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NSF Nanoscale Science and Engineering Grantees Conference, Dec 3-5, 2008 Grant #: CMMI 0709293 NIRT: Composition Graded, Epitaxial Oxide Nanostructures: Fabrication and Properties NSF NIRT CMMI -0709293 PIs: Efstahios I. Meletis 1 , Jiechao Jiang 1 , Chonglin Chen 2 , Amar S. Bhalla 2 , and Gemunu Gunaratne 3 1 University of Texas Arlington, 2 University of Texas San Antonio, 3 University of Houston Introduction and Objectives: Perovskite oxides are of enormous fundamental interest and technological importance due to their intriguing properties which can be tailored for a wide range of applications in magnetic, magnetoelectronic, photonic, and spintronic technology. Such oxides have been synthesized in the past in bulk form or as thin films. Compositionally gradient thin films and nanostructures of these oxides are expected to offer enormous opportunities to explore intriguing physics and applications. However, major challenges exist in the synthesis of such structures since their fabrication by self-organization has not yet been attempted. Recently, we achieved fabrication of Figure 1. XTEM image of epitaxial (La,Sr)MnO3 continuous film (a) and nanopillars (b) on (001) LaAlO3 substrate. (c) Plan-view TEM of epitaxial (La,Sr)MnO3 nanopillars.

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NIRT: Composition Graded, Epitaxial Oxide Nanostructures: Fabrication and Properties

NSF Nanoscale Science and Engineering Grantees Conference, Dec 3-5, 2008

Grant #: CMMI 0709293

NIRT: Composition Graded, Epitaxial Oxide Nanostructures:

Fabrication and Properties

NSF NIRT CMMI -0709293

PIs: Efstahios I. Meletis1, Jiechao Jiang1, Chonglin Chen2, Amar S. Bhalla2, and

Gemunu Gunaratne3

1 University of Texas Arlington, 2University of Texas San Antonio, 3University of Houston

Introduction and Objectives: Perovskite oxides are of enormous fundamental interest and technological importance due to their intriguing properties which can be tailored for a wide range of applications in magnetic, magnetoelectronic, photonic, and spintronic technology. Such oxides have been synthesized in the past in bulk form or as thin films. Compositionally gradient thin films and nanostructures of these oxides are expected to offer enormous opportunities to explore intriguing physics and applications. However, major challenges exist in the synthesis of such structures since their fabrication by self-organization has not yet been attempted. Recently, we achieved fabrication of ordered arrays of coherent, orthogonal one-dimensional epitaxial (La, Sr)MnO3 nanopillars on (001) LaAlO3 substrate by pulsed-laser deposition (PLD), which to the best of our knowledge, has been the first report on the fabrication by self-organization of such epitaxial oxide nanopillars. The formation of the nanopillars depends strongly on the processing temperature and oxide composition. Such nanopillars exhibit novel magnetic properties different from those of their bulk, thin film, or nanoparticle counterparts. This research focuses on fully exploiting the enormous potential of these self-organized nanostructures by adding a novel and challenging dimension to their nanomanufacturing: to fabricate such nanopillars with a high perpendicular anisotropy arising from variation in composition, either continuously (graded) or discretely (composite, modulated layers) using PLD and investigate the effects of processing and material parameters on their formation by self-organization; to characterize their magnetic properties and morphological, structure and interface structures using newly developed HRTEM methods [1,2] and other complementary analytical techniques; to perform finite element modeling and physical property (ferroelectric, piezoelectric, ferromagnetic, ferroelastic, etc.) measurements on designed new ferroic composites and to conduct theoretical modeling of the self-organization process in conjunction with the experimental findings.

Results: We have systematically investigated the effects of processing parameters (temperature, pressure, laser energy and frequency) during deposition and post-annealing on the formation of epitaxial (La,Sr)MnO3 continuous films and nanopillars. We are able to fabricate (La,Sr)MnO3 continuous epilayer (Fig. 1a) and discrete epitaxial nanopillars (Figs. 1b and c) by manipulating the experimental conditions and parameters and confirmed the repeatability for achieving a variety of designed nanostructures. A roadmap for fabricating various distinct epitaxial nanostructures has been established. Knowledge obtained from these series of investigations is used for theoretical modeling for precisely controlling and predicting the formation of the nanopillar structures. Structures formed during the growth of an epilayer on a substrate are determined by minimizing the energy of the configuration, which consists of (i) elastic energy of the epilayer, due to the requirement that it be commensurate with the substrate, (ii) the surface energy of the epilayer, and (iii) the wetting potential [3]. We assume that the substrate lattice is unchanged, and hence that there is no associated energy. The spatio-temporal dynamics of the epilayer is typically described using the evolution of its height h(x,y) via

where the diffusion is along the surface h(x,y) [3]. Unfortunately, the expressions for the terms on the right (the free energy density, curvature, wetting energy etc.) in terms of h(x,y) and its derivatives are very complicated. The analysis can be simplified by using the “small slope” expansion, which will be valid close to the Stransky-Krastonow instability, where the homogeneous solution destabilizes to a patterned array [4]. Under these conditions, the previous equation reduces to

In deriving this equation, we have scaled h(x,y) by the height L at which the homogeneous layer destabilizes. The control parameters L, g, p, and q can be evaluated n terms of the mechanical parameters of the substrate and the epilayer.

Under the model dynamics, a uniform (but noisy) deposition of atoms on a substrate gives self-assembled quantum-dot arrays. In order to form large-scale perfect arrays, we use a technique that we proposed previously; namely masking of the deposition [5]. Properties of the mask can be determined from the spatio-temporal dynamics of the formation of a disordered pattern in the absence of the mask [5]. Figure 2 shows such a large-scale ordered quantum-dot array.

We also recently identified non-lead ferroelectric material, Barium titanate (BaTiO3) and its modified materials, such as (Ba, Sr)TiO3 and Ba(Zr,Ti)O3, based thin films as another counterpart for the composition graded nanostructures. These thin films exhibit high dielectric constant, relatively low dielectric loss tangent and large electric field tunability that have attracted considerable attention for dynamic random access memories (DRAM), bypass capacitors, IR detectors, and tunable microwave applications in tunable filters, phase shifter, antennas, etc. We have recently successfully fabricated “microstructure” graded Ba(Zr,Ti)O3 thin films on (001) MgO substrate (Figs. 3a-d). Ba(Zr,Ti)O3 thin films were first epitaxially grown on the substrate. On the top of the Ba(Zr,Ti)O3 epilayer, multi-oriented twins were formed by sharing their {111} planes with the epilayer, as schematically illustrated in Fig. 3e. Such microstructure graded thin films show interesting abnormal ferroelectric properties (Fig. 3f) that do not exist in their bulk counterpart.

We expect that this synergistic effort will yield new fundamental knowledge on self-organization of 1-D, epitaxial oxide nanostructures with graded composition. Variation in chemical composition opens up various new possibilities of designing new multiferroic nanoscale structures with unusual cross coupled properties.

References

[1]J.C. Jiang, J. He, J. Liu, Z. Yuan, and C.L. Chen and E.I. Meletis, “Two-dimensional Modulated Interfacial Structures of Highly Epitaxial Ferromagnetic (La,Ca)MnO3 and Ferroelectric (Pb,Sr)TiO3 Thin Films on (001) MgO”, Journal of Nano Research 3, 59-66 (2008).

[2]J.C. Jiang, Z. Yuan, C.L. Chen and E.I. Meletis, “Interface Modulated Structure of Highly Epitaxial (Pb,Sr)TiO3 Thin Films on (001) MgO”, Applied Physics Letters 90, 051904 (2007).

[3]B. J. Spencer, P. W. Voohees, and S. H. Davis, “Morphological Instability in Epitaxially Strained Dislocation-Free Solid Films: Linear Stability Theory”, Journal of Applied Physics 73, 4955 (1993).

[4]A.A. Golovin, M.S. Levine, T.V. Savina, and S. H. Davis, “Faceting Instability in the Presence of Wetting Interactions: A Mechanism for the Formation of Quantum Dots”, Physical Review B 70, 235342 (2004).

[5]F. Shi, P. Sharma, D.J. Kouri, F. Hussain, and G.H. Gunaratne, “Nanostructures with Long-Range Order in Monolayer Self-Assembly”, Physical Review E 78, 025203 (2008).

Figure 1. XTEM image of epitaxial (La,Sr)MnO3 continuous film (a) and nanopillars (b) on (001) LaAlO3 substrate. (c) Plan-view TEM of epitaxial (La,Sr)MnO3 nanopillars.

Figure 2. Ordered quantum-dot array.

Figure 3. XTEM image of twin-coupled structure on epitaxial Ba(Zr,Ti)O3 film on (001) MgO substrate. (a) bright-field image, (b), (c) and (d) dark-field images showing presence of BZT epilayer and two twins, (e) schematic illustration showing coexistence of the twins with the epilayer, (f) hysteresis loop measurement of BZT film exhibiting interesting abnormal properties due to the formation of the twins in the films.