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Photonic crystals in biology

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Poster Session, Tuesday, June 15<br />

Theme A1 - B702<br />

Preparation and Characterization of Nanostructured ZnS Th<strong>in</strong> Films Grown on Glass and<br />

Monocrystall<strong>in</strong>e Si Substrates<br />

R. Sahraei 1* , G. Nabiyouni 2 and A. Daneshfar 1<br />

1 Department of Chemistry, University of Ilam, Ilam P.O. Box: 65315-516, Iran<br />

2 Department of Physics, University of Arak, Arak, Iran<br />

Abstract— Nanocrystall<strong>in</strong>e z<strong>in</strong>c sulfide th<strong>in</strong> films were prepared by a new chemical bath deposition technique onto glass and<br />

silicon (111) substrates. Deposition takes place at a temperature of 70 ºC and a pH of 6.0, from an aqueous solution conta<strong>in</strong><strong>in</strong>g<br />

z<strong>in</strong>c acetate, thioacetamide, and ethylenediam<strong>in</strong>e. Microstructure analysis us<strong>in</strong>g atomic force microscopy shows that the films<br />

deposited on glass substrates conta<strong>in</strong> 28-30 nm clusters, whereas much larger clusters (around 80-120 nm) comprise the films<br />

deposited on silicon (111) substrate. X-ray diffraction analysis <strong>in</strong>dicates that both the ZnS films deposited on glass and Si<br />

substrates have cubic z<strong>in</strong>cblende structure. Direct band gap energy for these samples was measured to be <strong>in</strong> the range of 3.97-<br />

4.00 eV.<br />

Recently, the II-VI compounds semiconductor th<strong>in</strong> films<br />

have received an <strong>in</strong>tensive attention due to their application <strong>in</strong><br />

th<strong>in</strong> film solar cells [1]. Among these metal chalcogenides,<br />

ZnS is an important semiconductor material because of its<br />

broad direct band gap energy (~3.6 eV) at room temperature<br />

[2]. Various techniques have been employed to fabricate ZnS<br />

th<strong>in</strong> films, such as, electrodeposition, pulsed-laser deposition,<br />

chemical vapor deposition (CVD), and chemical bath<br />

deposition (CBD) [3, 4].<br />

In this work, we report deposition of nanocrystall<strong>in</strong>e z<strong>in</strong>c<br />

sulfide th<strong>in</strong> films on the glass and mono-crystall<strong>in</strong>e Si<br />

substrates us<strong>in</strong>g a weak acidic bath <strong>in</strong> which ethylenediam<strong>in</strong>e<br />

acts as a complex<strong>in</strong>g agent and thioacetamide acts as a source<br />

of sulfide ions. Atomic force microscopy (AFM), X-ray<br />

diffraction (XRD), and UV-Vis spectrophotometery are used<br />

to <strong>in</strong>vestigate the surface morphology, structural, and optical<br />

properties of the nanostructured ZnS th<strong>in</strong> films. We show how<br />

the morphology and surface roughness of the ZnS th<strong>in</strong> films<br />

depend on the substrate type.<br />

Figure 1. AFM images (two- dimensional (2D)) of CBD ZnS th<strong>in</strong> films<br />

on (a) Si and glass substrate (b).<br />

X-ray diffraction patterns of the ZnS film grown on glass<br />

and monocrystall<strong>in</strong>e Si substrate show three dist<strong>in</strong>guished<br />

peaks at the angles of 28.6º, 47.7º and 56.5º reveal a cubic<br />

lattice structure and can be assigned to the (111), (220), and<br />

(311) plans, respectively. Broaden<strong>in</strong>g of diffraction peaks <strong>in</strong><br />

the XRD pattern of the ZnS film is attributed to the<br />

nanometer-sized crystallites. The calculated average size of<br />

nanocrystallites, us<strong>in</strong>g Scherrer equation is found to be about<br />

4.5 and 8 nm for the ZnS films deposited on glass and s<strong>in</strong>gle<br />

crystal Si substrates, respectively.<br />

The average transmittance of ZnS films is calculated to be<br />

84%, 78%, 74% and 71%, respectively, <strong>in</strong> the visible<br />

wavelength region. As it is clear from spectra the films have a<br />

steep optical absorption feature, <strong>in</strong>dicat<strong>in</strong>g good homogeneity<br />

<strong>in</strong> the shape and size of the nanocrystallites and low defect<br />

density near the band edge [5]. The band gap energy (E g ) was<br />

determ<strong>in</strong>ed to be <strong>in</strong> the range of 3.97-4.00 eV for the ZnS<br />

films with deposition times vary<strong>in</strong>g from 4 to 16 hours. These<br />

values are rather larger than the literature value for the bulk<br />

ZnS (~ 3.6 eV). The result could be attributed to the quantum<br />

size effects as expected from the nanocrystall<strong>in</strong>e nature of the<br />

ZnS th<strong>in</strong> films [6, 7].<br />

Figure 1 (a) and (b) illustrates two-dimensional AFM<br />

images of the ZnS th<strong>in</strong> films deposited on monocrystall<strong>in</strong>e Si<br />

and commercial glass slide substrates, respectively. The th<strong>in</strong><br />

film deposited on Si substrate is made of aggregates (clusters)<br />

with a square-like surface morphology, whereas much f<strong>in</strong>er<br />

aggregates with an isosceles triangular surface morphology<br />

comprise the film deposited on glass substrate. As can be seen,<br />

the films deposited on the glass substrate conta<strong>in</strong> smaller<br />

clusters (average gra<strong>in</strong> size of around 28-30 nm <strong>in</strong> diameter)<br />

and have more surface aggregates than those deposited on Si<br />

substrate (average gra<strong>in</strong> size of around 80-120 nm <strong>in</strong><br />

diameter).<br />

In summary, we have successfully deposited the<br />

nanocrystall<strong>in</strong>e ZnS th<strong>in</strong> films onto glass and monocrystall<strong>in</strong>e<br />

Si substrates, from a chemical bath at temperature of 70 °C,<br />

and us<strong>in</strong>g ethylenediam<strong>in</strong> as a complex<strong>in</strong>g agent. The XRD<br />

measurements <strong>in</strong>dicate that the structure of the ZnS th<strong>in</strong> films<br />

is cubic. In our experiment, based on the optical transmission<br />

measurements, the band gap energies are calculated to be<br />

between 3.97-4.00 eV for the ZnS films with different<br />

thicknesses. Morphology and optical properties of the ZnS<br />

films were characterized us<strong>in</strong>g AFM and UV-Visible<br />

spectroscopy.<br />

*Correspond<strong>in</strong>g author: reza_sahrai@yahoo.com<br />

[1] M. Bär, A. Ennaoui, J. Klaer, R. Sáez-Araoz, T. Kropp, L. We<strong>in</strong>hardt, C.<br />

Heske, H.-W. Schock, Ch.-H. Fischer, M.C. Lux-Ste<strong>in</strong>er, Chem. Phys. Lett.<br />

433, 71 (2006).<br />

[2] J. Mu, Y. Zhang, Appl. Surf. Sci. 252, 7826 (2006).<br />

[3] R.S. Mane, and C.D. Lokhande, Mater. Chem. Phys. 65, 1 (2000).<br />

[4] A. Goudarzi, G. Motedayen Aval, S. S. Park, . Choi, R. Sahraei, M.Habib<br />

Ullah, A. Avane, and C. S. Ha, Chemistry of Materials 21, 2375 (2009).<br />

[5] C. Hubert, N. Naghavi, B. Canava, A. Etcheberry, and D. L<strong>in</strong>cot, Th<strong>in</strong><br />

Solid Films 515, 6032 (2007).<br />

[6] R. Sahraei, G. Motedayen Aval, A. Baghizadeh, M. Lamehi-Rachti, A.<br />

Goudarzi, M. H. Majles Ara, Materials Letters 62, 4345 (2008).<br />

[7] K. Yamaguchi, T. Yoshida, D. L<strong>in</strong>cot, H. M<strong>in</strong>oura, J. Phys. Chem. B 107,<br />

387 (2003).<br />

6th Nanoscience and Nanotechnology Conference, zmir, 2010 352

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