[en] The polarization of PbTiO3/SrTiO3 superlattices is experimentally tuned from 0-60 mu C/cm(-2) and the transition temperature from room temperature to 1000 K while maintaining a perfect crystal structure and low leakage currents (see figure). A simple model based on Landau theory is developed as a guide for the straightforward production of samples with ferroelectric properties designed for particular applications.
Disciplines :
Chemistry Materials science & engineering Physics
Author, co-author :
Dawber, Matthew
Stucki, Nicolas
Lichtensteiger, Celine
Gariglio, Stefano
Ghosez, Philippe ; Université de Liège - ULiège > Département de physique > Physique théorique des matériaux
Triscone, Jean*-Marc
Language :
English
Title :
Tailoring the properties of artificially layered ferroelectric superlattices
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Bibliography
See, for instance, M. Dawber, K. M. Rabe, J. F. Scott, Rev. Mod. Phys. 2005, 77, 1083.
J. F. Scott, Ferroelectric Memories, Springer, Berlin 2000.
P. Muralt, J. Micromech. Microeng. 2000, 10, 136.
C. H. Ahn, K. M. Rabe, J.-M. Triscone, Science 2004, 303, 488.
P. Ghosez, J. Junquera, in Handbook of Theoretical and Computational Nanotechnology, Vol. 4(Eds: M. Rieth, W. Schommens), American Scientific Publishers, Stevenson ranch, CA 2006, p. 623.
J. B. Neaton, K. M. Rabe, Appl. Phys. Lett. 2003, 82, 1586.
M. Dawber, C. Lichtensteiger, M. Cantoni, M. Veithen, P. Ghosez, K. Johnston, K. M. Rabe, J.-M. Triscone, Phys. Rev. Lett. 2005, 95, 177601.
H. N. Lee, H. M. Christen, M. F. Chrisholm, c. M. Rouleau, D. M. Lowndes, Nature 2005, 433, 395.
D. Tenne, A. Bruchhausen, N. D. Lanzillotti-Kimura, A. Fainstein, R. S. Katiyar, A. Cantarero, A. Soukiassian, V. Vatihyanathan, J. H. Haeni, W. Tian, D. G. Schlom, K. J. Choi, D. M. Kim, C. B. Eom, H. P. Sun, X. Q. Pan, Y. L. Li, L. Q. Chen, Q. X. Jia, S. M. Nakhmanson, K. M. Rabe, X. X. Xi, Science 2006, 313, 1614.
B. Jaffe, W. R. Cook, H. Jaffe, Piezoelectric Ceramics, Academic, London 1971.
Landolt-Börnstein, Vol. III/16a (Eds: K. H. Hellwege, A. M. Hellwege), Springer, Berlin 1981.
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. Tagantsev, X. Q. Pan, S. K. Streiffer, L. Q. Chen, S. W. Kirchoefer, J. Levy, D. G. Schlom, Nature 2004, 430, 758.
S. A. Mabud, A. M. Glazer, J. Appl. Crystallogr. 1979, 12, 49.
N. A. Pertsev, A. G. Zembilgotov, A. K. Tagantsev, Phys. Rev. Lett. 1998, 80, 1988.
H. Tabata, H. Tanaka, T. Kawai, Appl. Phys. Lett. 1994, 65, 1970.
A. L. Roytburd, S. Zhong, S. P. Alpay, Appl. Phys. Lett. 2005, 87, 092902.
S. Zhong, S. P. Alpay, J. V. Mantese, Appl. Phys. Lett. 2006, 88, 132904.
N. A. Pertsev, A. K. Tagantsev, N. Setter, Phys. Rev. B 2000, 67, R825.
All values are given in SI units (a1 = J m C-2, a11 = J m5 C-4, a111 = J m 9 C-6, gij = J m C-2, cij = J m-3). For PbTiO3: a1 = 3.8 × 10 5(T - 752), a11 = 4.229 × 108, a 111 = 2.6 × 108, C11 = 1.746 × 1011, C12 = 0.794 × 1011, g11 = 1.14 × 1010, g12 = 4.63 × 108. For SrTiO3: a1 = 7.45 × 105(T - 51.64) (This is a linear approximation that is only valid above - 100K), a11 = 2.02 × 109, c11 = 3.36 × 1011, c12 = 1.07 × 1011, g11 = 1.25 × 1010, g12 = -0.108 × 1010.
J. F. Scott, L. Kammerdiner, M. Parris, S. Traynor, V. Ottenbacher, A. Shawabkeh, W. F. Oliver, J. Appl. Phys. 1988, 64, 787.
C. Lichtensteiger, J.-M. Triscone, J. Junquera, P. Ghosez, Phys. Rev. Lett. 2005, 94, 047603.
S. K. Streiffer, J. A. Eastman, D. D. Fong, C. Thompson, A. Munkholm, M. V. R. Murty, O. Auciello, G. R. Bai, G. B. Stephenson, Phys. Rev. Lett. 2002, 89, 067601.
D. D. Fong, A. M. Kolpak, J. A. Eastman, S. K. Streiffer, P. H. Fuoss, G. B. Stephenson, C. Thompson, D. M. Kim, K. J. Choi, C. B. Eom, I. Grinberg, A. M. Rappe, Phys. Rev. Lett. 2006, 96, 127601.
C.-L. Jia, V. Nagarajan, J. Q. He, L. Houben, T. Zhao, R. Ramesh, K. Urban, R. Waser, Nat. Mater. 2007, 6, 64.
S. Ganglio, N. Stucki, G. Triscone, J.-M. Triscone, Appl. Phys. Lett. 2007, 90, 202905.
K. J. Choi, M. Biegalski, Y. L. Li, A. Sharan, J. Schubert, R. Uecker, P. Reiche, Y. B. Chen, X. Q. Pan, V. Gopalan, L. Q. Chen, D. G. Schlom, C. B. Eom, Science 2004, 306, 1005.
C. H. Ahn, J.-M. Triscone, J. Mannhart, Nature 2003, 424, 1015.
C. H. Ahn, A. Bhattacharya, M. Di Ventra, J. N. Eckstein, C. D. Frisbie, M. E. Gershenson, A. M. Goldman, I. H. Inoue, J.Mannhart, A. J. Millis, A. F. Morpurgo, D. Natelson, J.-M. Triscone, Rev. Mod. Phys. 2006, 78, 1185.
A. I. Kingon, J. P. Maria, S. K. Streiffer, Nature 2000, 406, 1032.
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