Applied Physics Letters
Search:
   
 
 
 
Previous Article
Piezoelectric responses in poly(vinylidene fluoride/hexafluoropropylene) copolymers
The authors show that a high transverse piezoelectric response with both high piezoelectric d31 (d31=43.1  pm/V) and electromechanical coupling k31 coefficients (k31=0.187), much higher than...
Next Article
Near-field laser parallel nanofabrication of arbitrary-shaped patterns
The authors present a simple and efficient technique for laser writing of arbitrary nanopatterns across a large surface area without using projection masks. It is based on the unique near-field focusi...

Theoretical phase diagram of ultrathin films of incipient ferroelectrics

Appl. Phys. Lett. 90, 242918 (2007); doi:10.1063/1.2748844

Published 15 June 2007

You are not logged in to this journal. Log in

A. R. Akbarzadeh
Department of Materials Science and Engineering, University of California, Los Angeles, P.O. Box 951595, Los Angeles, California 90095-1595 and Physics Department, University of Arkansas, Fayetteville, Arkansas 72701

L. Bellaiche
Physics Department, University of Arkansas, Fayetteville, Arkansas 72701

Jorge Íñiguez
Institut de Ciencia de Materials de Barcelona (ICMAB-CSIC), Campus UAB, 08193 Bellaterra, Spain

David Vanderbilt
Department of Physics and Astronomy, Rutgers University, Piscataway, New Jersey 08854-8019
A first-principles-based scheme is used to compute the temperature-versus-misfit strain “Pertsev” phase diagram of ultrathin films of incipient ferroelectric KTaO3. The results suggest that, at variance with the bulk material, KTaO3 ultrathin films cannot be described as quantum paraelectrics. Rather, the behavior of the films is largely determined by surface/interface effects that favor ferroelectricity and the imperfect screening of the depolarizing fields. This leads to Pertsev phase diagrams that are qualitatively similar to those of normal ferroelectrics such as BaTiO3. ©2007 American Institute of Physics
History: Received 1 May 2007; accepted 21 May 2007; published 15 June 2007
Permalink: http://link.aip.org/link/?APPLAB/90/242918/1
BUY THIS ARTICLE   (US$24)
Download HTML Download Sectioned HTML Download PDF (200 kB) View Cart

KEYWORDS and PACS

Keywords
PACS
  • 77.84.Dy
    Dielectric, piezoelectric, and ferroelectric niobates, titanates, tantalates, PZT ceramics, etc
  • 77.55.+f
    Dielectric thin films
  • 81.30.Dz
    Phase diagrams of other materials excluding metals and alloys
  • 77.80.-e
    Ferroelectricity and antiferroelectricity
  • 77.22.Ej
    Dielectric polarization and depolarization
  • 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:
0003-6951 (print)   1077-3118 (online)
Publisher:
AIP is a member of CrossRef AIP

REFERENCES (27)

For access to fully linked references, you need to log in. For access to fully linked references, you need to Log in.
  1. M. Dawber, K. M. Rabe, and J. F. Scott, Rev. Mod. Phys. 77, 1083 (2006).
  2. J. F. Scott, Science 246, 1400 (1989).
  3. I. Kornev, H. Fu, and L. Bellaiche, J. Mater. Sci. 41, 137 (2006).
  4. B.-K. Lai, I. Kornev, L. Bellaiche, and G. J. Salamo, Appl. Phys. Lett. 86, 132904 (2005).
  5. N. A. Pertsev, V. G. Kukhar, H. Kohlstedt, and R. Waser, Phys. Rev. B 67, 054107 (2003).
  6. O. Diéguez, S. Tinte, A. Antons, C. Bungaro, J. B. Neaton, K. M. Rabe, and D. Vanderbilt, Phys. Rev. B 69, 212101 (2004).
  7. S. K. Streiffer, J. A. Eastman, D. D. Fong, C. Thompson, A. Munkholm, M. V. Ramana Murty, O. Auciello, G. R. Bai, and G. B. Stephenson, Phys. Rev. Lett. 89, 067601 (2002).
  8. I. Kornev, H. Fu, and L. Bellaiche, Phys. Rev. Lett. 93, 196104 (2004).
  9. I. Ponomareva and L. Bellaiche, Phys. Rev. B 74, 064102 (2006).
  10. R. Viana, P. Lunkenheimer, J. Hemberser, R. Bohmer, and A. Loidl, Phys. Rev. B 50, 601(R) (1994).
  11. A. R. Akbarzadeh, L. Bellaiche, K. Leung, J. Íñiguez, and D. Vanderbilt, Phys. Rev. B 70, 054103 (2004).
  12. B. Salce, J. L. Gravil, and L. A. Boatner, J. Phys.: Condens. Matter 6, 4077 (1994).
  13. J. H. Haeni, P. Irvin, W. Chang, R. Uecker, P. Reiche, Y. L. Li, S. Choudhury, W. Tian, M. E. Hawley, B. Craigo, A. K. Taganstev, X. Q. Pan, S. K. Streiffer, L. Q. Chen, S. W. Kirchoefer, J. Levy, and D. G. Schlom, Nature (London) 430, 758 (2004).
  14. W. Zhong, D. Vanderbilt, and K. M. Rabe, Phys. Rev. Lett. 73, 1861 (1994);
  15. Phys. Rev. B 52, 6301 (1995).
  16. I. Ponomareva, I. Naumov, I. Kornev, H. Fu, and L. Bellaiche, Phys. Rev. B 72, 140102(R) (2005).
  17. I. I. Naumov and H. Fu, arXiv:cond-mat/0505497.
  18. At a quantitative level, our simple truncation may well be underestimating this enhancement for some choices of electrodes and overestimating it for others. At any rate, as the interesting effects resulting from our simulations are very pronounced, we are confident that they can be taken as reliable qualitative predictions.
  19. N. Sai, A. M. Kolpak, and A. M. Rappe, Phys. Rev. B 72, 020101(R) (2005).
  20. J. E. Spanier, A. M. Kolpak, J. J. Urban, I. Grinberg, L. Quyang, W. Soo Yun, A. M. Rappe, and H. Park, Nano Lett. 6, 735 (2006).
  21. N. Metropolis, A. W. Rosenbluth, M. N. Rosenbluth, A. H. Teller, and E. T. Teller, J. Chem. Phys. 21, 1087 (1953).
  22. W. Zhong and D. Vanderbilt, Phys. Rev. B 53, 5047 (1996).
  23. J. Íñiguez and D. Vanderbilt, Phys. Rev. Lett. 89, 115503 (2002).
  24. D. M. Ceperley, Rev. Mod. Phys. 67, 279 (1995).
  25. The lines displayed in Figs. 1 and 2 do not intersect at an accurately defined strain-temperature four-phase point. This is partly because the transition lines are linear fits of our simulated data points, and also because we have a 10–20  K uncertainty in the predicted transition temperatures.
  26. S. Rios, J. F. Scott, A. Lookman, J. McAneney, R. M. Bowman, and J. M. Gregg, J. Appl. Phys. 99, 024107 (2006).
  27. For zero misfit strain, beta=1 and T=50  K, both CMC and PI-QMC rendered uz[approximate]0.041 and 0.037  a.u. for surface/interface and inner layers, respectively. For beta=0.96, these values get reduced to 0.015 and 0.013  a.u., respectively, for CMC, and to 0.013 and 0.012  a.u., respectively, for PI-QMC. The corresponding magnitude of the local mode is 0.024  a.u. at T=20  K in bulk KTaO3, according to CMC.
  28. J. Junquera and P. Ghosez, Nature (London) 422, 506 (2003).

CITING ARTICLES

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