5 research outputs found
Magnetostatic Interactions in Self-Assembled Co<sub><i>x</i></sub>Ni<sub>1–<i>x</i></sub>Fe<sub>2</sub>O<sub>4</sub>/BiFeO<sub>3</sub> Multiferroic Nanocomposites
Self-assembled
vertically aligned oxide nanocomposites consisting
of magnetic pillars embedded in a ferroelectric matrix have been proposed
for logic devices made from arrays of magnetostatically interacting
pillars. To control the ratio between the nearest neighbor interaction
field and the switching field of the pillars, the pillar composition
Co<sub><i>x</i></sub>Ni<sub>1–<i>x</i></sub>Fe<sub>2</sub>O<sub>4</sub> was varied over the range 0 ≤ <i>x</i> ≤ 1, which alters the magnetoelastic and magnetocrystalline
anisotropy and the saturation magnetization. Nanocomposites were templated
into square arrays of pillars in which the formation of a “checkerboard”
ground state after ac-demagnetization indicated dominant magnetostatic
interactions. The effect of switching field distribution in disrupting
the antiparallel nearest neighbor configuration was analyzed using
an Ising model and compared with experimental results
Multiferroic Behavior of Templated BiFeO<sub>3</sub>–CoFe<sub>2</sub>O<sub>4</sub> Self-Assembled Nanocomposites
Self-assembled BiFeO<sub>3</sub>–CoFe<sub>2</sub>O<sub>4</sub> nanocomposites were templated into ordered structures
in which the
ferrimagnetic CoFe<sub>2</sub>O<sub>4</sub> pillars form square arrays
of periods 60–100 nm in a ferroelectric BiFeO<sub>3</sub> matrix.
The ferroelectricity, magnetism, conductivity, and magnetoelectric
coupling of the ordered nanocomposites were characterized by scanning
probe microscopy. The insulating BiFeO<sub>3</sub> matrix exhibited
ferroelectric domains, whereas the resistive CoFe<sub>2</sub>O<sub>4</sub> pillars exhibited single-domain magnetic contrast with high
anisotropy due to the magnetoelasticity of the spinel phase. Magnetoelectric
coupling was observed in which an applied voltage led to reversal
of the magnetic pillars
Combinatorial Pulsed Laser Deposition of Fe, Cr, Mn, and Ni-Substituted SrTiO<sub>3</sub> Films on Si Substrates
Combinatorial pulsed laser deposition (CPLD) using two
targets
was used to produce a range of transition metal-substituted perovskite-structured
Sr(Ti<sub>1–<i>x</i></sub>M<sub><i>x</i></sub>)O<sub>3−δ</sub> films on buffered silicon substrates,
where M = Fe, Cr, Ni and Mn and <i>x</i> = 0.05–0.5.
CPLD produced samples whose composition vs distance fitted a linear
combination of the compositions of the two targets. Sr(Ti<sub>1–<i>x</i></sub>Fe<sub><i>x</i></sub>)O<sub>3−δ</sub> films produced from a pair of perovskite targets (SrTiO<sub>3</sub> and SrFeO<sub>3</sub> or SrTiO<sub>3</sub> and SrTi0<sub>0.575</sub>Fe<sub>0.425</sub>O<sub>3</sub>) had properties similar to those
of films produced from single targets, showing a single phase microstructure,
a saturation magnetization of 0.5 μ<sub>B</sub>/Fe, and a strong
out-of-plane magnetoelastic anisotropy at room temperature. Films
produced from an SrTiO<sub>3</sub> and a metal oxide target consisted
of majority perovskite phases with additional metal oxide (or metal
in the case of Ni) phases. Films made from SrTiO<sub>3</sub> and Fe<sub>2</sub>O<sub>3</sub> targets retained the high magnetic anisotropy
of Sr(Ti<sub>1–<i>x</i></sub>Fe<sub><i>x</i></sub>)O<sub>3−δ</sub>, but had a much higher saturation
magnetization than single-target films, reaching for example an out-of-plane
coercivity of >2 kOe and a saturation magnetization of 125 emu/cm<sup>3</sup> at 24%Fe. This was attributed to the presence of maghemite
or magnetite exchange-coupled to the Sr(Ti<sub>1–<i>x</i></sub>Fe<sub><i>x</i></sub>)O<sub>3−δ</sub>. Films of Sr(Ti<sub>1–<i>x</i></sub>Cr<sub><i>x</i></sub>)O<sub>3−δ</sub> and Sr(Ti<sub>1–<i>x</i></sub>Mn<sub><i>x</i></sub>)O<sub>3−δ</sub> showed no room temperature ferromagnetism, but Sr(Ti<sub>1–<i>x</i></sub>Ni<sub><i>x</i></sub>)O<sub>3−δ</sub> did show a high anisotropy and magnetization attributed mainly to
the perovskite phase. Combinatorial synthesis is shown to be an efficient
process for enabling evaluation of the properties of epitaxial substituted
perovskite films as well as multiphase films which have potential
for a wide range of electronic, magnetic, optical, and catalytic applications
Magnetic and Photoluminescent Coupling in SrTi<sub>0.87</sub>Fe<sub>0.13</sub>O<sub>3−δ</sub>/ZnO Vertical Nanocomposite Films
Self-assembled
growth of SrTi<sub>0.87</sub>Fe<sub>0.13</sub>O<sub>3−δ</sub> (STF)/ZnO vertical nanocomposite films by combinatorial pulsed laser
deposition is described. The nanocomposite films form vertically aligned
columnar epitaxial nanostructures on SrTiO<sub>3</sub> substrates,
in which the STF shows room-temperature magnetism. The magnetic properties
are discussed in terms of strain states, oxygen vacancies, and microstructures.
The nanocomposites exhibit magneto-photoluminescent coupling behavior
that the near-band-edge emission of ZnO is shifted as a function of
magnetic field
Hierarchical Templating of a BiFeO<sub>3</sub>–CoFe<sub>2</sub>O<sub>4</sub> Multiferroic Nanocomposite by a Triblock Terpolymer Film
A process route to fabricate templated BiFeO<sub>3</sub>/CoFe<sub>2</sub>O<sub>4</sub> (BFO/CFO) vertical nanocomposites is presented in which the self-assembly of the BFO/CFO is guided using a self-assembled triblock terpolymer. A linear triblock terpolymer was selected instead of a diblock copolymer in order to produce a square-symmetry template, which had a period of 44 nm. The triblock terpolymer pattern was transferred to a (001) Nb:SrTiO<sub>3</sub> substrate to produce pits that formed preferential sites for the nucleation of CFO crystals, in contrast to the BFO, which wetted the flat regions of the substrate. The crystallographic orientation and magnetic properties of the templated BFO/CFO were characterized