Microscopically structural studies of lithium niobate powders
Introduction
Lithium niobate LiNbO3 (LN) is an important functional crystal material that has been widely used in the modern science and technology due to its large pyroelectric, piezoelectric, electro-optical and photo-elastic coefficients and good optical, electric, acousto-optical and electro-mechanical properties, etc. Recently, with the development of the application of functional devices, the synthesis of LN powders attracts much attention and becomes an interesting topic in the field of LN crystals, since materials scientists have focused on the first step of the growth of LN single crystals (the synthesis of LN powders) in order to obtain LN single crystals with a high quality and large size, which can match different kinds of practical needs.
Over the past several decades, LN powders were traditionally synthesized by the conventional high temperature solid-state method at 1200 °C from the raw powders of Li2CO3 and Nb2O5, which often results in the growth of inhomogeneous and uncontrollable large grains, the formation of additional phases and possible loss of the crystal stoichiometry due to the easy volatilization of lithium at the high temperature. In recent years, a number of the wet chemical syntheses have been reported for the synthesis of LN powders, which include the hydrothermal route [1], peroxide route [2], water-soluble complex method [3], solvethermal route [4] and metal alkoxides method [5]. However, there still exist some problems, such as the uneasy control of reaction conditions and long reaction time. The combustion synthesis is an attractive technique for producing LN powders [6], whose advantages are that an organic compound (e.g. urea) gives out heat that can be effectively supplied to the raw reagent of Li2CO3 and Nb2O5 powders, the supplied energy can speed up the chemical reaction, decrease the reaction time, and also reduce the reaction temperature (∼500–600 °C). Moreover, this method does not need to use any organic and inorganic solvents in the whole reaction process, on the other hand, the generation of impurities during this processing can be greatly avoided.
The crystallographic structure of LN crystals consists of distorted oxygen octahedra by sharing their common faces (along the c-axis) or edges (at the ab plane), which forms a trigonal (c-axial) lattice. The succession of the cations in the columns of octahedra along a three-fold axis (c-axis) is as follows: Li, Nb and an empty octahedron. In the ferroelectric phase, both Nb5+ and Li+ cations are displaced from the centers of their respective octahedra. Additionally, in the three dimensional frame, NbO6 octahedra link each other by sharing their common corners and similarly, LiO6 octahedra each other by sharing their common corners [7], [8]. The crystallographic structure of LN crystals is shown in Fig. 1. Although the structure of LN crystals has been extensively studied for several decades, however, the characteristic structure of LN powders has not yet been investigated. In this work, the crystallographic structure of the LN powders is studied in detail on the basis of crystal structure properties. And the structural analysis is also validated by the characterization result of the obtained LN powders that are synthesized by an organic combustion method.
Section snippets
Experimental
Analytical reagent (A.R.) Li2CO3 and ultra purity Nb2O5 powders are mixed with a molar ratio of [Nb]/[Li]=1:1, followed by addition of some urea (A.R.) powders. The quantity ratio [urea]: [Li2CO3+Nb2O5]≈3:1 is adopted in our experiment. The reagent is finely grounded into powders to form the homogeneity, and is put into a clean crucible. The crucible is then put into a heater, the temperature of the heater is continuously increased and kept at 500–600 °C for 2.5 h. The obtained samples are pure
Results and discussion
Law of Bravais—“The points in any lattice can be arranged to lie on a larger number of different planes, called lattice planes, some of which will contain more points per unit area than others. The external faces of a crystal are parallel to lattice planes, and the most commonly occurring faces will be those which correspond to planes containing a high density of points, usually referred to as a high reticular density” [9]. Cleavage also occurs along lattice planes. Bravais suggested that the
Acknowledgements
The financial support from the National Natural Science Foundation of China (Grant No. 20471012), a Foundation for the Author of National Excellent Doctoral Dissertation of P.R. China (Grant No. 200322), the Research Fund for the Doctoral Program of Higher Education (Grant No. 20040141004) and the Scientific Research Foundation for the Returned Overseas Chinese Scholars, State Education Ministry is greatly acknowledged.
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