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Endo Tamio. - Correlated Functional Oxides: Nanocomposites and Heterostructures

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Endo Tamio. Correlated Functional Oxides: Nanocomposites and Heterostructures

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This book introduces a variety of basic sciences and applications of the nanocomposites and heterostructures of functional oxides. The presence of a high density of interfaces and the differences in their natures are described by the authors. Both nanocomposites and heterostructures are detailed in depth by researchers from each of the research areas in order to compare their similarities and differences. A new interfacial material of heterostructure of strongly correlated electron systems is introduced.;Functional Iron Oxides and Their Heterostructures -- Functional Properties of Polydomain Ferroelectric Oxide Thin Films -- Stress Accommodation and Structural Distortions at Correlated Oxide Interface -- The Influence of Different Additives on MgB2 Superconductor Obtained by ex-situ Spark Plasma Sintering: Pinning Force Aspects -- Infrared Spectra in Oxide Nanocomposites/Minerals -- Self-Assembled Nanocomposite Oxide Films -- Functionality in Insulating Oxide Thin Films: Work Function Control and Polar Surface -- Material Design of Metal Oxide Nanowires and Their Promises -- Atomic Processes of Pulsed Laser Deposition During Growth of Alkaline Earth Oxide Thin Films.

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Springer International Publishing AG 2017
Hiroaki Nishikawa , Nobuyuki Iwata , Tamio Endo , Yayoi Takamura , Gun-Hwan Lee and Paolo Mele (eds.) Correlated Functional Oxides 10.1007/978-3-319-43779-8_1
1. Functional Iron Oxides and Their Heterostructures
Munetoshi Seki 1 and Hitoshi Tabata 1
(1)
Department of Electrical Engineering and Information Systems, Graduate School of Engineering, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku 113-8656, Tokyo, Japan
Munetoshi Seki
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Abstract
Iron oxides, which are also called ferrites, have been known to humans since ancient times and have been the subject of intensive research activity from fundamental as well as practical perspectives for a long time. One of the most advantageous properties of iron oxides is that they are chemically stable and nontoxic. In addition, Fe and O are earth-abundant elements [high Clarke numbers for Fe (4.7) and O (49.5)]. These features mean that the ferrites are suitable for applications in low cost, environmentally-friendly electronics. In this chapter, we examine some of the functional iron oxides and their heterostructures. First, we focus on the growth of FeO (wstite) epitaxial thin films, and their properties as p -type transparent semiconductors will be discussed. Next, we will consider -Fe2O3 (hematite), which is well known as the main component of red rust. It is demonstrated that band engineering and control of the crystal growth direction of -Fe2O3 are useful to enhance its photoelectrochemical properties for high efficiency water splitting using sunlight. The third topic is Fe3O4 (magnetite), which is known to be a ferromagnetic oxide semiconductor. The control of the carrier type in Fe3O4 and its possible application to spintronic devices will be discussed. Finally, we will focus on the spin-fluctuation system in iron oxides. The long-term potentiation with the photomemory effect is observed in a Si-substituted garnet ferrite with high temperature spin-glass-like properties, which mimics the pre- and post-synaptic potentials of biological systems.
Keywords
Iron oxides Magnetite Hematite Photoelectrochemical water splitting Oxide spintronics
1.1 Introduction
The challenge of developing a new material technology that can solve increasingly serious problems on a global scale, pertaining to the environment, energy, and resources, is being pursued actively. It is against such a backdrop that iron oxide , which is an inexhaustible resource that is nontoxic and offers a superior environmental affinity, is drawing much attention. Iron oxide has been used in a various devices, such as recording media to communication equipment. It is a representative magnetic material that has been supporting the development of modern industry from the ground up. The aspects of iron oxide responsible for its wide applicability are its high magnetic transition temperature (500 C and higher) and superior chemical stability. Most iron oxide materials currently being used in practical applications contain iron in the stable +3 valence state. Their localized spin allows for strong bond formation via oxygen ions (i.e. superexchange interaction) to achieve stable magnetic structure and magnetic field responsiveness, as well as high insulation, all of which are essential for practical applications. Transition metal oxides that contain iron oxide, on the other hand, feature an attractive characteristic of their electrical, magnetic, and optical properties varying significantly according to the valence of metal ions []. In iron oxides , the control of the valence states of Fe ions has been particularly difficult, and this has been a significant barrier for the progress of research and development in the application of new functional materials. This chapter describes the attempts made to control the valence of iron oxide using the film growth technique based on pulsed laser deposition (PLD). A variety of iron oxide thin films fabricated using these methods are then explored for their potentials as functional materials.
1.2 FeO: Transparent P-Type Oxide Semiconductor
Iron oxides are known to exhibit a wide range of physical properties and crystal structures. For example, multifunctional bismuth ferrite (BiFeO3) has been attracted considerable owing to its numerous promising applications in multiferroic and photovoltaic devices [].
Fig 11 Basic iron oxides with different valence state of Fe ions in the - photo 1
Fig. 1.1
Basic iron oxides with different valence state of Fe ions in the electron conduction path and their physical properties. Images and crystal structures of these iron oxides are also shown
In this section, we focus on FeO thin films with a rock-salt crystal structure. FeO has attracted scientific interest over a long period because of its importance as a possible chemical component of the Earths core. Furthermore, FeO is currently a subject of intense investigation in a wide variety of research fields such as spintronics and chemical engineering []. Therefore, the extraction of the spinel phase may be suppressed by the substitution of Si in the film. In addition, the substitution of Si4+ in FeO enhances the [Fe2+]/[Fe3+] ionic ratio owing to charge neutrality, which is expected to improve the antioxidant properties of the films.
XRD patterns of the films prepared using PLD technique with Fe2O3SiO2 mixture target [] direction. In contrast to the FeO samples used in previous studies, no impurity phases such as Fe or Fe3O4 were observed in the XRD pattern of the Si:FeO film.
Fig 12 XRD patterns for the films grown on -Al2O3 001 by PLD using targets - photo 2
Fig. 1.2
XRD patterns for the films grown on -Al2O3 (001) by PLD using targets with Si/(Si + Fe) atomic rations of 0.00, 0.03, and 0.08. The second XRD pattern from the top is for the film annealed in air at 800 C for 3 h. C, S, and R denote the XRD peaks of the corundum, spinel, and rock-salt phases, respectively. The crystal structures of the films are illustrated next to the XRD patterns
Figure ]
11 where b g is the so-called bowing parameter and E gFSMO E gMgO - photo 3
(1.1)
where b g is the so-called bowing parameter and E g(FSMO), E g(MgO), and E g(Si:FeO) are the bandgaps of FSMO, MgO, and Si:FeO, respectively. The dependence of the optical bandgap on the MgO fraction is well fitted with b g = 6.7 eV, as shown in Fig. ] and hence may be responsible for the large bandgap bowing in the FSMO films.
Fig 13 a Optical transmittance spectra of the -Fe2O3 SiFe3O4 and SiFeO - photo 4
Fig. 1.3
a Optical transmittance spectra of the -Fe2O3, Si:Fe3O4, and Si:FeO films. Inset shows the enlarged spectra. b Tauc plots for MgO-Si:FeO solid solution thin films ( left ) and images of the films ( x = 0.1, 0.3, 0.5, and 0.9; right ). c Bandgap energy of MgOSi:FeO solid solution thin films as a function of MgO fraction x
Figure c), and hence presumably reflects the bowing of the valence band. In general, the limited conductivity of p -type wide-gap oxides has been the main difficulty in electrode and hole injection applications. The conductivity of the FSMO films is 0.17.8 S/cm at 300 K without the intentional doping of acceptors, which is significantly higher than that of most nondoped p -type wide-gap semiconducting oxides. In addition, note that the elements constituting the film (i.e., Fe, Si, and Mg) are abundant in the Earths crust, which means that the FSMO film is feasible for application in low cost and environmentally-friendly electronics.
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