Abstract:We report on the synthesis of PbTiO3–CoFe2O4 multiferroic nanocomposites and continuous tuning of their ferroelectric and magnetic properties as a function of the average composition on thin-film composition spreads. The highest dielectric constant and nonlinear dielectric signal was observed at (PbTiO3)85–(CoFe2O4)15, where robust magnetism was also observed. Transmission electron microscopy revealed a pancake-shaped epitaxial nanostructure of PbTiO3 on the order of 30 nm embedded in the matrix of CoFe2O4 at … Show more
“…97 Among different types of multiferroic materials, nanocomposite materials have been well studied, since they have the potential to realize RT device operation due to cross coupled ferroelectric/ ferromagnetic properties. To study the formation of nanocomposite multiferroic thin films, PLD based CCS libraries were designed to directly probe continuous "mixing" of a ferroelectric material and a ferromagnetic material on an MgO (100) substrate, 98 Fig . 25.…”
Section: Ferroelectric Piezoelectric and Multiferroic Materialsmentioning
High throughput (combinatorial) materials science methodology is a relatively new research paradigm that offers the promise of rapid and efficient materials screening, optimization, and discovery. The paradigm started in the pharmaceutical industry but was rapidly adopted to accelerate materials research in a wide variety of areas. High throughput experiments are characterized by synthesis of a "library" sample that contains the materials variation of interest (typically composition), and rapid and localized measurement schemes that result in massive data sets. Because the data are collected at the same time on the same "library" sample, they can be highly uniform with respect to fixed processing parameters. This article critically reviews the literature pertaining to applications of combinatorial materials science for electronic, magnetic, optical, and energy-related materials. It is expected that high throughput methodologies will facilitate commercialization of novel materials for these critically important applications. Despite the overwhelming evidence presented in this paper that high throughput studies can effectively inform commercial practice, in our perception, it remains an underutilized research and development tool. Part of this perception may be due to the inaccessibility of proprietary industrial research and development practices, but clearly the initial cost and availability of high throughput laboratory equipment plays a role. Combinatorial materials science has traditionally been focused on materials discovery, screening, and optimization to combat the extremely high cost and long development times for new materials and their introduction into commerce. Going forward, combinatorial materials science will also be driven by other needs such as materials substitution and experimental verification of materials properties predicted by modeling and simulation, which have recently received much attention with the advent of the Materials Genome Initiative. Thus, the challenge for combinatorial methodology will be the effective coupling of synthesis, characterization and theory, and the ability to rapidly manage large amounts of data in a variety of formats. V C 2013 AIP Publishing LLC. [http://dx
“…97 Among different types of multiferroic materials, nanocomposite materials have been well studied, since they have the potential to realize RT device operation due to cross coupled ferroelectric/ ferromagnetic properties. To study the formation of nanocomposite multiferroic thin films, PLD based CCS libraries were designed to directly probe continuous "mixing" of a ferroelectric material and a ferromagnetic material on an MgO (100) substrate, 98 Fig . 25.…”
Section: Ferroelectric Piezoelectric and Multiferroic Materialsmentioning
High throughput (combinatorial) materials science methodology is a relatively new research paradigm that offers the promise of rapid and efficient materials screening, optimization, and discovery. The paradigm started in the pharmaceutical industry but was rapidly adopted to accelerate materials research in a wide variety of areas. High throughput experiments are characterized by synthesis of a "library" sample that contains the materials variation of interest (typically composition), and rapid and localized measurement schemes that result in massive data sets. Because the data are collected at the same time on the same "library" sample, they can be highly uniform with respect to fixed processing parameters. This article critically reviews the literature pertaining to applications of combinatorial materials science for electronic, magnetic, optical, and energy-related materials. It is expected that high throughput methodologies will facilitate commercialization of novel materials for these critically important applications. Despite the overwhelming evidence presented in this paper that high throughput studies can effectively inform commercial practice, in our perception, it remains an underutilized research and development tool. Part of this perception may be due to the inaccessibility of proprietary industrial research and development practices, but clearly the initial cost and availability of high throughput laboratory equipment plays a role. Combinatorial materials science has traditionally been focused on materials discovery, screening, and optimization to combat the extremely high cost and long development times for new materials and their introduction into commerce. Going forward, combinatorial materials science will also be driven by other needs such as materials substitution and experimental verification of materials properties predicted by modeling and simulation, which have recently received much attention with the advent of the Materials Genome Initiative. Thus, the challenge for combinatorial methodology will be the effective coupling of synthesis, characterization and theory, and the ability to rapidly manage large amounts of data in a variety of formats. V C 2013 AIP Publishing LLC. [http://dx
“…[5][6][7][8][9][10] Through a strictive interaction between the piezoelectricity of the ferroelectric ͑FE͒ phase and the magnetostriction of the ferromagnetic ͑FM͒ phase, said composites are capable of producing relatively large ME coefficients. The most widely studied phase connectivities for twophase ME composite films are ͑i͒ a ͑2-2͒ layer-by-layer structure [11][12][13][14][15][16][17][18] and ͑ii͒ a ͑0-3͒ structure of second phase particles embedded in a primary matrix phase. 19,12,[20][21][22][23] In addition, ͑1-3͒ self-assembled ME composite thin films consisting of FE ͓or ͑FM͔͒ nanopillars embedded in a FM ͑or FE͒ matrix was first reported in 2004.…”
Section: Introductionmentioning
confidence: 99%
“…The most widely studied phase connectivities for twophase ME composite films are ͑i͒ a ͑2-2͒ layer-by-layer structure [11][12][13][14][15][16][17][18] and ͑ii͒ a ͑0-3͒ structure of second phase particles embedded in a primary matrix phase. 19,12,[20][21][22][23] In addition, ͑1-3͒ self-assembled ME composite thin films consisting of FE ͓or ͑FM͔͒ nanopillars embedded in a FM ͑or FE͒ matrix was first reported in 2004. 24 Self-assembled epitaxial BiFeO 3 -CoFe 2 O 4 ͑BFO-CFO͒ nanocomposite thin films deposited on differently oriented substrates are known to have different types of nanostructures.…”
We report the ferroelectric, ferromagnetic, and magnetoelectric ͑ME͒ properties of self-assembled epitaxial BiFeO 3 -CoFe 2 O 4 ͑BFO-CFO͒ nanostructure composite thin films deposited on ͑001͒, ͑110͒, and ͑111͒ SrTiO 3 ͑STO͒ single crystal substrates. These various properties are shown to depend on orientation. The maximum values of the relative dielectric constant, saturation polarization, longitudinal piezoelectric coefficient, saturation magnetization, and ME coefficient at room temperature were 143, 86 m / cm 2 , 50 pm/V, 400 emu/cc, and 20 mV/ cm Oe, respectively.
“…8 Zheng et al 9 deposited epitaxial two phase films that self-assembled into nanopillars of CoFe 2 O 4 ͑CFO͒ in a BaTiO 3 ͑BTO͒ matrix. For two-phase multiferroic thin films, not only have such ͑1-3͒ and ͑3-1͒ structures ͑i.e., nanopillars in a second phase matrix͒ been reported, [9][10][11][12][13][14][15][16][17] but many other types of structures with different phase interconnectives have also, such as ͑0-3͒ nanoparticles dispersed in a matrix [18][19][20][21][22] and ͑2-2͒ mutilayer two-phase composite thin films. 23,24 Theoretically, the ͑1-3͒ structure should be the best type for ME coupling in epitaxial films.…”
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