Photonic crystals in biology
Photonic crystals in biology
Photonic crystals in biology
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Poster Session, Tuesday, June 15<br />
Theme A1 - B702<br />
Synthesis and Characterization of Electrospun Ba 0.6 Sr 0.4 TiO 3 Nanofibers and 3-3 Nanocomposites<br />
Yahya Toprak, 1 Ebru Menur Alkoy 2 and Sedat Alkoy 1,*<br />
1 Department of Materials Science and Eng<strong>in</strong>eer<strong>in</strong>g, Gebze Institute of Technology, Kocaeli 41400, Turkey<br />
2 Faculty of Eng<strong>in</strong>eer<strong>in</strong>g, Maltepe University, Istanbul 34857, Turkey<br />
Abstract— Barium strontium titanate – Ba 0.6 Sr 0.4 TiO 3 (BST) nanofibers with diameters of 50–200 nm were prepared<br />
us<strong>in</strong>g electrospun BST/polyv<strong>in</strong>ylpyrrolidone (PVP) fibers by calc<strong>in</strong>ation for 1 h at temperatures <strong>in</strong> the range of 650–800ºC<br />
<strong>in</strong> air. The morphology and crystal structure of calc<strong>in</strong>ed BST/PVP nanofibers were characterized us<strong>in</strong>g SEM and XRD.<br />
Nanocomposites with 3-3 phase connectivity were prepared by <strong>in</strong>filtrat<strong>in</strong>g an epoxy matrix phase <strong>in</strong>to the nanofiber mats.<br />
Dielectric properties of the BST/epoxy nanocomposites were evaluated for tunable microwave dielelectric applications.<br />
BST powders were also prepared by gelation and dry<strong>in</strong>g of BST precursor sol-gel solutions. Dried gels were then<br />
calc<strong>in</strong>ed, ground, pressed and s<strong>in</strong>tered to obta<strong>in</strong> dense BST ceramics. Electrical properties of BST ceramics were<br />
determ<strong>in</strong>ed through dielectric and PE hysteresis measurements.<br />
Barium strontium titanate - Ba 1x Sr x TiO 3 (BST) is a<br />
perovskite type material with a ferroelectric-paraelectric<br />
transition temperature that can be tuned from 30 to 400 K by<br />
vary<strong>in</strong>g the Ba/Sr ratio [1]. Solid solutions with x = 0.2 to<br />
0.5 are normally used to shift the transition temperature to,<br />
or just below, room temperature. BST solid solutions have<br />
unique comb<strong>in</strong>ation of large dielectric constant, high<br />
tunability, low dc leakage, low loss tangent, and stable<br />
operation at high temperature [2]. With this comb<strong>in</strong>ation of<br />
favorable properties, BST f<strong>in</strong>ds niche <strong>in</strong> tunable microwave<br />
devices such as microwave tunable phase shifters, tunable<br />
filters, and high-Q resonators for radar and communication<br />
applications [3]. Fiberization of the functional ceramics<br />
expand their utility <strong>in</strong>to the micro and nanodevices, and<br />
<strong>in</strong>corporation of these fibers <strong>in</strong>to composite structures<br />
provides an added flexibility and mechanical <strong>in</strong>tegrity [4].<br />
Electrosp<strong>in</strong>n<strong>in</strong>g represents a simple and versatile method for<br />
prepar<strong>in</strong>g ceramic fibers <strong>in</strong> the nanoscale range [5].<br />
In the preparation of BST precursor sol-gel solution<br />
barium acetate, strontium acetate and titanium isopropoxide<br />
were used as source materials. A mixture of acetic acid and<br />
2-methoxyethanol with 1:2 mix ratio was used as solvent.<br />
Poly(v<strong>in</strong>ylpyrrolidone) (PVP) was used as the carrier<br />
polymer. The Ba:Sr molar ratio was 0.6:0.4 and the molarity<br />
of the f<strong>in</strong>al precursor solution was 0.27 M. Various PVP<br />
additions from 5 to 30 wt% were studied. The electric field<br />
dur<strong>in</strong>g the electrosp<strong>in</strong>n<strong>in</strong>g process was varied from 10 to 20<br />
kV/cm and the pump<strong>in</strong>g rate from 1 to 5 l/h.<br />
Electrospun BST/polyv<strong>in</strong>ylpyrrolidone (PVP) fibers were<br />
obta<strong>in</strong>d by calc<strong>in</strong>ation for 1 h at temperatures <strong>in</strong> the range of<br />
650–800ºC <strong>in</strong> air. The morphology and crystal structure of<br />
calc<strong>in</strong>ed BST/PVP nanofibers were characterized us<strong>in</strong>g<br />
SEM and XRD. Nanocomposites with 3-3 phase<br />
connectivity were prepared by <strong>in</strong>filtrat<strong>in</strong>g an epoxy matrix<br />
phase <strong>in</strong>to the nanofiber mats. Dielectric properties of the<br />
BST/epoxy nanocomposites were evaluated for tunable<br />
microwave dielelectric applications. BST powders were<br />
also prepared by gelation and dry<strong>in</strong>g of BST precursor solgel<br />
solutions. Dried gels were then calc<strong>in</strong>ed, ground, pressed<br />
and s<strong>in</strong>tered to obta<strong>in</strong> dense BST ceramics. Electrical<br />
properties of BST ceramics were determ<strong>in</strong>ed through<br />
dielectric and PE hysteresis measurements.<br />
X-ray diffraction patterns presented <strong>in</strong> Fig. 1 for calc<strong>in</strong>ed<br />
BST powders <strong>in</strong>dicate that a calc<strong>in</strong>ation temperature of<br />
700ºC was enough to obta<strong>in</strong> pure BST phase with perovskite<br />
structure. The scann<strong>in</strong>g electron micrograph shown <strong>in</strong> Fig.<br />
2 <strong>in</strong>dicates that nanofibers with diameters rang<strong>in</strong>g from 50<br />
to 200 nm can be obta<strong>in</strong>ed without the formation of<br />
undesired beads.<br />
Figure 1. XRD pattern of BST powders calc<strong>in</strong>ed at 700ºC-1 h.<br />
Figure 2. SEM micrograph of the as deposited BST/PVP<br />
nanofibers.<br />
The dielectric constant of the bulk BST ceramic pellets<br />
were as high as 2000 with a dielectric loss of less than 2%<br />
measured at room temperature at 100 kHz. The polarization<br />
vs. electric field hysteresis loops <strong>in</strong>dicates a ferroelectric<br />
behavior with a remnant polarization of 5 C/cm 2 and a<br />
coercive field of 15 kV/cm measured under an electric field<br />
of 50 kV/cm.<br />
*Correspond<strong>in</strong>g author: sedal@gyte.edu.tr<br />
[1] K.V. Saravanan et al., Mater. Chem. Phy. 105, 426 (2007).<br />
[2] S. Maensiri et al., J. Colloid Interface Sci. 297, 578 (2006).<br />
[3] D.Y. Lee et al., J Sol-Gel Sci Technol 53, 43 (2010).<br />
[4] E.M Alkoy et al., J. Amer. Ceram. Soc. 92, 2566 (2009).<br />
[5] R. Ramaseshan et al., J. Appl. Phys. 102, 111101 (2007).<br />
6th Nanoscience and Nanotechnology Conference, zmir, 2010 328