<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">MSCE</journal-id><journal-title-group><journal-title>Journal of Materials Science and Chemical Engineering</journal-title></journal-title-group><issn pub-type="epub">2327-6045</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/msce.2014.212001</article-id><article-id pub-id-type="publisher-id">MSCE-52086</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject></subj-group></article-categories><title-group><article-title>
 
 
  Preparation and Characterization of ZnO Nanocrystalline Layers
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>.</surname><given-names>Haddad</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>A.</surname><given-names>Hafidi</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>A.</surname><given-names>Ain-Souya</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>N.</surname><given-names>Chahmat</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>R.</surname><given-names>Ganfoudi</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>M.</surname><given-names>Ghers</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Laboratory for the Study of Surfaces and Interfaces of Solid Material (LESIMS), Badji Mokhtar-Annaba University, Annaba, Algeria</addr-line></aff><aff id="aff2"><addr-line>Physics Laboratory of Matter and Radiation (LPMR), Med Cherif Mesaadia-Souk Ahras University, Souk Ahras, Algeria</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>haddadammar@yahoo.fr(.H)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>05</day><month>12</month><year>2014</year></pub-date><volume>02</volume><issue>12</issue><fpage>1</fpage><lpage>6</lpage><history><date date-type="received"><day>17</day>	<month>September</month>	<year>2014</year></date><date date-type="rev-recd"><day>30</day>	<month>October</month>	<year>2014</year>	</date><date date-type="accepted"><day>19</day>	<month>November</month>	<year>2014</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  This work consists on the study of the optical properties of zinc oxide layers. These Layers are elaborated under various conditions by cathode sputtering on glass substrates and by thermal oxidations of Zn layers deposited on different types of substrates by vacuum evaporation. The oxidation treatments of Zn are made in oxygen atmosphere at temperatures between 400&#176;C and 450&amp;degC for different times. The analyses by diffraction of X-rays, Optical Microscopy and Scanning electron microscopy enabled us to understand that the zinc oxide films deposited by cathode sputtering on a glass substrate and having a thickness of at least 240 nm and those prepared by thermal oxidation at 450&amp;degC during 2 hours of layers of Zn on an alumina substrate are homogeneous and consist of grains of size 30 nm. The optical transmission measurements show that the gap is around 3.02 eV for layers obtained by oxidation and 3.3 eV for those deposited by sputtering. These samples have a good optical transparency in the visible.
 
</p></abstract><kwd-group><kwd>Oxide</kwd><kwd> Gas</kwd><kwd> Adsorption</kwd><kwd> Conductance</kwd><kwd> Properties</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Zinc oxide has interesting properties that qualifies it among semiconductor materials the most used in the field of gas detectors [<xref ref-type="bibr" rid="scirp.52086-ref1">1</xref>] .</p><p>In order to obtain materials with good stability in the environment, metal oxides appear to be most appropriate for many applications. In the field of gas detection, several studies [<xref ref-type="bibr" rid="scirp.52086-ref2">2</xref>] showed that zinc oxide is very promising.</p><p>It is a semiconductor with a direct large gap and generally, crystallizes in w&#252;rtzite structure [<xref ref-type="bibr" rid="scirp.52086-ref3">3</xref>] . However, the size, the orientation of grains and the surface quality depend on the conditions in which the material was prepared and the different treatments which could be made. Indeed, surface states of semiconductor materials generate su- perficial electronic properties which are often significantly affected by their interactions with foreign elements [<xref ref-type="bibr" rid="scirp.52086-ref4">4</xref>] .</p></sec><sec id="s2"><title>2. Experimental Conditions</title><p>In the aim to obtain various qualities of zinc oxide layers, in order to study their stability and to propose them for practical uses, particularly in the gas detection, we used two techniques: the sputtering of zinc oxide and thermal oxidation of zinc layers prepared by vacuum evaporation.</p><p>In the technique of sputtering, the layers were deposited on glass substrates by using a target of zinc and injecting oxygen in argon atmosphere. Oxygen will interact with the zinc to form molecules of ZnO.</p><p>Other layers of zinc oxide were obtained by thermal oxidation of Zn layers, in oxygen atmosphere, at temperatures 420˚C - 450˚C during different periods of 2 to 4 hours. The layers of Zn were prepared by vacuum evaporation on glass and alumina substrates.</p></sec><sec id="s3"><title>3. Characterization of ZnO layers</title><p>Analysis by X-rays diffraction, optical microscopy and scanning electron microscopy, were carried out in order to identify the phases formed, the crystalline structure, size and superficial aspect of ZnO layers elaborated. <xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="fig" rid="fig2">Figure 2</xref> present spectra of X-rays diffraction obtained on layers prepared under different conditions. They show a preferred orientation of grains for all layers, according to the plans (002).</p><p>The samples prepared by thermal oxidation of zinc layers gave spectra (<xref ref-type="fig" rid="fig1">Figure 1</xref>) characteristics of ZnO but with the presence of lines specific of O<sub>2</sub> and Zn. The presence of Zn proves that, under the conditions used, the oxidation reaction is partial.</p><p>In the case of layers obtained by sputtering, the spectra of X-rays diffraction (<xref ref-type="fig" rid="fig2">Figure 2</xref>) are characteristic of the compound.</p><p>The micrographs (<xref ref-type="fig" rid="fig3">Figure 3</xref> and <xref ref-type="fig" rid="fig4">Figure 4</xref>) of optical microscopy show that layers prepared under different conditions have different aspects.</p><p>Layers obtained by thermal oxidation on alumina substrates (<xref ref-type="fig" rid="fig3">Figure 3</xref>(a)) are more homogeneous than those prepared using the same technique on glass substrates (<xref ref-type="fig" rid="fig3">Figure 3</xref>(b)). According to <xref ref-type="fig" rid="fig4">Figure 4</xref>, layers obtained by sputtering are relatively homogeneous and this aspect seems to improve with the thickness.</p><p>We observe that there is a granulometry for the various aspects of layers obtained by thermal oxidation on the glass substrate (<xref ref-type="fig" rid="fig4">Figure 4</xref>).</p><p>The observations by scanning electron microscopy show that the layers obtained by thermal oxidation on alumina substrates (<xref ref-type="fig" rid="fig5">Figure 5</xref>) are more homogeneous than those obtained on glass substrates (<xref ref-type="fig" rid="fig6">Figure 6</xref>). We</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> X-rays diffraction of zinc oxide layers obtained by ther- mal oxidations at 450˚C during (1h-2h-4h) on glass substrates</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1740111x5.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> X-ray diffraction of zinc oxide layer, obtained by sputtering on glass substrate</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1740111x6.png"/></fig><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Optical microscopy of zinc oxide layers obtained by thermal oxi- dation during 2 hours at: (a) 420˚C on an alumina substrate; and (b) 450˚C on glass substrate.</title></caption><fig id ="fig3_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1740111x8.png"/></fig><fig id ="fig3_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1740111x7.png"/></fig></fig-group><fig-group id="fig4"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Optical Microscopy of zinc oxide layers with different thicknesses, obtained by sputtering on a glass substrates.</title></caption><fig id ="fig4_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1740111x9.png"/></fig><fig id ="fig4_2"><label> (c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1740111x10.png"/></fig><fig id ="fig4_3"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1740111x11.png"/></fig></fig-group><p>note the existence of grains with different forms and aspects for the layers produced by thermal oxidation on glass substrates.</p><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Scanning electron microscopy of zinc oxide layer, ob- tained on an alumina substrate by oxidation at 450˚C for 2 hours</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1740111x12.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Scanning electron microscopy of zinc oxide layer, ob- tained on a glass substrate by oxidation at 450˚C for 2 hours</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1740111x13.png"/></fig><p>The analysis of X-rays diffraction results and scanning electron microscopy allowed us to determine the grains sizes which are about 60nm for the layers prepared by thermal oxidation on alumina substrates and 30 nm for the layers obtained by sputtering on glass substrates. This nano-size grain gives the material a large specific surface favouring a strong adsorption of gas.</p><p>Measures of optical transmission (Figures 7-10) made on the zinc oxide layers allowed us to identify that the values of the gap are varying from 3.2 eV to 3.3 eV for layers prepared by sputtering and 3.02 eV for layers obtained by thermal oxidation. The layers have a good optical transparency in the visible.</p></sec><sec id="s4"><title>4. Conclusions</title><p>The zinc oxide layers prepared by various techniques have a preferential orientation of the grains according to the plans (002).</p><p>The layers obtained by thermal oxidation on the alumina substrates have a more homogeneous aspect compared with those prepared by the same technique on glass substrates.</p><p>The techniques used in elaboration of the samples allowed us to obtain layers with grains sizes about 60 nm for the materials prepared by thermal oxidation on alumina substrate and 30 nm for those prepared by sputtering</p><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Optical transmission of a zinc oxide layer obtained by sputtering on a glass substrate, (thickness = 240 nm)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1740111x14.png"/></fig><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Curve (αυh)<sup>2</sup> = f(hυ) of a zinc oxide layer obtained by sputtering on a glass substrate, (thickness = 240 nm)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1740111x15.png"/></fig><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> Optical transmission of a zinc oxide layer obtained on a glass substrate by oxidation at 420˚C for 2 hours</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1740111x16.png"/></fig><fig id="fig10"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> Curve (αυh)<sup>2</sup> = f(hυ) of zinc oxide layer obtained by thermal oxidation on a glass substrate at 420˚C for 2 hours</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1740111x17.png"/></fig><p>on glass substrates. This nano-size grain gives the material a large specific surface favouring a strong adsorption of gas.</p><p>The values of the gap are varying from 3.2 eV to 3.3 eV for layers prepared by sputtering and 3.02 eV for layers obtained by thermal oxidation. The layers have a good optical transparency in the visible.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.52086-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Gaidi, M. and Chenevier, B. (2000) Electrical Properties Evolution under Reducing Gaseous Mixtures (H2, H2S, CO) of SnO2 Thin Films Doped with Pd/Pt Aggregates and Used as Polluting Gas Sensors. Sensors and Actuators, B62, 43- 48. http://dx.doi.org/10.1016/S0925-4005(99)00358-5</mixed-citation></ref><ref id="scirp.52086-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Wang, M., Wang, J., Chen, W., Cui, Y. and Wang, L. 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