NSF Chemical Bonding Center: Chemical Design of MaterialsNational Science Foundation


Theme II: Anion control of polar behavior
Theme Leader: Woodward

The traditional approach to the design of functional materials is to consider a certain fixed anion lattice and then to vary the nature and relative amounts of the cations. In this research theme we will explore the feasibility and consequences of substitution on the anion lattice, as an alternative and underutilized approach to materials development. There are a number of mixed anionic systems already known that possess interesting properties. For example superconductivity has been found in copper oxychlorides[1,2], nitride-chlorides of zirconium and hafnium[3,4], and oxyfluorides related to the copper oxide superconductors[5,6]. All of these examples adopt layered structures, which are strongly favored when the two anions have highly contrasting size and/or polarizabilities. While layered structural motifs are clearly favorable for the occurrence of superconductivity[7,8,9], there are relatively few polar materials that adopt layered structures. Thus our efforts will be initially directed towards compounds where the two ions are relatively similar in size, in particular oxynitrides, and to a lesser extent oxyfluorides and nitride fluorides. As the project progresses computations will be used to see if layered structures are inherently incompatible with strong polarity, and if not, to suggest which systems should be synthetically targeted for further study.

Our work will initially focus on oxynitrides, in which some (but not all) oxide ions are replaced by nitride ions. The importance of this class of materials is manifested in the recent discovery (by Woodward) of high permittivity in the perovskite oxynitrides BaTaO2N (k ~ 5000) and SrTaO2N (k ~ 2500)[10]. The key role of anion substitution is underscored by the fact that the all-oxide analogues, KTaO3 and NaTaO3, do not exhibit unusual dielectric properties[11]. However the detailed origin of the large dielectric response is not yet well understood, and potential applications have yet to be explored. In this theme we will explain the fundamental chemical interactions driving the high permittivity, and develop new oxynitride materials with properties tailored for specific applications.

Our rationale for replacing oxide ions by nitride ions is twofold. First, the covalency of the metal-anion bond is increased thereby enhancing the tendency for SOJT distortions. We will use this effect to induce or enhance SOJT displacements of cations that normally do not show a strong tendency to undergo out-of-center displacements (i.e. Ta5+, Zr4+, etc.). Second, the presence of two distinct types of anions affords the opportunity to create an acentric environment about a metal cation in a structure where the cation environment would otherwise be a symmetric octahedron. Here we will use density functional theory to predict off-centering, since simple intuition based on symmetry considerations has proved inadequate in the past. For example in BaTaO2N each Ta-centered octahedron contains on average four oxide ions and two nitride ions Symmetry suggests that the Ta5+ ion should displace from the center of its coordination polyhedron when the nitride ions occupy cis-positions in the octahedron, but not when they adopt a trans-configuration. However density functional calculations on ordered variants of BaTaO2N indicate ~ 0.10 Å displacements of the Ta cation[12] in both cis- and trans-configurations, with the trans- displacement originating from the strong covalency of the Ta-N interaction. This type of distortion can be rationalized after the fact, but without the aid of accurate calculational tools it is difficult to predict in advance. The ATaO2N (A = Ba, Sr) system offers one example of how polar displacements can be triggered and controlled through manipulations of the composition and distribution of the anion lattice; in the CDM we will search computationally and synthetically for other examples.

Progress in the field has been hampered by two factors, both of which will be overcome in this collaboration. First, oxynitrides are very difficult to sinter. Preliminary work in Woodward's group (in collaboration with the Center for Functional Nanomaterials at Brookhaven National Lab) has shown that thin films of BaTaO2N can be grown, and that the resulting films have high dielectric constants[13]. Film orientation, the properties and the potential impurity phases are very sensitive to the substrate, the oxygen partial pressure and the growth temperature. Extending the study to related materials, for example SrTaO2N and CaTaO2N, or ordered oxynitrides, such as La3Ta2MgO6N3 and La2TaMgO5N, vastly increases the number of variables. Therefore, to realize the potential of these intriguing materials, our experts in film deposition (Salvador and Stemmer). will collaborate closely with our chemists. A second issue, is understanding the many variables in structure and composition space that play pivotal roles, and how to manipulate these variables to design materials with optimal properties. For example, in BaTaO2N the anion distribution is disordered and powder diffraction measurements suggest a centrosymmetric, cubic crystal structure [10,14,15]. This is in contradiction to the DFT calculations on ordered structures[12] as well as the dielectric properties, and is likely the result of averaging over differently oriented polar regions. Recent EXAFS measurements give strong evidence that the Ta ions are displaced and the average crystal structures do not represent the true local structure[16]. We will use high level calculations to explore the properties of various anion arrangements. Another question raised by the initial work is the role of the A-site cation. Measurements on fairly porous ceramic disks show different temperature dependencies of the dielectric constant (tck) in BaTaO2N (tck ~ +1138 ppm/K) and SrTaO2N (tck ~ -739 ppm/K), raising the possibility that solid solutions might show extremely high permittivity with almost no temperature dependence. Furthermore, CaTaO2N does not possess a high permittivity (k ~ 30). While it is well known that dielectric properties are closely linked to various types of distortions in perovskites the reasons for strikingly different behavior in these three compounds are not understood at this time. To develop a better understanding, Spaldin will perform DFT calculations to determine the types of displacements that occur in ordered oxynitrides, and the influence of various displacements on the dielectric response. The correlations between octahedral tilting, SOJT displacements and dielectric properties will be determined. Her calculations of structural stabilities will also help determine the range of structure types and counterions that can be realized with oxynitrides. Finally, with modern DFT tools, it is possible, to some degree, to study how the energies and properties of ordered and disordered materials differ. Spaldin's results will allow us to to screen for new and interesting oxynitride materials, and determine which materials are worthwhile candidates for large-scale preparation efforts. The added efficiency obtained by utilizing computations to guide synthetic efforts should also allow us to broaden our investigations to other structure types, such as pyrochlore, Ruddlesden-Popper and Aurivillius phases.

The initial studies of semiconducting oxynitrides are very exciting. This class of compounds potentially represents a new class of dielectric and optical materials. Once formed, the perovskite oxynitrides are stable in air, water, and even strong acids[14,15], so the potential for applications is very real. However, the synthesis can be slow and unpredictable. Consequently, the interplay between synthesis and computations is necessary to increase efficiency. Furthermore, the extreme difficulty in preparing either single crystal or highly sintered ceramics makes thin film deposition essential in order to accurately characterize properties. The skills in synthesis, thin film growth, electrical and optical characterization and computation that will be assembled in the CDM represent an ideal mix of skills to effectively attack this challenging, but potentially very rewarding area of research.

Current research activities:

The preparation of oxynitride targets is diffcult and time-consuming, therefore Woodward and Salvador are exploring the effect of growth conditions on the stability and stoichiometry of oxynitride thin films using PLD from oxide targets. The work of graduate student Young-Il Kim (Woodward group) has resulted in the growth of thin film specimens of BaTaO2N perovskites on SrTiO3/SrRuO3 substrates using PLD from a target of the same composition (in collaboration with Weidong Si and Tom Vogt at BNL). In a collaboration between Woodward and Salvador, thin films of SrNbO2N have been deposited from an oxide target (Sr2Nb2O7), and are now being prepared for physical property measurements. The SrNbO2N was found to form as both epitaxial and polycrystalline films when deposited from the Sr2Nb2O7 target in a N2 atmosphere at 700 ºC. The stability of polycrystalline films implies that the phase is stable in the ablation conditions and is not an artifact of epitaxial stabilization; consequently other oxynitrides are likely to be easily synthesized. Ablation targets have therefore been prepared for other phases, and synthesis conditions of LaTiO2N, LaZrO2N, and LaSnO2N are currently being optimized. Characterization of the dielectric properties of all the oxynitrides (for Theme III) is in progress.

Research findings

Pulsed laser deposition from oxide (rather than oxynitrides) targets is an effective way of growing new oxynitrides. For example SrNbO2N can be formed as both epitaxial and polycrystalline films when deposited using pulsed laser deposition with a Sr2Nb2O7 ablation target in a nitrogen atmosphere at ºC. The stability of polycrystalline films implies that the phase is stable in the ablation conditions and is not an artifact of epitaxial stabilization. This suggests that other oxynitrides are likely to be easily synthesized.

 

References

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[3] S. Yamanaka, K. Hotehama, and H. Kawaji. Superconductivity at 25.5 K in electron-doped layered hafnium nitride. Nature, 392:580-582, 1998.

[4] S. Yamanaka, H. Kawaji, K. Hotehama, and M. Ohashi. A new layer-structured nitride superconductor. lithium-intercalated b-zirconium nitride chloride, LixZrNCl. Adv. Mater., 8:771-773, 1996.

[5] A. C. W. P. James, S. M. Zahurak, and D. W. Murphy. Superconductivity at 27 K in fluorine-doped Nd2CuO4. Nature, 338:240-241, 1989.

[6] M. Almamouri, P. P. Edwards, C. Greaves, and M. Slaski. Synthesis and superconducting properties of the strontium copper oxy-fluoride Sr2CuO2F2+x. Nature, 369:382-384, 1994.

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[8] C. Felser, K. Thieme, and R. Seshadri. Electronic instabilities in compounds with hexagonal nets. J. Mater. Chem., 9:451-457, 1999.

[9] C. Felser and R. Seshadri. Electronic structures and instabilities of ZrNCl and HfNCl: implications for superconductivity in the doped compounds. J. Mater. Chem., 9:459-454, 1999.

[10] Y.-I. Kim, P. M. Woodward, K. Z. Baba-Kishi, and C. W. Tai. Characterization of the structural, optical and dielectric properties of oxynitride perovskites AMO2N (A = Ba, Sr, Ca; M = Ta, Nb). Chem. Mater., 16:1267-1276, 2004.

[11] R. D. Shannon and C. T. Prewitt. Revised effective ionic radii and systematic studies of interatomic distances in halides and chalcogenides. Acta Crystallogr. A, 32:751-767, 1976.

[12] C. M. Fang, G. A. de Wijs, E. Orhan, G. de With, R. A. de Groot, H. T. Hintzen, and R. Marchand. Local structure and electronic properties of BaTaO2N with perovskite-type structure. J. Phys. Chem. Solids, 64:281-286, 2003.

[13] Y. I. Kim, P. M. Woodward, W. D. Si, S. M. Park, T. Vogt, and P. Johnson. Pulsed laser deposition of high permitivity BaTaO2N films. 2004. in preparation.

[14] R. Marchand, Y. Laurent, J. Guyader, P. L'Haridon, and P. Verdier. Nitrides and oxynitrides: preparation, crystal chemistry and properties. J. Eur. Ceram. Soc., 8:197-213, 1991.

[15] M. Jansen and H. P. Letschert. Inorganic yellow-red pigments without toxic metals. Nature, 404:980-982, 2000.

[16] B. Ravel, Y. I. Kim, and P. M. Woodward. EXAFS studies of the local structure of ATaO2N (A = Ba, Sr, Ca) oxynitrides. 2004. in preparation.


 

   
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