<?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">MSA</journal-id><journal-title-group><journal-title>Materials Sciences and Applications</journal-title></journal-title-group><issn pub-type="epub">2153-117X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/msa.2017.810052</article-id><article-id pub-id-type="publisher-id">MSA-78959</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>
 
 
  Composition and Band Gap Controlled AACVD of ZnSe and ZnS&lt;sub&gt;x&lt;/sub&gt;Se&lt;sub&gt;1-x&lt;/sub&gt; Thin Films Using Novel Single Source Precursors
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yousef</surname><given-names>Alghamdi</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Chemistry, Faculty of Science, King Abdulaziz University, Jeddah, KSA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>earthquake70@googlemail.com</email></corresp></author-notes><pub-date pub-type="epub"><day>05</day><month>09</month><year>2017</year></pub-date><volume>08</volume><issue>10</issue><fpage>726</fpage><lpage>737</lpage><history><date date-type="received"><day>21,</day>	<month>July</month>	<year>2017</year></date><date date-type="rev-recd"><day>5,</day>	<month>September</month>	<year>2017</year>	</date><date date-type="accepted"><day>8,</day>	<month>September</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>
 
 
  Polycrystalline thin films of ZnSe and ZnS
  <sub>x</sub>Se
  <sub>1-x</sub> have been deposited on glass substrates by Aerosol Assisted Chemical Vapour Deposition (AACVD) from bis(diethyldiselenocarbamato)zinc(II) and a 1:1 and 1:0.75 mixtures of bis(diethyldiselenocarbamato)zinc(II) and 
  bis(diethyldithiocarbamato)zinc(II) as precursors. All films were characterized by p-XRD, SEM, EDX, Raman spectroscopy, photoluminescence (PL and UV/Vis spectroscopy. The band gap of pure ZnSe thin films was found to be 2.25 whereas the band gap of ZnS
  <sub>x</sub>Se
  <sub>1-x</sub> films varied from 2.55 to 2.66 eV depending on the sulfur content in the films. PL emission spectra showed a clear blue shift for ZnS
  <sub>x</sub>Se
  <sub>1-x</sub> films compared to ZnSe due to the sulphur content in the films which increase the band gap. The band gap of ZnSSe can be controlled by sulfur to selenium ratio in the alloy. The morphology of the ZnSe thin films changed from small randomly shaped crystallites to triangles whereas the morphology of ZnS
  <sub>x</sub>Se
  <sub>1-x</sub> was mainly based on cuboids.
 
</p></abstract><kwd-group><kwd>&lt;i&gt;Bis&lt;/i&gt;(diethyldiselenocarbamato)zinc(II)</kwd><kwd> ZnSe</kwd><kwd> ZnSSe</kwd><kwd> AACVD</kwd><kwd> SEM</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Metal selenides are wide band gap materials and have applications in light-emitting devices, solar cells, sensors, and optical recording materials [<xref ref-type="bibr" rid="scirp.78959-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref4">4</xref>] . ZnSe is ideal material for blue-green laser diodes [<xref ref-type="bibr" rid="scirp.78959-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref2">2</xref>] , mid-IR laser sources for remote sensing applications [<xref ref-type="bibr" rid="scirp.78959-ref5">5</xref>] , and in optically controlled switching devices due to its large photo resistivity [<xref ref-type="bibr" rid="scirp.78959-ref6">6</xref>] . Zinc selenide thin films had been fabricated by photochemical deposition (PCD) [<xref ref-type="bibr" rid="scirp.78959-ref7">7</xref>] , chemical bath deposition (CBD) [<xref ref-type="bibr" rid="scirp.78959-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref9">9</xref>] and electrochemical deposition (ECD) [<xref ref-type="bibr" rid="scirp.78959-ref10">10</xref>] , but all these methods have their own drawbacks including higher annealing temperatures for PCD, controlling rate of reaction for CBD and the use of only conductive substrates for ECD [<xref ref-type="bibr" rid="scirp.78959-ref7">7</xref>] .</p><p>Several reports have been published for the use of single-source precursors for the deposition of metal chalcogenide [<xref ref-type="bibr" rid="scirp.78959-ref11">11</xref>] - [<xref ref-type="bibr" rid="scirp.78959-ref22">22</xref>] . A range of chalcogenides have been deposited from M[ESi(SiMe)<sub>3</sub>]<sub>2</sub> (M = Zn, Cd, Hg; E = S, Se or Te) complexes as single source precursors [<xref ref-type="bibr" rid="scirp.78959-ref23">23</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref24">24</xref>] .<sup> </sup>Metal complexes with the general formula [M(R<sub>2</sub>PSe<sub>2</sub>)<sub>n</sub>] (M = Zn, Cd, Pb, In, Ga, Cu, Bi, Ni; R = <sup>i</sup>Pr, Ph) have been synthesised and used for the deposition of metal selenide thin films by CVD [<xref ref-type="bibr" rid="scirp.78959-ref25">25</xref>] .<sup> </sup>Other metal complexes used as single source precursors include: [(M(E<sub>2</sub>CNR<sub>2</sub>)<sub>2</sub>] (symmetrical) or [M(E<sub>2</sub>CNRR’)<sub>2</sub>] (unsymmetrical) (R, R’ = alkyl, E = S, Se; M = Zn, Cd) [<xref ref-type="bibr" rid="scirp.78959-ref22">22</xref>] , mixed alkyl/dithio- or diseleno-carbamato complexes [M(E<sub>2</sub>CNRR’)<sub>2</sub>], where R = Me, Et, Bu<sup>t</sup> or Me<sub>3</sub>CCH<sub>2</sub>, M = Zn or Cd; E = S or Se; R’ = Me or Et [<xref ref-type="bibr" rid="scirp.78959-ref26">26</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref28">28</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref29">29</xref>] , imino-bis(dialkylphos-phineselenide) complexes [M[(EP<sup>i</sup>Pr<sub>2</sub>)<sub>2</sub>N]<sub>2</sub>] (M = Cd, Zn; E = S, Se) and [M[(SePPh<sub>2</sub>)<sub>2</sub>N]<sub>2</sub>] (M = Cd, Zn) [<xref ref-type="bibr" rid="scirp.78959-ref30">30</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref31">31</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref32">32</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref33">33</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref34">34</xref>] .</p><p>ZnS<sub>x</sub>Se<sub>1?x</sub> is found to be one of the best substituent for CdS as a buffer layer. When the sulphur composition is larger than 0.2, then it becomes another good candidate for cladding layers for blue laser diodes [<xref ref-type="bibr" rid="scirp.78959-ref35">35</xref>] . Polycrystalline ZnSxSe<sub>1?x</sub> thin films were deposited by co-evaporation of ZnS and ZnSe [<xref ref-type="bibr" rid="scirp.78959-ref36">36</xref>] , by low-pressure metal-organic chemical vapour deposition (LP-MOCVD) process from the zinc alkyls dimethylzinc (DMZ) or diethylzinc (DEZ) and H<sub>2</sub>Se and H<sub>2</sub>S [<xref ref-type="bibr" rid="scirp.78959-ref37">37</xref>] , and by molecular beam epitaxy (MBE) using radio-frequency (RF) plasma [<xref ref-type="bibr" rid="scirp.78959-ref38">38</xref>] . We have recently reported the deposition of CdSe and CdSSe thin films from molecular precursors by AACVD [<xref ref-type="bibr" rid="scirp.78959-ref39">39</xref>] . Herein we report the deposition of highly crystalline hexagonal ZnSe thin films from bis(diethyldiselenocarbamato)zinc(II) complex and ZnSSe composite from a mixture of bis(diethyldiselenocarbamato)zinc(II) and bis(diethyldithiocarbamato)zinc(II) complexes and their detailed optical and structural characterisation. To the best of our knowledge ZnSe or ZnSSe thin films have never been deposited by AACVD method from diselenocarbamato complexes of zinc.</p></sec><sec id="s2"><title>2. Experimental</title><sec id="s2_1"><title>2.1. Synthesis of Precursors</title><p>Bis(diethyldiselnocarbamato)zinc(II)[Zn(Se<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] and bis(diethyldithiocarba- mato)-zinc(II) [Zn(S<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] precursors were synthesised using method described in literature [<xref ref-type="bibr" rid="scirp.78959-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref28">28</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref29">29</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref30">30</xref>] . In a typical synthesis sodium salt of diethyl dithiocarbamate ([Na(S<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>]) was reacted with zinc nitrate (Zn(NO<sub>3</sub>)<sub>2</sub>) in a water solution. The white precipitate of [Zn(S<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] was separated by filtration, washed with water and dried under vacuum.</p></sec><sec id="s2_2"><title>2.2. Thermogravimetric Analysis</title><p>Thermogravimetric analysis measurements were carried out by a Seiko SSC/S200 model under a heating rate of 10˚C∙min<sup>−1</sup> under nitrogen. Indium metal is used as a reference to calibrate the instrument. TGA was performed by School of Chemistry, University of Manchester, micro-analysis team</p></sec><sec id="s2_3"><title>2.3. Deposition of Thin Films</title><p>The depositions of thin films were carried out at 300˚C and 350˚C using 14 mmol of the [Zn(Se<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] precursor in 15 mL THF and for the deposition of ZnSSe; 1:1 ratio of [Zn(Se<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] (7 mmol) and [Zn(S<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] (7 mmol) in 15 mL THF and Zn(Se<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] (5 mmol) and [Zn(S<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] (7 mmol) in 15 mL THF to reduce the amount of Se on the thin films at 350˚C.</p><p>The depositions were carried out onto glass slides with the dimensions of 1 &#215; 3 cm by AACVD. In a typical experiment, the precursor was dissolved in 15 mL THF in a two-necked 100 mL round-bottom flask. The flask was connected with an argon gas inlet carried the aerosols generated by a PIFCO ultrasonic humidifier to the reactor tube connected to other neck of the flask and placed in a Carbolite furnace. The gas flow rate was controlled at 160 Sccm through a Platon flow gauge. The precursor mist was thermolysed in the hot zone at the surface of glass substrate and resulted in the deposition of thin film as reported previously [<xref ref-type="bibr" rid="scirp.78959-ref39">39</xref>] .</p></sec><sec id="s2_4"><title>2.4. Characterisation of Thin Films</title><p>XRD patterns were recorded on a Bruker D8 AXE diffractometer (Cu-Kα) from 20 to 80 degrees with a step size of 0.05. SEM studies were carried out by using a Philips XL 30 FEGSEM and EDAX analysis for the composition of films were carried out by using a DX4 instrument. TEM i were recorded on a Tecnai F30 microscope and Raman spectra were measured by Renishaw 1000 Micro Raman system. UV/Vis spectra were carried out by Perkin Elmer Lambda 1050 spectrophotometer. And PL spectra were taken by using HOIBO Fluorolog FL3 iHR at excitation wavelength of 400 nm.</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><p>Bis(diethyldithio/diselenocarbamato)zinc(II) complexes can easily be synthesised by a single step reaction and are stable at room temperature for periods of years as the complexes used in these experiments were synthesised 5 years ago. The analysis of the complexes after 5 years proved that no decomposition occurred. These complexes are soluble in common organic solvents such as toluene, THF, chloroform. Both decompose in the same the same manner and in the same temperature range (vide infra) making them suitable to be used as a mixture in different ratios to control the sulfur or selenium concentration in the alloy. The effect of precursor concentration and deposition temperature on the stoichiometric composition and morphology of the ZnSe and ZnSSe thin films were investigated.</p><sec id="s3_1"><title>3.1. Thermogravimetric Analysis (TGA)</title><p>Thermogravimetric analysis (TGA) of [Zn(Se<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] and [Zn(S<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] films were studied from 10˚C - 600˚C under nitrogen. [Zn(S<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] and [Zn(Se<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] decomposed in one relatively sharp step with almost similar rate and resulted with ~8% and ~10% residual mass, which found to be half or less than half of the mass of the expected metal chalcogenides; ZnS (27%) or ZnSe (20%). The sharp transition shows a one-step decomposition for both complexes to give the metal chalcogenides and all the rest of impurities volatilised. The less quantity of the residue appears to be due to the volatility of sulphur and selenium at high temperatures. Decomposition of both precursors at similar temperature makes them highly suitable for depositing ZnSe, ZnS, and ZnSSe thin films by AACVD within a temperature range of 250˚C to 350˚C (<xref ref-type="fig" rid="fig1">Figure 1</xref>).</p></sec><sec id="s3_2"><title>3.2. AACVD of ZnSe Thin Films</title><sec id="s3_2_1"><title>3.2.1. Powder X-Ray Diffraction for ZnSe Thin Films</title><p>Depositions were carried out at 300˚C and 350˚C using 14 mmol of the [Zn(Se<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] precursor in 15 mL THF.</p><p>Films deposited at 300˚C were slightly yellow and thick, p-XRD did not give any diffraction peaks indicating the amorphous nature of the deposited material whereas, films deposited at 350˚C were thick adherent, specular golden in appearance. <xref ref-type="fig" rid="fig2">Figure 2</xref>(a) shows the p-XRD pattern of ZnSe thin films deposited at 350˚C. The main peaks at about 27.3˚, 45.2˚ and 53.6˚ correspond to cubic ZnSe (ICDD: 01-088-2345).</p></sec><sec id="s3_2_2"><title>3.2.2. Scanning Electron Microscopy of ZnSe Films</title><p>Morphology of the films was studied using by SEM. <xref ref-type="fig" rid="fig2">Figure 2</xref>(b) shows the SEM images of the films with an inset at higher magnification. The films are based on</p><p>small (100 - 300 nm) random crystallites thickly packed together. EDX analysis showed Zn:Se ratio as 49.44:50.55, which is very close to the 1:1 ratio expected for ZnSe.</p></sec><sec id="s3_2_3"><title>3.2.3. Raman and PL Spectra of ZnSe Films</title><p>Raman spectra showed peaks at 205, 253, 412 and 498 cm<sup>−1</sup> which are close to the Raman peaks for the TO, LO and 2LO phonon modes of ZnSe (~206, 252 and 493 cm<sup>−1</sup>) [<xref ref-type="bibr" rid="scirp.78959-ref40">40</xref>] - [<xref ref-type="bibr" rid="scirp.78959-ref45">45</xref>] (<xref ref-type="fig" rid="fig3">Figure 3</xref>(a)).</p><p>PL spectra showed a very strong emission between 530 to 580 nm (<xref ref-type="fig" rid="fig3">Figure 3</xref>(b)). The emission maximum shift towards the higher energy, as compared to the bulk values, is due to the smaller size of crystallites and large surface defects and Zn vacancies at the interstitial sites [<xref ref-type="bibr" rid="scirp.78959-ref46">46</xref>] .</p></sec></sec><sec id="s3_3"><title>3.3. AACVD of Zinc Sulfoselenide (ZnS<sub>x</sub>Se<sub>1−x</sub>) Thin Films</title><sec id="s3_3_1"><title>3.3.1. p-XRD of ZnSSe Thin Films</title><p>The deposition was carried out at 300˚C and 350˚C but no deposition occurred at 300˚C. Thick specular yellow films were obtained at 350˚C using 1:1 and 1:0.75 ratios of [Zn(Se<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] and [Zn(S<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] precursors. The p-XRD patterns of ZnS<sub>x</sub>Se<sub>1−x</sub> thin films deposited using 1:1 ratio of mixture are shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>. The p-XRD patterns were indexed using the standard patterns for cubic ZnSe<sub>0.5</sub>S<sub>.0.5</sub> (ICDD: 04-001-6856) space group F-43m, lattice parameters, a = b = c = 5.500 &#197;. The main peaks at 2θ: 28.07 (111), 32.53 (200), 46.67 (220), 55.35 (311) and 58.04 (222) are slightly shifted from the standard pattern. Minor peaks are due to the contamination of binary phases as ZnS and ZnSe (<xref ref-type="fig" rid="fig4">Figure 4</xref>).</p><p>1:0.75 molar ratio of [Zn(Se<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>]and [Zn(S<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] precursor mixture at 350˚C produced thin orange adherent films. The p-XRD patterns showed good matching with cubic ZnSe<sub>0.5</sub>S<sub>.0.5</sub> (ICDD: 04-001-6856). The main peaks were observed at 2θ: 28.07 (111), 32.53 (200), 46.67 (220), 55.35 (311) and 58.04 (222) similar to those observed for films deposited from 1:1 mixture. Again the films</p><p>had minor contamination of ZnS and ZnSe phases. The p-XRD patterns showed good agreement with the reported X-ray diffraction data related to the ZnSSe thin films for different x-values (x= 0, 0.2, 0.4, 0.6). It can be noted that the higher the x-value the more the (1 1 1) peak shifts from the ZnSe (1 1 1) peak to ZnS(1 1 1) peak as reported [<xref ref-type="bibr" rid="scirp.78959-ref35">35</xref>] .</p></sec><sec id="s3_3_2"><title>3.3.2. Morphology of ZnSSe Thin Films</title><p>The SEM images of ZnS<sub>x</sub>Se<sub>1−x</sub> thin films deposited using 1:1 ratio of [Zn(Se<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] and [Zn(S<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] precursor mixture showed irregular shaped crystallites which showed some kind of tetragonal morphologies (<xref ref-type="fig" rid="fig5">Figure 5</xref>). EDX result showed the ratio of Zn: S: Se: 47.34:36.68:13.98 giving a stoichiometric formula of Zn<sub>1.0</sub>Se<sub>0.77</sub>S<sub>0.30</sub>. The EDX results gave good explanation for the larger deviation of the p-XRD patterns peaks from the ZnS patterns than the ZnSe pattern. Morphology of the ZnS<sub>x</sub>Se<sub>1−x</sub> films deposited using 1:0.75 molar ratio of [Zn(Se<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] and [Zn(S<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] is based on a mixture of irregular and cubic crystallites.</p><p>EDX results showed the ratio of Zn: S: Se: 49.25:23.84:26.91 giving a stoichiometric formula of Zn<sub>1.0</sub>Se<sub>0.48</sub>S<sub>0.54</sub>. The elemental map of the films showed uniform distribution of elements on the entire area of the substrate (<xref ref-type="fig" rid="fig6">Figure 6</xref>).</p></sec><sec id="s3_3_3"><title>3.3.3. Raman Spectroscopic Studies of ZnSSe Thin Films</title><p>Raman spectra of ZnS<sub>x</sub>Se<sub>1−x</sub> thin films deposited using 1:1 ratio of [Zn(Se<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] and [Zn(S<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] precursor mixture showed strong peaks at 240 cm<sup>−1</sup> which shifted from the ZnSe peaks at (253 cm<sup>−1</sup>) and the peak at 300 cm<sup>−1</sup> corresponds to ZnS phases (306 cm<sup>−1</sup>). Similarly the peak at 490 cm<sup>−1</sup> corresponds to the Raman mode of ZnSe (498 cm<sup>−1</sup>). Other peak observed at 550 cm<sup>−1</sup> was closer to the peak for ZnS (546 cm<sup>−1</sup>) (<xref ref-type="fig" rid="fig3">Figure 3</xref>(a)) [<xref ref-type="bibr" rid="scirp.78959-ref31">31</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref32">32</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref33">33</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref34">34</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref35">35</xref>] [<xref ref-type="bibr" rid="scirp.78959-ref37">37</xref>] . The Raman spectra of the ZnS<sub>x</sub>Se<sub>1−x</sub> films deposited using 1:0.75 molar ratio of [Zn(Se<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] and [Zn(S<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] showed strong peaks at 240 cm<sup>−1</sup> which is shifted from the ZnSe peak at 252 cm<sup>−1</sup> along with peaks at 300 cm<sup>−1</sup> which correspond</p><p>to ZnS peak at 306 cm<sup>−1</sup> [<xref ref-type="bibr" rid="scirp.78959-ref47">47</xref>] . Other peaks are similar to those observed for the films obtained from 1:1 mixture.</p></sec><sec id="s3_3_4"><title>3.3.4. PL Spectra of ZnSSe Films</title><p>PL spectra of the ZnS<sub>x</sub>Se<sub>1−x</sub> films deposited using two different precursor mixture concentrations (1:1 and 1: 0.75 molar ratio of [Zn(Se<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] and [Zn(S<sub>2</sub>CNEt<sub>2</sub>)<sub>2</sub>] mixture) showed less intense emission than the ZnSe films. The Se rich ZnSSe films showed PL at about 485 nm which gave a band gap of about 2.55 eV. Whereas the one with 1:1 ratio of S:Se showed PL absorption about 465 nm which gave an average band gap of 2.66 eV. Both values found to be higher than the band gap for ZnSe (2.25 eV) (<xref ref-type="fig" rid="fig3">Figure 3</xref>(b)). PL absorption showed that the absorption shifted towards blue region because of the presence of S and PL absorption decreases with increase in S content in the ZnSSe films. PL spectra measured for these films showed blue shift compared to ZnSe films and showed band gap around 2.4 eV (referred as ZnSSe1). The values showed good agreement with the reported values of ZnS<sub>x</sub>Se<sub>1?x</sub> thin films with increase in value of S content [<xref ref-type="bibr" rid="scirp.78959-ref33">33</xref>] .</p></sec></sec></sec><sec id="s4"><title>4. Conclusion</title><p>The band gap of ZnSe had been tuned from 2.25 eV to 2.66 eV by increasing the sulfur content in the alloy (ZnS<sub>x</sub>Se<sub>1−x</sub>). XRD and Raman spectra showed the purity of ZnSe and confirmed the formation of ternary phase (ZnSSe). The morphology of the films was changed by addition of sulphur into the selenium precursor. The recent use of thin film absorber layers in solar energy conversion devices has led to the real possibility of sustainable and inexpensive replacements for silicon-based photovoltaics based on compound semiconductors. Our new manuscript shows how band gap tuning can be achieved from the doping of sulphur or selenium in metal chalcogenide thin films. Chemical vapour deposition (CVD) techniques to produce these films are currently highly sought-after as they have the potential for eventual scale up should these materials for solar cells be the solution to the renewable energy problem.</p></sec><sec id="s5"><title>Acknowledgements</title><p>YA is thankful to University of King Abdulaziz University for Funding.</p></sec><sec id="s6"><title>Cite this paper</title><p>Alghamdi, Y. (2017) Composition and Band Gap Controlled AACVD of ZnSe and ZnS<sub>x</sub>Se<sub>1−x</sub> Thin Films Using Novel Single Source Precursors. 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