Loading [MathJax]/jax/output/HTML-CSS/jax.js

Formation of the Ordered L10-FePt Phase in Fe50Pt50/Au/Fe50Pt50 Films at Annealing in Hydrogen

M. Yu. Verbytska1, M. N. Shamis1, P. V. Makushko1, Ya. A. Berezniak2, K. O. Grayvoronska2, T. I. Verbytska1, Yu. M. Makogon1, Yu. V. Kudryavtsev3

1National Technical University of Ukraine ‘Igor Sikorsky Kyiv Polytechnic Institute’, 37 Peremohy Ave., UA-03056 Kyiv, Ukraine
2I. M. Frantsevich Institute for Problems in Materials Science, NAS of Ukraine, 3 Academician Krzhyzhanovsky Str., UA-03142 Kyiv, Ukraine
3G. V. Kurdyumov Institute for Metal Physics, NAS of Ukraine, 36 Academician Vernadsky Blvd., UA-03142 Kyiv, Ukraine

Received: 31.01.2018. Download: PDF

Influence of the intermediate Au layer during annealing in hydrogen ambience on the hard magnetic, chemically ordered L10-FePt phase formation in film Fe50Pt50(15 nm)/Au(7.5 nm; 30 nm)/Fe50Pt50(15 nm) compositions deposited by the magnetron sputtering on SiO2(100 nm)/Si(001) substrate is investigated. The annealing of films is carried out in hydrogen ambience within the temperature range of 500–800°C for 30 s. The rates of heating and cooling are of 1°C/s. Before gas inflow, the chamber is pre-pumped out to a pressure of 0.1 Pa. The hydrogen pressure at annealing is of 101.3 kPa. The A1-FePt L10-FePt phase transition begins during annealing at 500°C in both films. The ordering degree of the L10-FePt phase, coercivity HC, and sizes of FePt grains are increased, when annealing temperature is elevated. During interdiffusion of the Au and FePt layers, gold does not participate in the ordering process of FePt. It is located in the intergranular area that limits the exchange interaction between the L10-FePt phase grains and additionally increases HC. Moreover, coercivity additionally rises with Au layer thickness increasing. Introduction of hydrogen atoms into the octahedral interstices of the L10-FePt crystal lattice leads to a decrease in the tetragonality degree by means of the increasing the lattice parameter c during annealing at temperature above 600°C. The penetration of hydrogen into the Au lattice leads to gold-hydride formation. The preferred (111) texture is formed in both Au and FePt layers.

Key words: thin film, chemically ordered L10-FePt phase, annealing, hydrogen, coercivity.

URL: http://mfint.imp.kiev.ua/en/abstract/v40/i08/1069.html

DOI: https://doi.org/10.15407/mfint.40.08.1069

PACS: 66.30.Pa, 68.55.-a, 75.50.Ss, 75.50.Vv, 75.70.Ak, 81.40.Ef, 81.40.Rs

Citation: M. Yu. Verbytska, M. N. Shamis, P. V. Makushko, Ya. A. Berezniak, K. O. Grayvoronska, T. I. Verbytska, Yu. M. Makogon, and Yu. V. Kudryavtsev, Formation of the Ordered L10-FePt Phase in Fe50Pt50/Au/Fe50Pt50 Films at Annealing in Hydrogen, Metallofiz. Noveishie Tekhnol., 40, No. 8: 1069—1079 (2018) (in Ukrainian)


REFERENCES
  1. M. H. Kryder, E. C. Gage, T. W. McDaniel, W. A. Challener, R. E. Rottmayer, G. Ju, Y.-T. Hsia, and M. F. Erden, Proc. IEEE, 96, Iss. 11: 1810 (2008). Crossref
  2. D. Weller, G. Parker, O. Mosendz, A. Lyberatos, D. Mitin, N. Y. Safonova, and M. Albrecht, J. Vac. Sci. Technol. B, 34: 060801 (2016). Crossref
  3. D. Weller, A. Moser, L. Folks, M. E. Best, Wen Lee, M. F. Toney, M. Schwickert, J.-U. Thiele, and M. F. Doerner, IEEE Trans. Magn., 36, Iss. 1: 10 (2000). Crossref
  4. C. L. Platt, K. W. Wierman, E. B. Svedberg, R. van de Veerdonk, J. K. Howard, A. G. Roy, and D. E. Laughlin, J. Appl. Phys., 92, Iss. 10: 6104 (2002). Crossref
  5. C. Y. You, Y. K. Takahashi, and K. Hono, J. Appl. Phys., 100, Iss. 5: 056105 (2006). Crossref
  6. Yu. M. Makogon, O. P. Pavlova, S. I. Sidorenko, T. I. Verbytska, M. Yu. Verbytska, and O. V. Fihurna, Metallofiz. Noveishie Tekhnol., 37, No. 4: 487 (2015). Crossref
  7. Yu. M. Makogon, O. P. Pavlova, S. I. Sidorenko, T. I. Verbyts'ka, M. Yu. Verbyts'ka, and O. V. Figurna, Metallofiz. Noveishie Tekhnol., 36, No. 11: 1513 (2014) (in Ukrainian). Crossref
  8. Iu. M. Makogon, E. P. Pavlova, S. I. Sidorenko, T. I. Verbytska, I. A. Vladymyrskyi, and R. A. Shkarban, Metallofiz. Noveishie Tekhnol., 35, No. 4: 553 (2013) (in Russian).
  9. T. Kamiki and S. Nagawa, J. Magn. Soc. Jpn., 28, Iss. 3: 330 (2004). Crossref
  10. S. Nakagawa and T. Kamiki, J. Magn. Magn. Mat., 287: 204 (2005). Crossref
  11. M. Yamauchi, K. Okubo, T. Tsukuda, K. Kato, M. Takatae, and S. Takedaf, Nanoscale, 6, Iss. 8: 4067 (2014). Crossref
  12. K. Barmak, J. Kim, L. H. Lewis, K. R. Coffey, M. F. Toney, A. J. Kellock, and J.-U. Thiele, J. Appl. Phys., 98: 033904 (2005). Crossref
  13. L. Liu, H. Lv, W. Sheng, Yu. Lou, J. Bai, J. Cao, B. Ma, and F. Wei, Appl. Surf. Sci., 258, Iss. 15: 5770 (2012). Crossref
  14. V. E. Antonov, T. E. Antonova, I. T. Belash, A. E. Gorodetskii, and E. G. Ponyatovskii, Dokl. Phys. Chem., 266, No. 2: 722 (1982).
  15. I. A. Vladymyrskyi, M. V. Karpets, F. Ganss, G. L. Katona, D. L. Beke, S. I. Sidorenko, T. Nagata, T. Nabatame, T. Chikyow, G. Beddies, M. Albrecht, and Iu. M. Makogon, J. Appl. Phys., 114, Iss. 16: 164314 (2013). Crossref