<?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">NJGC</journal-id><journal-title-group><journal-title>New Journal of Glass and Ceramics</journal-title></journal-title-group><issn pub-type="epub">2161-7554</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/njgc.2017.74008</article-id><article-id pub-id-type="publisher-id">NJGC-79600</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>
 
 
  Structural, Morphology and Some Optical Properties of Chalcogenide Ga&lt;sub&gt;80-x&lt;/sub&gt;Se&lt;sub&gt;x&lt;/sub&gt;Te&lt;sub&gt;20&lt;/sub&gt; (Where x = 10%, 15% and 20%) Glassy Material
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Khadijah</surname><given-names>M. Al Mokhtar</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>Bahia</surname><given-names>O. Alsobhi</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Physics, Faculty of Science, Taibah University, Madinah, Saudi Arabia</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>khmadina@yahoo.com(KMAM)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>12</day><month>10</month><year>2017</year></pub-date><volume>07</volume><issue>04</issue><fpage>91</fpage><lpage>99</lpage><history><date date-type="received"><day>18,</day>	<month>August</month>	<year>2017</year></date><date date-type="rev-recd"><day>10,</day>	<month>October</month>	<year>2017</year>	</date><date date-type="accepted"><day>13,</day>	<month>October</month>	<year>2017</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>
 
 
  Ga
  <sub>80-x</sub>
  Se
  <sub>x</sub>
  Te
  <sub>20</sub>
   amorphous system was prepared by conventional technique. Structural, morphology and optical properties have been investigated. X-ray diffraction (XRD) patterns reveal the non-crystalline nature of the prepared sample. Differential thermal analysis (DTA) traces indicate the presen
  ce
   glass transition temper
  a
  ture T<sub>g </sub>for all samples below 500&#176;C. Addition T<sub>g</sub> values increases by increas
  ing
   
  Se content. Energy dispersive X-ray spectroscopy (EDX) data shows good agreement with actual composition. Moreover
  ,
   surface characterization was achieved by scanning electron microscope (SEM)
  .
   The patterns confirmed the non-crystalline nature. In order to analyze the data
  ,
   the cohesive energy C.E w
  as
   calculated 
  by
   all three composition optical properties 
  that 
  have been investigated in the wavelength range 500 - 2500 nm. Reflectivity R and transmitivity T spectrum were used to estimate the band gap energy using UV-Visible absorption spectrum. It is worthy mention that the optical band gap follows the T<sub>g</sub> and cohesive energy behavior, where it increases by increasing Se content.
 
</p></abstract><kwd-group><kwd>Chalcogenide Glasses</kwd><kwd> Structure</kwd><kwd> Optical</kwd><kwd> Cohesive Energy</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Chalcogenide glasses find wide applications in various fields of up-to-date technology due to their peculiar properties [<xref ref-type="bibr" rid="scirp.79600-ref1">1</xref>] , such as target materials of television cameras, microwave devices, switching and diodes [<xref ref-type="bibr" rid="scirp.79600-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.79600-ref3">3</xref>] . This is most likely due to their high optical transparency in the IR region, strong optical nonlinearity, high photo sensitivity, ease of fabrication and processing, and good chemical durability. Chalcogenide glasses based on the chalcogen elements S, Se, Te are used widely in ultra-fast optical switches, frequency converters, optical amplifiers, optical recording devices, an optical integrated circuit for IR operations and infrared transmitting optical fibers [<xref ref-type="bibr" rid="scirp.79600-ref4">4</xref>] - [<xref ref-type="bibr" rid="scirp.79600-ref10">10</xref>] . Ga-X systems where elements X = S, Se or Te have revealed to be particular interest [<xref ref-type="bibr" rid="scirp.79600-ref10">10</xref>] . In the present article, the structural, morphological and some optical properties of Ga<sub>80−x</sub>Se<sub>x</sub>Te<sub>20</sub> (where X = 10%, 15% and 20%) have been studied with thickness ranging between 165 nm, 615 nm and 1027 nm.</p></sec><sec id="s2"><title>2. Experimental Procedure</title><p>Bulk amorphous of Ga<sub>80−x</sub>Se<sub>x</sub>Te<sub>20</sub> (where x = 10, 15 and 20 at %) chalcogenide glass were prepared by conventional melt quenching technique [<xref ref-type="bibr" rid="scirp.79600-ref11">11</xref>] . High purity (99.9999% purity) materials of Ga, Se, and Te were weighed according to their atomic percentage and sealed in quartz ampoules with a vacuum of 10<sup>−5</sup> Torr. The samples were then heated and melted in a rocking furnace, where temperature was raised at a rate of 4 K per minute for up to 1273 ˚K for 15 h. During heating process, the ampoules were frequently rocked by rotating a ceramic rod to which the amorphous were tucked away in the furnace is order to obtain a compositionally homogeneous melt. The molten samples were then rapidly quenched in ice cooled water. The quenched samples were taken out by breaking the ampoules. The glassy nature of the samples was established by the non-isothermal differential scanning (DTA-50) Measurements at a constant heating rate of 20 K/min. The DTA scan was obtained by heating 8 mg of powdered samples sealed in an aluminum pan.</p><p>The x-ray diffraction machine (XD-D ShimadZu) was used to study nature of the prepared sample). Moreover the scanning electron microscope (Joel-SEM-5400) which connected by energy dispersive spectroscopy (EDX) technique was used to study the morphology together with chemical compositions of samples, constitutes fully quantitative analyses results were obtained from the spectra by processing date through Zaf correction program. The transmittance and reflectance were measured using a double beam UV-VIS Spectrophotometer in the wavelength range 500 - 2500 nm.</p></sec><sec id="s3"><title>3. Results and Discussion</title><sec id="s3_1"><title>3.1. Thermal Properties</title><p><xref ref-type="fig" rid="fig1">Figure 1</xref> represents the DTA thermogram of the investigated system. It was obtained for a bulk glass sample by heating 8mg using a heating rate of 20 k/min. By increasing Se content T<sub>g</sub> shows tendency to increase <xref ref-type="fig" rid="fig1">Figure 1</xref>. The temperature was found to be 433 K, 445 K, and 447 K respectively.</p></sec><sec id="s3_2"><title>3.2. Structural of Characterization</title><p>The X-ray diffraction pattern of theGa<sub>80−x</sub>Se<sub>x</sub>Te<sub>20</sub> (where x = 10, 15 and 20 at %) glass composition was presented in <xref ref-type="fig" rid="fig2">Figure 2</xref>. It is clear that the absence of sharp diffraction lines and the presence of hump only confirm the amorphous nature of the prepared samples.</p></sec><sec id="s3_3"><title>3.3. Surface Morphology</title><p>Morphological inspections performed by SEM on as-grown films have shown a flat surface without the presence of cracks agglomerates and precipitated <xref ref-type="fig" rid="fig3">Figure 3</xref>. SEM image has confirmed the absence of spurious phase. The morphology of thin films of different compositions has been found to be of coniform contrast. The diffraction pattern for the as-prepared thin films of different compositions is similar, indicating the amorphous nature of as-prepared thin films of different compositions. The elemental compositions of Ga<sub>80−x</sub>Se<sub>x</sub>Te<sub>20</sub> (where x = 10, 15 and 20 at %) chalcogenide glasses were checked by energy dispersive X-ray analysis (EDX). It is noticed that <xref ref-type="fig" rid="fig4">Figure 4</xref> which clearly show that amount of selenium increase with the increase of X.</p></sec><sec id="s3_4"><title>3.4. Cohesive Energy</title><p>The possible bonds formed in chalcogenids system Ga<sub>80−x</sub>Se<sub>x</sub>Te<sub>20</sub> are Se-Ga, Se-Se, Se-Te. According to chemical bond approach (CBA) [<xref ref-type="bibr" rid="scirp.79600-ref12">12</xref>] combination in different type in the atoms takes place more easily rather in the atoms of same type. These bonds are formed in the sequence of decreasing bond energy until the available valence of atoms is saturated. The Ga-Se glassy system is covalent chalcogenide system. The bond energy of homopolar bonds can be estimated by The Pauling method in terms of the bond energy of homopolar bonds and the electronegativity of the atoms involved.</p><p>The bond energy E(A-B) of hetero nuclear bond, can be calculated by Equation [<xref ref-type="bibr" rid="scirp.79600-ref13">13</xref>]</p><p>E A − B = ( E A − A − E B − B ) 1 / 2 + 30 ( x A − x B ) 2 (1)</p><p>E<sub>A−A</sub> and E<sub>B−B</sub> are the bonds energies of homo nuclear bonds, x<sub>A</sub> and x<sub>B</sub> are electronegativity values of A and B Elements.</p><p>The bond energy of the homo polar bonds E<sub>Ga−Ga</sub> is 31.82, E<sub>Se−Se</sub> is 44, and E<sub>Te−Te</sub> is 33 Kal/mol [<xref ref-type="bibr" rid="scirp.79600-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.79600-ref15">15</xref>] .</p><p>The electronegativity value are 1.81, 2.55, and 2.10 for Ga, Se and Te respectively [<xref ref-type="bibr" rid="scirp.79600-ref13">13</xref>] .</p><p>By using Equation (1) values of E<sub>Ga−Se</sub>, E<sub>Se−Te</sub> and E<sub>Te−Se</sub> are gives as 53.85, 44.93 and 44.18 respectively.</p><p>The bonds are formed in order of decreasing bond energy.</p><p>Ga-Se bonds having maximum energy are first followed by E<sub>Te−Se</sub> then E<sub>Ga−Te</sub> bonds.</p><p>As these bond energies are assumed to be addition, so cohesive energies calculated by summing the bond energies over all possible in a compound. Cohesive energies calculated as:</p><p>C E = ∑ C i E i (2)</p><p>where C<sub>i</sub> is the probability of formation of expected bonds, and E<sub>i</sub> is the energy of the corresponding bond present in the system.</p><p><xref ref-type="table" rid="table1">Table 1</xref> listed the chemical distribution of bonds, electronegativity, and cohesive energy of the sample.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Electronegativity, distribution of chemical bonds and cohesive energy for the composition Ga<sub>80-x</sub>Se<sub>x</sub>Te<sub>20</sub> (where x = 10, 15 and 20 at %)</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Composition</th><th align="center" valign="middle"  rowspan="2"  >Electronegativity</th><th align="center" valign="middle"  colspan="3"  >Distribution of chemical bonds</th><th align="center" valign="middle" >Cohesive energy<sub> </sub></th></tr></thead><tr><td align="center" valign="middle" >Ga-Se</td><td align="center" valign="middle" >Ga-Te</td><td align="center" valign="middle" >Ga-Ga</td><td align="center" valign="middle" >CE ev</td></tr><tr><td align="center" valign="middle" >Ga<sub>70</sub>Se<sub>10</sub>Te<sub>20</sub></td><td align="center" valign="middle" >1.81</td><td align="center" valign="middle" >0.09523810</td><td align="center" valign="middle" >0.1904762</td><td align="center" valign="middle" >0.7143857</td><td align="center" valign="middle" >1.496454</td></tr><tr><td align="center" valign="middle" >Ga<sub>65</sub>Se<sub>15</sub>Te<sub>20</sub></td><td align="center" valign="middle" >2.55</td><td align="center" valign="middle" >0.1538462</td><td align="center" valign="middle" >0.2051282</td><td align="center" valign="middle" >0.6410256</td><td align="center" valign="middle" >1.5544054</td></tr><tr><td align="center" valign="middle" >Ga<sub>60</sub>Se<sub>20</sub>Te<sub>20</sub></td><td align="center" valign="middle" >2.10</td><td align="center" valign="middle" >0.2222222</td><td align="center" valign="middle" >0.2222222</td><td align="center" valign="middle" >0.5555556</td><td align="center" valign="middle" >1.6220154</td></tr></tbody></table></table-wrap><p>It is observed that by increasing Se content leads to increasing the cohesive energy in chalcogenide system Ga<sub>80−x</sub>Se<sub>x</sub>Te<sub>20</sub>.</p></sec><sec id="s3_5"><title>3.5. Optical Properties</title><p>Optical properties of Ga<sub>80−x</sub>Se<sub>x</sub>Te<sub>20</sub> (where x = 10, 15 and 20 at %) have been investigated in the wavelength (500 - 2500) nm. Figures 5(a)-(c) show reflectivity R and transmition T of investigated then films with wavelength.</p><p>The data of (<xref ref-type="fig" rid="fig5">Figure 5</xref>(a)) Ga<sub>70</sub>Se<sub>10</sub>Te<sub>20</sub> reveled reflectivity R decrees by increasing wavelength, while transimtion T is increase by increasing wavelength. It is worthy to mention that the observed edg in transmtion spectra extended over wide wavelength ranged, confirming a non-crystalline nature of the films.</p><p><xref ref-type="fig" rid="fig5">Figure 5</xref>(b) and <xref ref-type="fig" rid="fig5">Figure 5</xref>(c) of composition Ga<sub>65</sub>Se<sub>15</sub>Te<sub>20</sub> and Ga<sub>60</sub>Se<sub>20</sub>Te<sub>20</sub> show that the dependence of R and T is non-linear, by increasing the selenium content, the transimtion increase up to 1750 nm with minimum reflection at the same wavelength. Such observed nonlinearity allows to conclude that we are dealing with more than one absorption mechanism.</p><p>The obtained spectra were used to estimate the optical band gap energies as 0.721 ev, 0.97 ev, and 1.007 ev for Ga<sub>70</sub>Se<sub>10</sub>Te<sub>20</sub>, Ga<sub>65</sub>Se<sub>15</sub>Te<sub>20</sub> and Ga<sub>60</sub>Se<sub>20</sub>Te<sub>20</sub> respectively.</p><p>It is worthy to mention that the band gap increases by increase Se content, i.e. by increasing C.E the letter represent the average binding energy of the system.</p></sec></sec><sec id="s4"><title>4. Conclusions</title><p>Glassy system of Ga<sub>80−x</sub>Se<sub>x</sub>Te<sub>20</sub> (where x = 10%, 15% and 20%) Chalcogenide Semiconductors has been successfully prepared. The study includes DTA, XRD, SEM, EDX and UV-visible absorption spectrum. The analysis of DTA reveals the absence of any sharp exothermic peak indicating the absence of structural change, which is in a good agreement with X-ray diffraction, confirmed the amorphous state of the system. Also (SEM) and (EDX) are confirmed the absence of serious phase. Moreover, the cohesive energy of the investigated has been calculated by using chemical bond. It follows the T<sub>g</sub> behavior, and by increasing Se content, cohesive energy increases.</p><p>Addition of selenium content in the Ga<sub>80−x</sub>Se<sub>x</sub>Te<sub>20</sub> system modifies the properties of the present sample especially the optical (T &amp; R). Optical measurements indicate that the non-direct transition is dominant in mechanism responsible for the photon absorption inside the investigated samples. It is also observed that the increasing of Se content leads to increase of band gap. This is in fair agreement with T<sub>g</sub> and cohesive energy data.</p></sec><sec id="s5"><title>Cite this paper</title><p>Al Mokhtar, K.M. and Alsobhi, B.O. (2017) Structural, Morphology and Some Optical Properties of Chalcogenide Ga<sub>80−x</sub>Se<sub>x</sub>Te<sub>20</sub> (Where x = 10%, 15% and 20%) Glassy Material. New Journal of Glass and Ceramics, 7, 91-99. https://doi.org/10.4236/njgc.2017.74008</p></sec></body><back><ref-list><title>References</title><ref id="scirp.79600-ref1"><label>1</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Mehta</surname><given-names> N. </given-names></name>,<etal>et al</etal>. 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