<?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.2015.311005</article-id><article-id pub-id-type="publisher-id">MSCE-61325</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>
 
 
  Synthesis of ZnS, CdS and Core-Shell Mixed CdS/ZnS, ZnS/CdS Nanocrystals in Tapioca Starch Matrix
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>aren</surname><given-names>Khachatryan</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>Gohar</surname><given-names>Khachatryan</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>Maciej</surname><given-names>Fiedorowicz</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Chemistry and Physics, Agricultural University, Cracow, Poland</addr-line></aff><pub-date pub-type="epub"><day>13</day><month>11</month><year>2015</year></pub-date><volume>03</volume><issue>11</issue><fpage>30</fpage><lpage>38</lpage><history><date date-type="received"><day>22</day>	<month>September</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>14</month>	<year>November</year>	</date><date date-type="accepted"><day>20</day>	<month>November</month>	<year>2015</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>
 
 
  Gel of tapioca starch (TS) is a suitable matrix for the formation of ZnS, CdS and core-shell ZnS/CdS as well as CdS/ZnS quantum dots (QDs). These QDs reside in the matrix as non-agglomerating 3 - 10 nm nanocrystals. It is demonstrated that amylopectin is responsible for the QDs formation rather than amylose. Combination of ZnS with CdS in the core-shell QDs results in the increase in the intensity of emission without any shift of its wavelength.
 
</p></abstract><kwd-group><kwd>Bilayered Quantum Dots</kwd><kwd> Luminescent Biocomposites</kwd><kwd> Quantum Dots</kwd><kwd> Tapioca Starch</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Quantum dots (QDs) are colloidal semiconducting nanocrystals composed of an inorganic core surrounded by an organic outer layer of surfactant molecules (ligands) [<xref ref-type="bibr" rid="scirp.61325-ref1">1</xref>] . They develop emission when excited with a UV light. The wavelength of emission depends on the size of the nanoparticles [<xref ref-type="bibr" rid="scirp.61325-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.61325-ref3">3</xref>] . Their semiconducting properties originate from their excitons confined in all three spatial dimensions [<xref ref-type="bibr" rid="scirp.61325-ref4">4</xref>] . Especially, useful are the core-shell type nanoparticles composed of two kinds of semiconductors, e.g. CdS/ZnS [<xref ref-type="bibr" rid="scirp.61325-ref5">5</xref>] , CdSe/ZnS [<xref ref-type="bibr" rid="scirp.61325-ref6">6</xref>] and CdSe/CdS [<xref ref-type="bibr" rid="scirp.61325-ref7">7</xref>] . In each pair of the sulphides/selenides, the first of them plays a role of the core while the second one forms a shell extending the gap of the emission of the core QDs. Such paired nanoparticles are high-efficiency photoluminescent (PL) materials [<xref ref-type="bibr" rid="scirp.61325-ref8">8</xref>] . Such property extends a wide range of applications of QDs as transistors, components of solar cells, light-emitting devices and diode lasers; they can also be used as agents for medical imaging [<xref ref-type="bibr" rid="scirp.61325-ref9">9</xref>] -[<xref ref-type="bibr" rid="scirp.61325-ref12">12</xref>] , fluorescent labels [<xref ref-type="bibr" rid="scirp.61325-ref13">13</xref>] -[<xref ref-type="bibr" rid="scirp.61325-ref15">15</xref>] , fluorescent probes [<xref ref-type="bibr" rid="scirp.61325-ref16">16</xref>] -[<xref ref-type="bibr" rid="scirp.61325-ref20">20</xref>] , and immunosensors [<xref ref-type="bibr" rid="scirp.61325-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.61325-ref22">22</xref>] .</p><p>Concentration of diluted suspensions of nanoparticles of several materials results in agglomeration leading to loss of advantages resulting from their nanodimensions. Therefore, QDs are frequently synthesized in the presence of organic molecules which prevent them from agglomeration and form a coating for the QDs. Application of QDs in biological studies succeeded due to their conjugation with proteins [<xref ref-type="bibr" rid="scirp.61325-ref23">23</xref>] -[<xref ref-type="bibr" rid="scirp.61325-ref27">27</xref>] , peptides and amino acids [<xref ref-type="bibr" rid="scirp.61325-ref28">28</xref>] [<xref ref-type="bibr" rid="scirp.61325-ref29">29</xref>] . Also polysaccharides were applied for that purpose. The studies involved amino polysaccharides such as chitosan [<xref ref-type="bibr" rid="scirp.61325-ref30">30</xref>] -[<xref ref-type="bibr" rid="scirp.61325-ref35">35</xref>] , cellulose, starch and other polysaccharides [<xref ref-type="bibr" rid="scirp.61325-ref36">36</xref>] -[<xref ref-type="bibr" rid="scirp.61325-ref43">43</xref>] .</p><p>Polysaccharides offer some advantage as they provide drawing luminescent foils with embedded QDs. Properties of the foils depend on the polysaccharide applied. In case of starches, their pasting ability and rheological properties of resulting pastes are essential for the attributes of nanocrystals and the resulting foil composites. However, our former studies showed that the anionic/nonionic character of the polysaccharide matrix was also a factor. These observations prompted us to check how the generated QDs would behave in the tapioca starch matrix. Tapioca (cassava, manioq, yucca) starch (TS) is a common, non-ionic starch known for providing smooth uniform gels of much lower viscosity than many other natural starches [<xref ref-type="bibr" rid="scirp.61325-ref44">44</xref>] .</p><p>In this paper an original, simple and cheap in situ synthesis of ZnS, CdS, ZnS-CdS and CdS-ZnS core-shell QDs in aqueous TS gel is presented. Biocomposites were characterized by using photoluminescence (PL), FTIR and UV/VIS spectrometric techniques and Transmission Electron Microscopy (TEM). Thermal properties (DSC, TG) of biocomposites were also measured. In order to check the impact of the QDs formation on the structure of polysaccharide chains, the absolute molecular weights (M<sub>W</sub>) were measured for two dominating fractions of TS prior and after generation QDs. They were determined with a size exclusion chromatography with dual detection (SEC-MALLS-RI).</p></sec><sec id="s2"><title>2. Materials and Methods</title><sec id="s2_1"><title>2.1. Generation of QDs</title><p>Tapioca starch (TS)/ZnS, CdS nanocomposites were prepared from gelatinized TS and either zinc acetate (Aldrich, 99.99%) or cadmium acetate (Aldrich, 99.99%) and Na<sub>2</sub>S (Aldrich, Na<sub>2</sub>S∙9H<sub>2</sub>O ≥99.99%). TS (1 g in 30 mL of deionized water) was heated with continuous stirring until it was completely gelatinized (70˚C for 30 min), treated with 0.35 mmol given salt solution (zinc or cadmium acetate), then a stoichiometric amount of 0.1 M aq. Na<sub>2</sub>S∙9H<sub>2</sub>O solution was added. To obtain nanocomposites with equal amounts of QDs, ZnS and CdS nanocrystals were prepared the same way as above but using half of substrates (0.175 mmol acetate solution and stoichiometric amount of 0.1 M aq. Na<sub>2</sub>S∙9H<sub>2</sub>O solution). Core-shell ZnS/CdS and CdS/ZnS nanocrystals were generated by adding 0.175 mmol acetate of a proper metal (Cd or Zn) to either ZnS or CdS QDs followed by addition of a stoichiometric amount of 0.1 M aq. Na<sub>2</sub>S∙9H<sub>2</sub>O solution.</p><p>All resulting suspensions were brought to room temperature then centrifuged. The deposits were applied to clean, smooth either Teflon or glass surfaces, and left for evaporation in the air. The dry foils were collected and stored in closed vessels.</p></sec><sec id="s2_2"><title>2.2. Transmission Electron Microscopy (TEM)</title><p>Analyses of sizes and morphologies of the as-prepared nanoparticles were studied using a high resolution JEOL 7550 scanning electron microscope equipped with Energy dispersion X-ray spectroscopy (EDS) analyzer for local chemical analysis. Samples for TEM and SEM microscopies were prepared after drop-coating 10 &#181;L of the sample on a carbon-coated copper grid (PELCO<sup>&#174;</sup>). Because the material was sufficiently conducting, the gold sputtering of the samples was dispensable.</p></sec><sec id="s2_3"><title>2.3. Size Exclusion Chromatography</title><p>Molecular weight, M<sub>w</sub>, and radii of gyration, R<sub>G</sub>, of the polysaccharide chains from the nanocomposites samples were estimated with the system consisting of a pump (Shimadzu 10AC, Tokyo, Japan), an injection valve (model 7021, Rheodyne, Palo Alto, CA, USA), two connected size exclusion columns TSKgel GMPWXL (300 &#215; 7.8 mm, Tosoh Corporation, Tokyo, Japan) and TSKgel 2500 PWXL (300 &#215; 7.8 mm, Tosoh Corporation, Tokyo, Japan), a multiangle laser light scattering detector (MALLS) (Dawn-DSP-F, Wyatt Technology, Santa Barbara, CA, USA) and a differential refractive index detector (L-7490, Merck, Darmstadt, Germany).</p></sec><sec id="s2_4"><title>2.4. UV-VIS Spectroscopy</title><p>The UV-VIS absorption spectra were recorded with a Shimadzu 2101 scanning spectrophotometer in the range of 200 - 800 nm using 10 mL, 10 cm thick quartz cells. Concentration of the solutions was 0.003 g/L.</p></sec><sec id="s2_5"><title>2.5. Photoluminescent Spectroscopy</title><p>Photoluminescence (PL) measurements for films were performed at room temperature using F7000 HITACHI spectrophotometer. The 360 nm wavelength was used for the excitation.</p></sec><sec id="s2_6"><title>2.6. Thermogravimetry (TG)</title><p>Thermogravimetric analysis coupled with mass spectrometry analyses (MS-TG/DTG/SDTA) was performed with a Mettler-Toledo 851e apparatus in 150 μl corundum crucibles, closed by a lid with a hole. The experiments were run in the air (80 mL/min) within the temperature range of and 30˚C - 700˚C (the heating rate was 10˚C/min).</p></sec><sec id="s2_7"><title>2.7. FTIR Spectroscopy</title><p>The FTIR-ATR spectra of the film were recorded in the range of 4000 - 700 cm<sup>−1</sup> at resolution of 4 cm<sup>−1</sup> using a Mattson 3000 FT-IR (Madison, Wisconsin, USA) spectrophotometer. That instrument was equipped with a 30SPEC 30˚ reflectance adapter fitted with the MIRacle ATR accessory from PIKE Technologies Inc., Madison, Wisconsin, USA.</p></sec><sec id="s2_8"><title>2.8. Differential Scanning Calorimetry (DSC)</title><p>The differential scanning calorimetry (DSC) was performed in a Mettler-Toledo 821e calorimeter equipped with anHaakeintracooler in 40 μL aluminum crucibles at a constant flow of argon (80 mL/min) within temperature range of 25˚C - 500˚C.</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><p>The TEM microscopy showed metal sulfides under study embedded in the TS matrix as 3 - 10 nm nanocrystals with a low tendency for agglomeration (<xref ref-type="fig" rid="fig1">Figure 1</xref>). This result confirmed our observation that nonanionic polysaccharides were superior matrices for generation of nanocrystals of metallic [<xref ref-type="bibr" rid="scirp.61325-ref45">45</xref>] and QDs [<xref ref-type="bibr" rid="scirp.61325-ref42">42</xref>] [<xref ref-type="bibr" rid="scirp.61325-ref43">43</xref>] particles.</p><p>The matrices made of anionic starches favored formation of much larger and agglomerating nanocrystals (Khachatryan, K., Khachatryan, G., Fiedorowicz, M., Distarch phosphate as a matrix for generation of quantum dots, Iran. J. Chem. Chem. Eng., submitted, 2015).</p><p>TS was separated with size exclusion chromatography into fractions among which two fractions dominated. They were higher molecular fraction of M<sub>w</sub> = 1.18 &#215; 10<sup>6</sup> g/mol and lower molecular fraction of M<sub>w</sub> = 1.27 &#215; 10<sup>5</sup> g/mol. The amount ratio of the collected fractions was high: low = 1.82. After generation of ZnS and ZnS/CdS QDs also two dominating fractions could be distinguished in the eluates but in the proportions of high: low = 0.43 and 0.47, respectively. Size exclusion chromatography of TS after generation CdS and CdS/ZnS QDs provided in the first case two fractions in that proportion of 0.69 and in the second case only low molecular fraction could be collected from the column. M<sub>w</sub> of all collected fractions insignificantly differed from the corresponding values for original gelatinized TS.</p><p>Thus, one could deduce that the generation of QDs within the high molecular weight fraction of the gel was favored. That observation fitted results of the study by Ciesielski and Tomasik [<xref ref-type="bibr" rid="scirp.61325-ref45">45</xref>] that amylopectin formed Werner complexes with metal ions whereas amylose was passive as a ligand.</p><p>The UV-VIS spectrum of TS (<xref ref-type="fig" rid="fig2">Figure 2</xref>) demonstrated a low absorption shoulder around 250 nm belonging likely to n → π<sup>*</sup> transitions in the lone electron pairs at the oxygen atoms. All preparations of TS with embedded QDs showed a strong absorption band around 220 nm followed by the long wavelength tail reaching its bottom in the spectrum of TS/ZnS already around 330 nm and between 450 - 500 nm in the spectra of the preparations containing CdS (<xref ref-type="fig" rid="fig2">Figure 2</xref>).</p><p>The emission spectra of the preparations (<xref ref-type="fig" rid="fig3">Figure 3</xref>) showed an emission maximum from TS/ZnS and TS/CdS around 440 and 540 nm, respectively. Supplementation of ZnS within TS with CdS QDs appeared very successful</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Taken at 100 000 (ZnS) and 200,000 (CdS, ZnS/CdS and CdS/ZnS) magnification TEM micrographs of QDs embedded in the TS matrix</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-1740243x6.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> UV-VIS spectra of TS and QDs embedded in the TS matrix</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-1740243x7.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> PL spectra of TS and QDs embedded in the TS matrix</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-1740243x8.png"/></fig><p>in a significant raising the intensity of the emission maximum, however, without a shift of the wavelength of the emission. The increase in the intensity of the emission band could be observed when in the TS/CdS preparation ZnS was additionally generated. The shoulder of an intensive emission could be observed around 440 nm (<xref ref-type="fig" rid="fig3">Figure 3</xref>). These effects showed that blending QDs of two different origins was a very successful approach in increasing the intensity of emission. The emission patterns implied that the original QDs were the nuclei for the formation of the subsequent QDs, thus the binary QDs could be bilayered species.</p><p>Thermograms of TS (<xref ref-type="fig" rid="fig4">Figure 4</xref>) showed that the polysaccharide lost ~10% of its weight around 100˚C. That loss resulted from departure of the absorbed moisture. That effect was followed by a rapid loss of further ~16% weight at approximately 250˚C. It could be associated with a departure of water molecules on formation of 3,6-anhydro derivatives of TS. Subsequently, TS lost further ~45% weight to 320˚C and another ~25% up to 450˚C. Above 450˚ there was no further decomposition and the weight stabilized on the level of 5% residual carbonizate.</p><p>The decomposition pattern of the TS/QDs preparations was initially similar. The preparations lost some moisture then began to decompose at the same temperature as plain TS. Further decomposition pattern was different. The preparations lost their weight less rapidly and only TS/CdS decomposed up to 320˚C in two well distinguished steps. Some slight increase in the weight after initial decomposition could result from a reaction of CdS with atmospheric oxygen as such effect was absent when thermogravimetry was run under argon. Further decomposition pattern for all other preparations was the same. Temperatures of the corresponding decomposition steps were the same and only the weight of the residues was different. The latter were approximately 15%, 12%, 8% and 8% for TS with embedded ZnS, CdS, ZnS-CdS and CdS-ZnS, respectively.</p><p>Such course of decomposition might suggest that the introduction of QDs into the TS gel could influence the internal structure of the gel but they did not form complexes with the polysaccharide. The latter assumption was backed by analysis of FTIR spectra of particular preparations and differential scanning calorimetry (DSC). All FTIR spectra were identical (<xref ref-type="fig" rid="fig5">Figure 5</xref>).</p><p>The DSC diagrams of TS and TS/QDS preparations differed solely in the low temperature region where endothermic effects associated with physical water-polysaccharide relations appeared. Further parts of the diagrams showed a close resemblance (<xref ref-type="fig" rid="fig6">Figure 6</xref>). There were slightly exothermic effects around 250˚C common for all samples. The major exothermic effect of comparable magnitude occurred around 320˚C.</p></sec><sec id="s4"><title>4. Conclusions</title><p>1) Tapioca starch is suitable as the matrix for QDs as it limits the growth of QDs particles and prevents them</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Thermograms of TS and TS/QDs preparations taken in the air</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-1740243x9.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> FTIR-ATR spectra of TS and TS/QDs foils</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-1740243x10.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> DSC diagrams of TS and its preparations containing QDs</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-1740243x11.png"/></fig><p>from agglomeration.</p><p>2) The core-shell technique of the generation of binary QDs provides a significant increase in the emission intensity without any shift of the emission wavelength. The recorded emission comes from the shell forming component.</p></sec><sec id="s5"><title>Cite this paper</title><p>KarenKhachatryan,GoharKhachatryan,MaciejFiedorowicz, (2015) Synthesis of ZnS, CdS and Core-Shell Mixed CdS/ZnS, ZnS/CdS Nanocrystals in Tapioca Starch Matrix. Journal of Materials Science and Chemical Engineering,03,30-38. doi: 10.4236/msce.2015.311005</p></sec></body><back><ref-list><title>References</title><ref id="scirp.61325-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Reiss, P., Proti&amp;egrave;re, M. and Li, L. (2009) Core/Shell Semiconductor Nanocrystals. Small, 5, 154-168. 
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