nanonet
| JNNB Top | Subscribe Now! | INTERVIEW | YOUNG RESEARCHERS | TEXT | Past Issues |
JNNB Search

JAPAN NANONET BULLETIN - 78th Issue - August 31, 2006

YOUNG RESEARCHERS’ INTRODUCTION

Yuji NOGUCHI
Lecturer, Research Center for Advanced Science and Technology, The University of Tokyo

Development of hazardous-lead-free novel ferroelectrics

(Issued in Japanese: August 3, 2005)

Lead zirconate titanate (PZT) has been used in a wide variety of device applications, such as non-volatile memories and piezoelectric products. However, pollution and the destruction of ecological systems, because of illegally-dumped PZT devices, which release toxic lead, have become serious problems. We are trying to develop a novel lead-free ferroelectric that can act as an alternative to PZT.

We have been studying a bismuth layered ferroelectric (see Figure 1), which is a promising candidate for lead-free ferroelectrics. The perovskite layers are composed of m layers of TiO6 octahedra and bismuth-oxide layers that are alternately stacked in the crystal structure. It is well known that the family of the bismuth layered compounds can be ferroelectrics with an m between 1 and 5. We have grown a single-crystal of natural superlattice-structured ferroelectrics having alternating of Bi4Ti3O12 (m = 3) and BaBi4Ti4O15 (m = 4) layers. The crystal has the largest spontaneous polarization of 62 μC/cm2 in lead-free perovskite materials, and this value is larger than that of commercialized PZT (see Figure 2). Structural stress occurs because of the stacking of two different perovskite layers with different in-plane lattice parameters. This peculiar stress in the superlattice structure induces ferroelectric displacement of the Bi ions in the bismuth-oxide layers, which is the origin of the large spontaneous polarization. Furthermore, the introduction of layered defects in the superlattice structure, or in other words, a change in the ratio of the m = 3 and m = 4 layers will result in a larger spontaneous polarization in this system.

Currently, we have been investigating the superlattice-structured crystals with a large amount of layered defects. In addition to crystals, grain-oriented ceramics of this material have synthesized, and we are currently trying to determine their piezoelectric properties.

Yuji NOGUCHI
Yuji NOGUCHI
Lecturer, Research Center for Advanced Science and Technology, The University of Tokyo
 
1997Research Associate, Nagaoka University of Technology
1998Research Associate, Graduate School of Engineering, The University of Tokyo
2001Research Associate, Institute of Industrial Science, The University of Tokyo
2004Lecturer, Graduate School of Engineering, The University of Tokyo
2004Lecturer, Research Center for Advanced Science and Technology, The University of Tokyo
E-mail:

HomePage

Fig.1
Fig.1 Large Image
Transmission electron micrograph of a natural-superlattice-structured Bi4Ti3O12 - BaBi4Ti4O15 crystal with a giant spontaneous polarization. The superlattice structure consists of two kinds of perovskite layers, Bi4Ti3O12 (m = 3) and BaBi4Ti4O15 (m = 4), where m is the number of TiO6 octahedral layers. The ferroelectric distortion is induced by the structural stress between two kinds of perovskite layers.
Fig.2
Fig.2 Large Image
Giant spontaneous polarization observed for natural-superlattice-structured Bi4Ti3O12 - BaBi4Ti4O15 crystals. The spontaneous polarization of the Bi4Ti3O12 - BaBi4Ti4O15 crystals (red) is larger than those of the constituent crystals of Bi4Ti3O12 (black) and BaBi4Ti4O15 (blue).

Relevant papers
  1. Kobayashi, T., Noguchi, Y. & Miyayama, M.
    Enhanced spontaneous polarization in superlattice-structured Bi4Ti3O12-BaBi4Ti4O15 single crystals
    Appl. Phys. Lett. 86, 012907 (2005).
  2. Noguchi, Y., Matsumoto, T. & Miyayama, M.
    Impact of Defect Control on the Polarization Properties in Bi4Ti3O12 Ferroelectric Single Crystals
    Jpn. J. Appl. Phys. (Express Letters) 44, L570-572 (2005).
  3. Goshima, Y., Noguchi, Y. & Miyayama, M.
    Dielectric and ferroelectric anisotropy of intergrowth Bi4Ti3O12-PbBi4Ti4O15 single crystals
    Appl. Phys. Lett. 81, 2226-2228 (2002).