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Photonic crystals in biology

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Poster Session, Tuesday, June 15<br />

Theme A1 - B702<br />

Formation of Thermoelectric Nanos tructures by2T Electroche mical Atom-by-atom Codeposition<br />

Ümit Demir 1 *<br />

1 Department of Chemistry, Atatürk University, Erzurum 25240, Turkey<br />

Abstract-Nanostructures of Bi 2 Te 3 , Sb 2 Te 3 and PbS were electrodeposited us<strong>in</strong>g a novel and p ractical electrochemical method, based on<br />

simultaneous underpotential deposition of precursors of target compound from the same solution at a constant potential. These nanostructures<br />

are characterized by X-ray diffraction (XRD), atomic force microscopy (AFM), energy dispersive spectroscopy (EDS) and reflection<br />

absorption-FTIR (RA-FTIR) to determ<strong>in</strong>e structure, morphology, composition and optic properties.<br />

Synthesis of nanomaterials with controlled size, shape and<br />

crystalographic orientation has become an important issue <strong>in</strong><br />

material science research. S<strong>in</strong>ce the properties of<br />

semiconductor nano<strong>crystals</strong>, which possess many novel<br />

properties that differ considerably from those of the bulk [1,2],<br />

depend both on dimension and superlattice structure.<br />

Therefore, the development of synthetic methods that enable<br />

their precise control is expected to have a significant impact<br />

on progress. Bi2Te 3 and Sb 2 Te 3 with a narrow band gap and<br />

other V-VI group semiconductors are best-known materials<br />

for TE applications at room temperature and are widely used<br />

for thermoelectric (TE), biomedical and optoelectronic<br />

applications as heat pumps, power generations, solid state<br />

refrigeration, cool<strong>in</strong>g IC chips, biochips, <strong>in</strong>frared sensors,<br />

optoelectronic sensors, photo detectors, and so on. Recently,<br />

we have developed a new electrochemical process, based on<br />

co-deposition from the same solution at the upd of the<br />

precursors of the target compound, which have been used for<br />

the electrochemical deposition of PbS, PbTe, ZnS, and CdS <strong>in</strong><br />

the s<strong>in</strong>gle crystal form [3-6]. The appropriate<br />

electrodeposition potentials based on the underpotential<br />

deposition potentials (upd) of precursors have been<br />

determ<strong>in</strong>ed by the cyclic voltammetric measurements. In the<br />

present study, we illustrated the detailed growth process of<br />

Bi 2 Te 3 and Sb 2 Te 3 [7] nano films and Bi 2 Te 3 nanorodstructured<br />

films on s<strong>in</strong>gle crystall<strong>in</strong>e Au(111) electrodes by<br />

us<strong>in</strong>g Atomic Force Microscopy (AFM), X-ray Diffraction<br />

(XRD), Electron Dispersive Spectroscopy (EDS), and UV-v is-<br />

NIR Spectroscopy techniques. We found out that that the<br />

growth direction (orientation) and thickness of nanostructured<br />

Bi 2 TeR 3 can be readily controlled by pH, composition of the<br />

solution, and the time of the electrodeposition.<br />

The morphological <strong>in</strong>vestigation of Bi2Te 3 nanostructures<br />

revealed that the film growth follows 3D and 2D nucleation<br />

and growth mechanism <strong>in</strong> acidic and basic solutions, result<strong>in</strong>g<br />

<strong>in</strong> nanofilms and nanowires, respectively. XRD results show<br />

that s<strong>in</strong>gle crystall<strong>in</strong>e nanostructures of Bi2Te 3 are highly<br />

preferentially orientated along the (015) for nanofilms and<br />

(110) for nanowires. The growth of Sb 2 Te 3 nanofilms follows<br />

the nucleation and three-dimensional (3D) growth mechanism<br />

result<strong>in</strong>g <strong>in</strong> high crystall<strong>in</strong>e films of Sb 2 Te 3 (110) <strong>in</strong><br />

hexagonal structure, which were grown at a k<strong>in</strong>etically<br />

preferred orientation at (110) on Au (111). Highly strong<br />

quantum conf<strong>in</strong>ement effect, for both Sb 2 Te 3 and Bi 2 Te 3<br />

nanostructures, was observed.<br />

Figure 1. Bi 2 Te 3 nanostructures; (a) nanofilm, (b) nanowires<br />

Figure 2. Nanostructures of Sb 2 Te 3 (a) and PbS (b)<br />

Moreover, we applied a new modified electrochemical<br />

method [8] to deposit nanostructure of PbS on a thiol modified<br />

Au(111) surfaces. Electrochemical deposition was carried out<br />

after the stripp<strong>in</strong>g of thiol from the surface at different<br />

potential pulses. We showed that the size of the PbS<br />

nanostructures could be controlled by the electrochemical<br />

deposition time and pulse width.<br />

In summary, structural and morphological studies <strong>in</strong>dicate<br />

that growth of these nanostructures follows atom by atom<br />

growth mechanism result<strong>in</strong>g <strong>in</strong> highly crystall<strong>in</strong>e<br />

nanostructures grown at a k<strong>in</strong>etically preferred orientation.<br />

Absorption measurements as a function of thicknesses<br />

<strong>in</strong>dicated that the band gap of the nanostructures <strong>in</strong>crease as<br />

the thickness decreases.<br />

This study was supported by Atatürk University<br />

[1] E. Ronsencher, A. Fiore, B. V<strong>in</strong>ter, V. Berger, P.Bois, J. Nagle,<br />

Science 271, 168 (1996).<br />

[2] S.Yanagida, M.Yooshiya, T.Shiragami, C. Pac, H. Mori, H.<br />

Fujita, J. Phys. Chem. 94, 3104 (1990).<br />

[3] T. Öznülüer, Ü. Demir, Chem. M ater. 17,<br />

935 (2005).<br />

Langmuir 22, 4415 (2006).<br />

[5] M. Ü. Demir, J. Phys. Chem. C 111,<br />

2670 (2007).<br />

[6] T. Öznülüer, F. Bülbül, Ü. Demir, Th<strong>in</strong> Solid Films<br />

517, 5419 (2009).<br />

J. Electroanal. Chem. 633, 253 (2009).<br />

<br />

54, 6554 (2009).<br />

6th Nanoscience and Nanotechnology Conference, zmir, 2010 367

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