Journal of Applied Physics
Search:
   
 
 
 
Previous Article
Effect of substrate-induced strains on the spontaneous polarization of epitaxial BiFeO3 thin films
A single-domain thermodynamic theory is employed to predict the spontaneous polarizations of (001)c, (101)c, and (111)c oriented epitaxial BiFeO3 thin films grown on dissimilar substrates. The effects...
Next Article
Phases and domain structures in tungsten-doped Pb(Mg1/3Nb2/3)1−xTixO3 (x=0.35) crystal
Dielectric permittivity, electric polarization, and domain structure have been carried out as a function of temperature in 0.5 mol % WO3-doped Pb(Mg1/3Nb2/3)0.65Ti0.35O3 (PMNT35%) single crystal. Two ...

Polarization and lattice strains in epitaxial BaTiO3 films grown by high-pressure sputtering

J. Appl. Phys. 101, 114106 (2007); doi:10.1063/1.2745277

Published 14 June 2007

You are not logged in to this journal. Log in

A. Petraru, N. A. Pertsev, H. Kohlstedt, U. Poppe, and R. Waser
Institut für Festkörperforschung and CNI, Forschungszentrum Jülich, D-52425 Jülich, Germany

A. Solbach and U. Klemradt
II. Physikalisches Institut B, RWTH Aachen University, 52074 Aachen, Germany
High-quality BaTiO3 films with thicknesses ranging from 2.9  to  175  nm were grown epitaxially on SrRuO3-covered (001)-oriented SrTiO3 substrates by high-pressure sputtering. The crystal structure of these films was studied by conventional and synchrotron x-ray diffraction. The in-plane and out-of-plane lattice parameters were determined as a function of film thickness by x-ray reciprocal space mapping around the asymmetric ([overline 1]03) Bragg reflection. BaTiO3 films were found to be fully strained by the SrTiO3 substrate up to a thickness of about 30  nm. Ferroelectric capacitors were then fabricated by depositing SrRuO3 top electrodes, and the polarization-voltage hysteresis loops were recorded at the frequencies 1–30  kHz. The observed thickness effect on the lattice parameters and polarization in BaTiO3 films was analyzed in the light of strain and depolarizing-field effects using the nonlinear thermodynamics theory. The theoretical predictions are in reasonable agreement with the measured thickness dependences, although the maximum experimental values of the spontaneous polarization and the out-of-plane lattice parameter exceed the theoretical estimates (43  µC/cm2 vs 35  µC/cm2 and 4.166  Å vs 4.143  Å). Possible origins of the revealed discrepancy between theory and experiment are discussed. ©2007 American Institute of Physics
History: Received 5 March 2007; accepted 20 April 2007; published 14 June 2007
Permalink: http://link.aip.org/link/?JAPIAU/101/114106/1
BUY THIS ARTICLE   (US$24)
Download HTML Download Sectioned HTML Download PDF (746 kB) View Cart

KEYWORDS and PACS

Keywords
PACS
  • 77.55.+f
    Dielectric thin films
  • 77.22.Ej
    Dielectric polarization and depolarization
  • 77.80.Dj
    Ferroelectric domain structure; hysteresis
  • 68.55.Jk
    Thin film structure and morphology; thickness; crystalline orientation and texture
  • 81.15.Cd
    Deposition by sputtering
  • 84.32.Tt
    Capacitors
  • YEAR: 2007

RELATED DATABASES


To view database links for this article,
you need to log in.
To view database links for this article,
you need to log in.

PUBLICATION DATA

ISSN:
0021-8979 (print)   1089-7550 (online)
Publisher:
AIP is a member of CrossRef AIP

REFERENCES (40)

For access to fully linked references, you need to log in. For access to fully linked references, you need to Log in.
  1. O. Auciello, J. F. Scott, and R. Ramesh, Phys. Today 51(7), 22 (1998).
  2. J. F. Scott, Ferroelectric Memories (Springer, Berlin, 2000).
  3. F. Jona and G. Shirane, Ferroelectric Crystals (Macmillan, New York, 1962).
  4. N. A. Pertsev, A. G. Zembilgotov, and A. K. Tagantsev, Phys. Rev. Lett. 80, 1988 (1998);
  5. Ferroelectrics 223, 79 (1999).
  6. A. G. Zembilgotov, N. A. Pertsev, H. Kohlstedt, and R. Waser, J. Appl. Phys. 91, 2247 (2002).
  7. Y. L. Li, L. E. Cross, and L. Q. Chen, J. Appl. Phys. 98, 064101 (2005).
  8. S. Tinte and M. G. Stachiotti, Phys. Rev. B 64, 235403 (2001).
  9. J. Junquera and Ph. Ghosez, Nature (London) 422, 506 (2003).
  10. O. Diéguez, S. Tinte, A. Antons, C. Bungaro, J. B. Neaton, K. M. Rabe, and D. Vanderbilt, Phys. Rev. B 69, 212101 (2004).
  11. B.-K. Lai, I. A. Kornev, L. Bellaiche, and G. J. Salamo, Appl. Phys. Lett. 86, 132904 (2005).
  12. N. Sai, A. M. Kolpak, and A. M. Rappe, Phys. Rev. B 72, 020101(R) (2005).
  13. G. Gerra, A. K. Tagantsev, N. Setter, and K. Parlinski, Phys. Rev. Lett. 96, 107603 (2006).
  14. R. Kretschmer and K. Binder, Phys. Rev. B 20, 1065 (1979).
  15. N. Yanase, K. Abe, N. Fukushima, and T. Kawakubo, Jpn. J. Appl. Phys., Part 1 38, 5305 (1999).
  16. K. J. Choi et al., Science 306, 1005 (2004).
  17. D. A. Tenne et al., Phys. Rev. B 69, 174101 (2004).
  18. O. Trithaveesak, J. Schubert, and Ch. Buchal, J. Appl. Phys. 98, 114101 (2005).
  19. D. J. Kim, J. Y. Jo, Y. S. Kim, Y. J. Chang, J. S. Lee, J.-G. Yoon, T. K. Song, and T. W. Noh, Phys. Rev. Lett. 95, 237602 (2005).
  20. Y. S. Kim et al., Appl. Phys. Lett. 88, 072909 (2006).
  21. F. He and B. O. Wells, Appl. Phys. Lett. 88, 152908 (2006).
  22. B. Dkhil, E. Defay, and J. Guillan, Appl. Phys. Lett. 90, 022908 (2007).
  23. B. Jaffe, W. R. Cook, Jr., and H. Jaffe, Piezoelectric Ceramics (Academic, London, 1971).
  24. N. A. Pertsev, Mater. Res. Soc. Symp. Proc. 902E, (2006).
  25. U. Poppe et al., Solid State Commun. 66, 661 (1988).
  26. J.-M. Triscone, P. Fivat, M. Andersson, M. Decroux, and Ø. Fisher, Phys. Rev. B 50, 1229 (1994).
  27. U. Pietsch, V. Holý, and T. Baumbach, High-Resolution X-Ray Scattering, 2nd ed. (Springer, Berlin, 2004), Chap. 9.
  28. N. A. Pertsev, J. Rodriguez Contreras, V. G. Kukhar, B. Hermanns, H. Kohlstedt, and R. Waser, Appl. Phys. Lett. 83, 3356 (2003).
  29. J. Y. Jo, Y. S. Kim, T. W. Noh, J.-G. Yoon, and T. K. Song, Appl. Phys. Lett. 89, 232909 (2006).
  30. J. Y. Jo, D. J. Kim, Y. S. Kim, S.-B. Choe, T. K. Song, J.-G. Yoon, and T. W. Noh, Phys. Rev. Lett. 97, 247602 (2006).
  31. R. R. Mehta, B. D. Silverman, and J. T. Jacobs, J. Appl. Phys. 44, 3379 (1973).
  32. A. Yu. Emelyanov, N. A. Pertsev, and A. L. Kholkin, Phys. Rev. B 66, 214108 (2002).
  33. N. A. Pertsev, A. K. Tagantsev, and N. Setter, Phys. Rev. B 61, R825 (2000).
  34. In the numerical calculations, we used the following set of thermodynamic parameters and material constants of BTO crystals (in SI units): a1=4.124(T−115)×105, a11=5.328×108, a12=3.426×108, a111=1.294×109,a112=−1.95×109, a123=−2.5×109, a1111=3.863×1010, a1112=2.529×1010, a1122=1.637×1010, a1123=1.367×1010,c11=1.755×1011, c12=8.464×1010, c44=1.082×1011, q11=1.203×1010, q12=−1.878×109, and q44=6.385×109. This set corresponds to the thermodynamics parameters of BTO reported in Ref. 6 and the electrostrictive and elastic constants listed in Ref. 4.
  35. N. A. Pertsev and H. Kohlstedt, e-print cond-mat/0603762 <http://arxiv.org/abs/cond-mat/0603762v2 [cond-mat.mtrl-sci].
  36. This value is equal to the nominal misfit strain S<sub>m</sub><sup>0</sup>=(ba0)/a0 between BTO and STO (b is the lattice parameter of the substrate).
  37. J. Matthews and A. E. Blakeslee, J. Cryst. Growth 27, 118 (1974).
  38. R. Dittmann, R. Plonka, E. Vasco, N. A. Pertsev, J. Q. He, C. L. Jia, S. Hoffmann-Eifert, and R. Waser, Appl. Phys. Lett. 83, 5011 (2003).
  39. J. S. Speck and W. Pompe, J. Appl. Phys. 76, 466 (1994).
  40. D. Fuchs, C. W. Schneider, R. Schneider, and H. Rietschel, J. Appl. Phys. 85, 7362 (1999).
  41. D. Fuchs, M. Adam, P. Schweiss, S. Gerhold, S. Schuppler, R. Schneider, and B. Obst, J. Appl. Phys. 88, 1844 (2000).

CITING ARTICLES

For access to citing articles, you need to log in.
For access to citing articles, you need to Log in.