Tailoring magnetic anisotropy at the ferromagnetic/ferroelectric interface
Appl. Phys. Lett. 92, 122905 (2008); doi:10.1063/1.2901879
Published 26 March 2008
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It is predicted that magnetic anisotropy of a thin magnetic film may be affected by the polarization of a ferroelectric material. Using a Fe/BaTiO3 bilayer as a representative model and performing first-principles calculations, we demonstrate that a reversal of the electric polarization of BaTiO3 produces a sizable change in magnetic anisotropy energy of Fe films. Tailoring the magnetic anisotropy of a nanomagnet by an adjacent ferroelectric material may yield entirely new device concepts, such as electric-field controlled magnetic data storage.
©2008 American Institute of Physics
| History: | Received 28 December 2007; accepted 4 March 2008; published 26 March 2008 |
| Permalink: |
http://link.aip.org/link/?APPLAB/92/122905/1 |
KEYWORDS and PACS
ab initio calculations,
barium compounds,
dielectric polarisation,
ferroelectric thin films,
ferromagnetic materials,
iron,
magnetic anisotropy,
magnetic multilayers,
magnetic thin films,
nanostructured materials
- 75.30.Gw
Magnetic anisotropy - 77.55.+f
Dielectric thin films - 77.80.-e
Ferroelectricity and antiferroelectricity - 77.84.Dy
Dielectric, piezoelectric, and ferroelectric niobates, titanates, tantalates, PZT ceramics, etc - 75.70.Cn
Magnetic properties of interfaces - 77.22.Ej
Dielectric polarization and depolarization - YEAR: 2008
RELATED DATABASES
PUBLICATION DATA
0003-6951 (print)
1077-3118 (online)
REFERENCES (31)
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- S. D. Bader, Rev. Mod. Phys. 78, 1 (2006).
- J. H. Van Vleck, Phys. Rev. 52, 1178 (1937).
- L. Néel,
J. Phys. Radium 15, 225 (1954) . - U. Gradmann, Handbook of Magnetic Materials, edited by K. H. J. Buschow (North-Holland-Elsevier, Amsterdam, 1993), Vol. 7.
- P. Gambardella, S. Rusponi, M. Veronese, S. S. Dhesi, C. Grazioli, A. Dallmeyer, I. Cabria, R. Zeller, P. H. Dederichs, K. Kern, C. Carbone, and H. Brune,
Science 300, 1130 (2003) . - G. Andersson, T. Burkert, P. Warnicke, M. Björck, B. Sanyal, C. Chacon, C. Zlotea, L. Nordström, P. Nordblad, and O. Ericksson, Phys. Rev. Lett. 96, 037205 (2006).
- D. Weller and T. McDaniel, Advanced Magnetic Nanostructures, edited by D. J. Sellmyer and R. Skomski (Springer, Berlin, 2006), Chap. 11.
- T. W. McDaniel,
J. Phys.: Condens. Matter 17, R315 (2005) . - R. H. Victora and X. Shen,
IEEE Trans. Magn. 41, 537 (2005) . - D. Suess, T. Schrefl, S. Fahler, M. Kirschner, G. Hrkac, F. Dorfbauer, and J. Fidler, Appl. Phys. Lett. 87, 012504 (2005).
- M. Fiebig,
J. Phys. D 38, R123 (2005) . - W. Eerenstein, N. D. Mathur, and J. F. Scott,
Nature (London) 442, 759 (2006) . - R. Ramesh and N. A. Spaldin,
Nat. Mater. 6, 21 (2007) . - C.-G. Duan, S. S. Jaswal, and E. Y. Tsymbal, Phys. Rev. Lett. 97, 047201 (2006).
- E. Y. Tsymbal and H. Kohlstedt,
Science 313, 181 (2006) . - J. P. Velev, C.-G. Duan, K. D. Belashchenko, S. S. Jaswal, and E. Y. Tsymbal, Phys. Rev. Lett. 98, 137201 (2007).
- M. Gajek, M. Bibes, S. Fusil, K. Bouzehouane, J. Fontcuberta, A. Barthélémy, and A. Fert,
Nat. Mater. 6, 296 (2007) . - M. Weisheit, S. Fähler, A. Marty, Y. Souche, C. Poinsignon, and D. Givord,
Science 315, 349 (2007) . - T. Zhao, A. Scholl, F. Zavaliche, K. Lee, M. Barry, A. Doran, M. P. Cruz, Y. H. Chu, C. Ederer, N. A. Spaldin, R. R. Das, D. M. Kin, S. H. Baek, C. B. Eom, and R. Ramesh,
Nat. Mater. 5, 823 (2006) . - F. Zavaliche, T. Zhao, H. Zheng, F. Straub, M. P. Cruz, P.-L. Yang, D. Hao, and R. Ramesh,
Nano Lett. 7, 1586 (2007) . - S. Sahoo, S. Polisetty, C.-G. Duan, S. S. Jaswal, E. Y. Tsymbal, and C. Binek, Phys. Rev. B 76, 092108 (2007).
- G. Bihlmayer, Y. M. Koroteev, P. M. Echenique, E. V. Chulkov, and S. Blügel,
Surf. Sci. 600, 3888 (2006) . - G. H. O. Daalderop, P. J. Kelly, and M. F. H. Schuurmans, Phys. Rev. B 41, 11919 (1990).
- Total energy calculations are performed within density-functional theory using the projector augmented wave (PAW) method implemented in the Vienna Ab Initio Simulation Package (VASP) [G. Kresse and D. Joubert, Phys. Rev. B 59, 1758 (1999)]. The exchange-correlation potential is treated in the generalized gradient approximation. We use the energy cutoff of 500 eV for the plane wave expansion of the PAWs and a 12×12×1 Monkhorst–Pack grid for k-point sampling in the self-consistent calculations. The convergences of MAE calculation over both cutoff energy and k-point sampling have been tested. The final MAE results are obtained using 6400 k points in the whole Brillouin zone. All the structural relaxations are performed until the Hellman–Feynman forces on the relaxed atoms become less than 10 meV/Å.
- C.-G. Duan, R. F. Sabiryanov, W. N. Mei, S. S. Jaswal, and E. Y. Tsymbal,
Nano Lett. 6, 483 (2006) , and references therein. - D. S. Wang, R. Q. Wu, and A. J. Freeman, Phys. Rev. Lett. 70, 869 (1993).
- R. Q. Wu and A. J. Freeman,
J. Magn. Magn. Mater. 200, 498 (1999) . - P. Ravindran, A. Kjekshus, H. Fjellvåg, P. James, L. Nordström, B. Johansson, and O. Eriksson, Phys. Rev. B 63, 144409 (2001).
- G. van der Laan,
J. Phys.: Condens. Matter 10, 3239 (1998) . - P. Bruno, Phys. Rev. B 39, 865 (1989).
- C. Li and A. J. Freeman, Phys. Rev. B 43, 780 (1991).







