8 research outputs found
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
Inhibition of Neurofilament and Shank2 Expression by Bevacizumab in Differentiated Retinoblastoma Cells.
<p>(A, B) SNUOT-Rb1 cells were treated with 0.1% BSA or 1 mg/ml bevacizumab. Neurofilament (A) and shank2 (B) were detected by Western blot analysis. β-actin was served as a loading control. Each figure is representative ones from three independent experiments. Quantitative analysis was performed by measuring protein expression relative to the controls. Each value represents means ± SE from three independent experiments (*P<0.05). BSA, bovine serum albumin. (C) SNUOT-Rb1 cells were treated with 0.1% BSA or 1 mg/ml bevacizumab. Neuronal differentiation was addressed by the morphological changes of neurite extensions. Immunocytochemistry for neurofilament (green) and shank2 (red) was performed, and nuclei were labeled with DAPI (blue). Each figure is representative ones from three independent experiments. Scale bar, 20 µm. DAPI, 4′, 6-diamidino-2-phenolindole. (D) SNUOT-Rb1 cells were treated with 0.1% BSA, 1 mg/ml human IgG, or 1 mg/ml bevacizumab. Neurite length in differentiated retinoblastoma cells was measured by manual tracing of neurite outgrowth in each cell. Quantitative analysis was performed using average length from total neurites measured. Each value represents means ± SE from three independent experiments (*P<0.05, **P>0.05). (E, F, G) Retinoblastoma cells of SNUOT-Rb1 (E) and Y79 (F, G) were treated with either 0.1% BSA or 1 mg/ml human IgG. Total mRNA was isolated from retinoblastoma cells, and reverse transcriptase-polymerase chain reaction was performed with specific primers for neurofilament or shank2. GAPDH was served as an internal control. Each figure is representative ones from three independent experiments. Quantitative analysis was performed by measuring mRNA expression relative to the control. Each value represents means ± SE from three independent experiments (*P<0.05, **P>0.05).</p
Bevacizumab-induced Inhibition of Differentiation of Retinoblastoma Cells through Blockade of ERK 1/2 Activation.
<p>SNUOT-Rb1 cells were treated with 0.1% BSA or 1 mg/ml bevacizumab. ERK 1/2, phospho-ERK 1/2, Akt, and phospho-Akt were detected by Western blot analysis. β-actin was served as a loading control. Each figure is representative ones from three independent experiments. Quantitative analysis was performed by measuring protein expression relative to the controls. Each value represents means ± SE from three independent experiments (*P<0.05, **P>0.05). BSA, bovine serum albumin.</p
Activation of TrkA Induced by VEGF in Retinoblastoma Cells.
<p>(A) Proteins of human retinoblastoma cell lines, Y79 and SNUOT-Rb1 <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0033456#pone.0033456-Kim5" target="_blank">[22]</a> as well as a human colorectal cancer cell lines, SW480 were resolved on 12% SDS-PAGE and western blot analysis was performed using anti-TrkA antibody. β-actin was served as a loading control. Each figure is representative ones from three independent experiments. (B) Proteins of Y79 and SNUOT-Rb1 cells were resolved on 12% SDS-PAGE and western blot analysis was performed using anti-VEGFR-2 and anti-TrkA antibody. β-actin was served as a loading control. Each figure is representative ones from three independent experiments. (C) SNUOT-Rb1 cells were treated with 10 ng/ml VEGF. TrkA and phospho-TrkA were detected by Western blot analysis. β-actin was served as a loading control. Each figure is representative ones from three independent experiments.</p
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
SrÂ(Ti<sub>1–<i>x</i></sub>M<sub><i>x</i></sub>)ÂO<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. SrÂ(Ti<sub>1–<i>x</i></sub>Fe<sub><i>x</i></sub>)ÂO<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 SrÂ(Ti<sub>1–<i>x</i></sub>Fe<sub><i>x</i></sub>)ÂO<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 SrÂ(Ti<sub>1–<i>x</i></sub>Fe<sub><i>x</i></sub>)ÂO<sub>3−δ</sub>. Films of SrÂ(Ti<sub>1–<i>x</i></sub>Cr<sub><i>x</i></sub>)ÂO<sub>3−δ</sub> and SrÂ(Ti<sub>1–<i>x</i></sub>Mn<sub><i>x</i></sub>)ÂO<sub>3−δ</sub> showed no room temperature ferromagnetism, but SrÂ(Ti<sub>1–<i>x</i></sub>Ni<sub><i>x</i></sub>)ÂO<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 Phase Formation in Self-Assembled Epitaxial BiFeO<sub>3</sub>–MgO and BiFeO<sub>3</sub>–MgAl<sub>2</sub>O<sub>4</sub> Nanocomposite Films Grown by Combinatorial Pulsed Laser Deposition
Self-assembled epitaxial BiFeO<sub>3</sub>–MgO and BiFeO<sub>3</sub>–MgAl<sub>2</sub>O<sub>4</sub> nanocomposite thin films
were grown on SrTiO<sub>3</sub> substrates by pulsed laser deposition.
A two-phase columnar structure was observed for BiFeO<sub>3</sub>–MgO
codeposition within a small window of growth parameters, in which
the pillars consisted of a magnetic spinel phase (Mg,Fe)<sub>3</sub>O<sub>4</sub> within a BiFeO<sub>3</sub> matrix, similar to the growth
of BiFeO<sub>3</sub>–MgFe<sub>2</sub>O<sub>4</sub> nanocomposites
reported elsewhere. Further, growth of a nanocomposite with BiFeO<sub>3</sub>–(CoFe<sub>2</sub>O<sub>4</sub>/MgO/MgFe<sub>2</sub>O<sub>4</sub>), in which the minority phase was grown from three
different targets, gave spinel pillars with a uniform (Mg,Fe,Co)<sub>3</sub>O<sub>4</sub> composition due to interdiffusion during growth,
with a bifurcated shape from the merger of neighboring pillars. BiFeO<sub>3</sub>–MgAl<sub>2</sub>O<sub>4</sub> did not form a well-defined
vertical nanocomposite in spite of having lower lattice mismatch,
but instead formed a two-phase film with in which the spinel phase
contained Fe. These results illustrate the redistribution of Fe between
the oxide phases during oxide codeposition to form a ferrimagnetic
phase from antiferromagnetic or nonmagnetic targets
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