and HREM images, fig.2. α –Fe and ZrN phases exhibited a texture.

Nanocrystalline conglomerates formed column structures (white arrows, fig.2) grown out of substrate.

EELS-mapping of the film annealed at T=6000C demonstrated compositional heterogeneity in the film-substrate interface, fig.3: Zr-atoms diffused inside of substrate, while Fe-atoms gathered on the interface regions. The film was impoverished by nitrogen in comparison with the substrate in the region of interface. Correlation of the compositional heterogeneity both zirconium and oxygen was observed.

In this connection we can suggest that Fe2N-phase formed as a result of decreasing of the N-content in the α –Fe crystals at high temperature of annealing; Zr1O1-x phase formed as a result of interaction with substrate that could become the reason of occurrence of γ –Fe phase with the same interplanar spacings.

1. E.N. Sheftel, E.E. Shalygina, G.Sh. Usmanova, S.I. Utitskikh, M.A. Mukasheva, M. Inoue, R. Fujikawa, Tech. Phys. Lett. 33 (2007) p881.

M6.P390 - 457 - MC2009

W. Grogger, F. Hofer, P. Pölt (Eds.): MC2009, Vol. 3: Materials Science, DOI: 10.3217/978-3-85125-062-6-601 , © Verlag der TU Graz 2009

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2. P. Stadelmann, JEMS. http://cime.www.epfl.chl.2008.

3. The work was supported by the State Program for Support of Leading Scientific schools, project № NSh-1955.2008.2. We kindly acknowledge SMA and FEI

Companies for organization of the opportunity to study the films structure by EELS.

Figure 1. Structure of as-sputtered film: DF TEM image and the corresponding electron diffraction pattern (SAED) with calculated pattern.

Figure 2. Structure of the film annealed at T=6500C: DF TEM image and the corresponding electron diffraction pattern (SAED).

Figure 3. EELS-mapping for the film annealed at T=6000C.

MC2009 - 458 - M6.P390

W. Grogger, F. Hofer, P. Pölt (Eds.): MC2009, Vol. 3: Materials Science, DOI: 10.3217/978-3-85125-062-6-601 , © Verlag der TU Graz 2009

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